National Library of Energy BETA

Sample records for bin csh fb

  1. PHONE FAX WEB +41-31-631-8534 +41-31-631-4405 www.csh.unibe.ch

    E-Print Network [OSTI]

    Sola, Rolf Haenni

    Wissenschaften (ExWi), Sidlerstrasse 5, 3012, Bern Joint CSH-WP: Mittwoch, 14.15-15.15 Uhr, Hörraum B5, ExWi, Sidlerstrasse 5, 3012, Bern The CSH Informal Lunch takes

  2. Analysis of C-S-H gel and cement paste by small-angle neutron scattering

    SciTech Connect (OSTI)

    Allen, Andrew J. [Materials Science and Engineering Laboratory, NIST, Gaithersburg, MD 20899 (United States)]. E-mail: andrew.allen@nist.gov; Thomas, Jeffrey J. [Department of Civil and Environmental Engineering, Northwestern University, Evanston, IL 60208 (United States)]. E-mail: jthomas@northwestern.edu

    2007-03-15

    The role of small-angle X-ray and neutron scattering (SAXS and SANS) in the characterization of cement is briefly reviewed. The unique information obtainable from SANS analysis of C-S-H gel in hydrating cement is compared with that obtainable by other neutron methods. Implications for the nature of C-S-H gel, as detected by SANS, are considered in relation to current models. Finally, the application of the SANS method to cement paste is demonstrated by analyzing the effects of calcium chloride acceleration and sucrose retardation on the resulting hydrated microstructure.

  3. Graduate Catalogue 201415 The Prince Alwaleed Bin Talal Bin Abdulaziz Alsaud Center

    E-Print Network [OSTI]

    195 Graduate Catalogue 2014­15 The Prince Alwaleed Bin Talal Bin Abdulaziz Alsaud Center for American Studies and Research (CASAR) The Prince Alwaleed Bin Talal Bin Abdulaziz Alsaud Center to include in their program of study additional Arabic credits. #12;196 Graduate Catalogue 2014­15 The Prince

  4. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul criteria, will be stated at the beginning of lecture #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2 · Muscle Physiology · Heart and circulatory functions · Neuroethology #12;FB2 Biologie / Chemie www

  5. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014%) written exam (60%) journal (20%) Preparation of course work (20%) #12;FB2 Biologie / Chemie www · Antioxidants #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014

  6. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Klausur (50%) Protokolle Grundkurs (50%) written exam (50%) journal (50%) #12;FB2 Biologie / Chemie www

  7. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Modulprüfung (MP) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie

  8. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie www

  9. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014-up to the tutorial protocol corrections communication with lecturers and students #12;FB2 Biologie / Chemie www

  10. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 protocols. #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 of the lecture #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014

  11. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 of lecture #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 functions · Learning, memory, sleep #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO

  12. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Lerntagebuches Journal #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd the different taxa #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd

  13. Time-bin entangled photon holes

    E-Print Network [OSTI]

    J. Liang; J. D. Franson; T. B. Pittman

    2012-08-23

    The general concept of entangled photon holes is based on a correlated absence of photon pairs in an otherwise constant optical background. Here we consider the specialized case when this background is confined to two well-defined time bins, which allows the formation of time-bin entangled photon holes. We show that when the typical coherent state background is replaced by a true single-photon (Fock state) background, the basic time-bin entangled photon-hole state becomes equivalent to one of the time-bin entangled photon-pair states. We experimentally demonstrate these ideas using a parametric down-conversion photon-pair source, linear optics, and post-selection to violate a Bell inequality with time-bin entangled photon holes.

  14. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 presentation #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014

  15. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2 Rechenmethoden in den Naturwissenschaften für Studierende der Chemie und Biologie B Calculus for the Natural

  16. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014%) presentation (30%) oral exam (70%) #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO

  17. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul

  18. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Mentorenprogramm statt. The oral exam is part of the mentoring. #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2

  19. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 (20%) report (80%) Presentation (20%) #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni

  20. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Modulprüfung (MP) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie of brains are included. Diseases and etiologies are also presented. #12;FB2 Biologie / Chemie www

  1. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 written exam #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd

  2. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014%) presentation (20%) #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd

  3. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014%) Protokolle (70%) presentation (30%) journal (70%) #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni

  4. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Biology" . #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014

  5. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 percent) and computational tasks (80 percent). #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni

  6. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Abschluss der Module Chemie 1, Bio 2. MBW 1. Studienvarianten /The module / submodule is part exam exclusively based on lecture #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO

  7. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Chemie 1, Bio 2 Studienvarianten /The module / submodule is part of the following study types Vollfach) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO

  8. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Biochemistry". #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014

  9. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 and to evalute the own level of knowledge through feedbacks. #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2

  10. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014: Erfolgreicher Abschluss der Module Chemie 1, Bio 2. MBW 1. Studienvarianten /The module / submodule is part work (not graded) #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011

  11. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014: Erfolgreicher Abschluss der Module Chemie 1, Bio 2. MBW 1. Studienvarianten /The module / submodule is part (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni

  12. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Modulprüfung (MP) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie, interference) #12;FB2 Biologie / Chemie www.

  13. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014, Kleingruppenpräsentation presentation script and presentation #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni

  14. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 (30%) report (70%) presentation (30%) #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni

  15. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014: Marine invertrebrates alternating with Marine Algae. #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2

  16. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014: Erfolgreicher Abschluss der Module Chemie 1, Bio 2. MBW 1. Studienvarianten /The module / submodule is part knowledge of genetics is relevant. #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO

  17. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO

  18. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 hours #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014

  19. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 geregelt (§ 7). #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd

  20. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Modulprüfung (MP) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie Kernphysik - Aufbau der Materie (Kernteilchen) - Radioaktivität content #12;FB2 Biologie / Chemie www

  1. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul written exam #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd

  2. Thermodynamic Systems for Tier 2 Bin 2 Diesel Engines | Department...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Systems for Tier 2 Bin 2 Diesel Engines Thermodynamic Systems for Tier 2 Bin 2 Diesel Engines Discusses engine technology enablers that help achieve overall system integration...

  3. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul / module their function. #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014

  4. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul / module code Bio 6 of vertebrates #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014

  5. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 of the exam is 50% of each submodule #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul / module

  6. Bin Set 1 Calcine Retrieval Feasibility Study

    SciTech Connect (OSTI)

    R. D. Adams; S. M. Berry; K. J. Galloway; T. A. Langenwalter; D. A. Lopez; C. M. Noakes; H. K. Peterson; M. I. Pope; R. J. Turk

    1999-10-01

    At the Department of Energy's Idaho Nuclear Technology and Engineering Center, as an interim waste management measure, both mixed high-level liquid waste and sodium bearing waste have been solidified by a calculation process and are stored in the Calcine Solids Storage Facilities. This calcined product will eventually be treated to allow final disposal in a national geologic repository. The Calcine Solids Storage Facilities comprise seven ''bit sets.'' Bin Set 1, the first to be constructed, was completed in 1959, and has been in service since 1963. It is the only bin set that does not meet current safe-shutdown earthquake seismic criteria. In addition, it is the only bin set that lacks built-in features to aid in calcine retrieval. One option to alleviate the seismic compliance issue is to transport the calcine from Bin Set 1 to another bin set which has the required capacity and which is seismically qualified. This report studies the feasibility of retrieving the calcine from Bi n Set 1 and transporting it into Bin Set 6 which is located approximately 650 feet away. Because Bin Set 1 was not designed for calcine retrieval, and because of the high radiation levels and potential contamination spread from the calcined material, this is a challenging engineering task. This report presents preconceptual design studies for remotely-operated, low-density, pneumatic vacuum retrieval and transport systems and equipment that are based on past work performed by the Raytheon Engineers and Constructors architectural engineering firm. The designs presented are considered feasible; however, future development work will be needed in several areas during the subsequent conceptual design phase.

  7. Joint-Frequency Bins versus Conventional Bin Weather Data in Analysis of HVAC System Operation 

    E-Print Network [OSTI]

    Jones, A.; Baltazar, J. C.; Claridge, D. E.

    2009-01-01

    Often in simplified energy analysis the use of bin weather data is employed for a more time efficient and better organized analysis than using the full 8760-hour annual weather data. It has been suggested that joint-frequency bins be used instead...

  8. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Art der Prüfung / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul / module code Bio 4

  9. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul / module

  10. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014: Erfolgreicher Abschluss der Module Chemie 1, Bio 2. MBW 1. Studienvarianten /The module / submodule is part Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Art der Prüfung

  11. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie www

  12. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 Abschluss der Module Chemie 1, Bio 2. MBW 1. Studienvarianten /The module / submodule is part Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Art der Prüfung

  13. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 20142 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul

  14. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014: Erfolgreicher Abschluss der Module Chemie 1, Bio 2. MBW 1. Studienvarianten /The module / submodule is part Modulprüfung (MP) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie

  15. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul / module code FD 1 6

  16. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014, Chemisches Grundpraktikum/ P Allgemeine Chemie für den Teil Biochemie-Praktikum Unterrichtssprache / language) or submodule (TP) entspricht Studienleistung (unbenotet) course work (not graded) #12;FB2 Biologie / Chemie www

  17. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul / module code Gentec

  18. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 learning outcome Domain I

  19. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modul / module code PM 1

  20. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014 insbesondere der Biologie und in Teilen der naturwissenschaftlicher Fächer Physik und Chemie an Beispielen- und situationsgerechten Einsatz nennen und erläutern (2.1 + 2.2) #12;FB2 Biologie / Chemie www

  1. 1 Compost Bin Designs 1. Why Compost?

    E-Print Network [OSTI]

    Kaye, Jason P.

    1 Compost Bin Designs 1. Why Compost? Composting livestock manure is an excellent manure management but you are also being environmentally friendly. Composting not only provides the owner with a free source of compost for the yard, garden, and pastures that will benefit plants by slowly releasing nutrients

  2. Challenges of Meeting Tier2 Bin2 Tailpipe Emissions | Department...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    of Meeting Tier2 Bin2 Tailpipe Emissions Challenges of Meeting Tier2 Bin2 Tailpipe Emissions Presentation given at the 2007 Diesel Engine-Efficiency & Emissions Research Conference...

  3. $A^t_{FB}$ Meets LHC

    SciTech Connect (OSTI)

    Hewett, JoAnne L.; /SLAC; Shelton, Jessie; /Yale U.; Spannowsky, Michael; /Oregon U.; Tait, Tim M.P.; /UC, Irvine; Takeuchi, Michihisa; /Heidelberg U.

    2012-02-14

    The recent Tevatron measurement of the forward-backward asymmetry of the top quark shows an intriguing discrepancy with Standard Model expectations, particularly at large t{bar t} invariant masses. Measurements of this quantity are subtle at the LHC, due to its pp initial state, however, one can define a forward-central-charge asymmetry which captures the physics. We study the capability of the LHC to measure this asymmetry and find that within the SM a measurement at the 5{sigma} level is possible with roughly 60 fb{sup -1} at {radical}s = 14 TeV. If nature realizes a model which enhances the asymmetry (as is necessary to explain the Tevatron measurements), a significant difference from zero can be observed much earlier, perhaps even during early LHC running at {radical}s = 7 TeV. We further explore the capabilities of the 7 TeV LHC to discover resonances or contact interactions which modify the t{bar t} invariant mass distribution using recent boosted top tagging techniques. We find that TeV-scale color octet resonances can be discovered, even with small coupling strengths and that contact interactions can be probed at scales exceeding 6 TeV. Overall, the LHC has good potential to clarify the situation with regards to the Tevatron forward-backward measurement.

  4. Formation of Hydroxyl Groups at Calcium-Silicate-Hydrate (C-S-H): Coexistence of Ca-OH and Si-OH on Wollastonite(001)

    E-Print Network [OSTI]

    Schmidt, Wolf Gero

    Formation of Hydroxyl Groups at Calcium-Silicate-Hydrate (C-S-H): Coexistence of Ca-OH and Si by hydroxyl groups is of particular interest for various further surface reactions. The activation energy of these hydroxyl groups required in chemical reactions largely determines the surface chemistry. In the present

  5. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modulbeschreibung / Module Description Modul / module code Che 2 6 ECTS-Punkte / credit points Chemie-Praktika Lab, Chemisches Grundpraktikum/ P Allgemeine Chemie für den Teil Biochemie-Praktikum Unterrichtssprache / language

  6. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni-bremen.de BPO Biologie 2011 / MEd 2014/15 Modulbeschreibung / Module Description Modul / module code Che 1 9 ECTS-Punkte / credit points Allgemeine Chemie Moduls ist, allen Studierenden der Biologie und Geologie Einblick in wesentliche Grundlagen der Chemie

  7. Growth of sheets in 3D confinements - a model for the C-S-H meso 2 structure

    E-Print Network [OSTI]

    Etzold, Merlin A.; McDonald, Peter J.; Routh, Alexander F.

    2014-06-21

    C-S-H [1]. However,158 we note that the sheet orientation in fibrillar micrographs appears orthogonal to that in the simulation.159 The closing of larger pores as seen in the sequence Figure 3a-b can mechanistically explain the densi-160 fication... .20 2.0 0 02 5 6 8 P0 rog resVaVNeoml i eet al. di al TmVGl Tewt Vhl eRWwWDml di al TmVGl Tewt Vhl eWi RWwWDml rhVaal TWi f ehI TRl en h p022ei ewt Al Tl Figure 6: Example scattering curves obtained for structure (h) in Figure 3 together with small...

  8. hescore_2012_bins | Department of Energy

    Broader source: Energy.gov (indexed) [DOE]

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-Sessions |discussed howCommercial LocalwasERI-2142.18-1501hescore_2012_bins.xlsx

  9. Photography, Tragedy and Osama Bin Laden: Looking at the enemy

    E-Print Network [OSTI]

    Wallace, Jennifer

    2015-01-01

    to her mouth, to cover her horror, her anxiety, or her cough?i The central subject of the event – Osama Bin Laden himself – is missing from the photograph; the television is turned away from the image’s spectator. The occlusion of Bin Laden continued...

  10. Joint Inference of Multiple Label Types in Large Networks Deepayan Chakrabarti DEEPAY@FB.COM

    E-Print Network [OSTI]

    @FB.COM Stanislav Funiak SFUNIAK@FB.COM Jonathan Chang JONCHANG@FB.COM Sofus A. Macskassy SOFMAC@FB.COM Facebook Inc-passing architecture. On a billion-node subset of the Facebook social network, EDGEEXPLAIN signif- icantly outperforms the group from u's actual current city C, causing label propagation to infer C for u. However, our proposed

  11. nh gi Tn hi Ti nguyn Thin nhin do Trn du Deep Horizon Khi phc loi chim ng bin ti vng b bin Alabama

    E-Print Network [OSTI]

    ánh giá Tn hi Tài nguyên Thiên nhiên do Tràn du Deep Horizon Khôi phc loài chim ng bin ti vùng b Alabama s hình thành 5 nn làm t ca chim ng dc theo vùng b bin Mobile và Baldwin, Alabama tng c hi làm có th c tìm thy quanh nm ti khu vc b bin Alabama. Chim ng bin òi hi nhng khu vc làm t rng rãi vi

  12. nh gi Tn tht Ti nguyn Thin nhin Trn du Deepwater Horizon D n phc hi C bin ti B Bin Quc Gia

    E-Print Network [OSTI]

    Horizon. Sau s c tràn du Deepwater Horizon, mt lng áng k du t n bãi bin dc theo Florida Panhandle. Trong vi C rùa( Thallasiumtestudium ) , loài ph bin nht ti thm c bin GUIS 3 ) t các im quan trc o lng và

  13. Closing the Wedge with 300 fb^-1 and 3000 fb^-1 at the LHC: A Snowmass White Paper

    E-Print Network [OSTI]

    Ian M. Lewis

    2013-08-08

    The discovery of a Higgs boson at the LHC begins the era of directly measuring the mechanism of electroweak symmetry breaking (EWSB). Searching for extensions of the Standard Model (SM) EWSB sector at the LHC is of vital importance. An important extension of the SM with an extended EWSB sector is the Minimal Supersymmetric Standard Model (MSSM). In this white paper, we extend current ATLAS and CMS bounds on direct searches for the heavy MSSM neutral Higgs bosons to 300 fb^-1 and 3000 fb^-1 of data at the LHC. In particular we focus on the \\tau^+\\tau^- channel and the pseudoscalar decay to light Higgs boson and Z, with additional discussion on how to further close the wedge.

  14. Internet Tomography Mark Coates Alfred Hero Robert Nowak Bin Yu

    E-Print Network [OSTI]

    Yu, Bin

    Internet Tomography Mark Coates Alfred Hero Robert Nowak Bin Yu January, 2002 ABSTRACT Today's Internet is a massive, distributed network which continues to explode in size as e- commerce and related activities grow. The heterogeneous and largely unregulated structure of the Internet renders tasks

  15. Bin packing with general cost structures Leah Epstein

    E-Print Network [OSTI]

    Epstein, Leah

    of Industrial Engineering and Management, The Technion, Haifa, Israel. levinas@ie.technion.ac.il. 1 #12;Anily a larger load than a processor that executes a smaller number of long tasks, even if the total duration are not related to this paper. A related model was studied by Li and Chen [25]. In this model the cost of a bin

  16. Compressed supersymmetry after 1 fb?¹ at the Large Hadron Collider

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    LeCompte, Thomas J.; Martin, Stephen P.

    2012-02-01

    We study the reach of the Large Hadron Collider with 1 fb?¹ of data at ?s=7 TeV for several classes of supersymmetric models with compressed mass spectra, using jets and missing transverse energy cuts like those employed by ATLAS for summer 2011 data. In the limit of extreme compression, the best limits come from signal regions that do not require more than 2 or 3 jets and that remove backgrounds by requiring more missing energy rather than a higher effective mass.

  17. Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel engine...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel engine Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel engine Discusses plan, baselining, and modeling, for new...

  18. Cummins' Next Generation Tier 2, Bin 2 Light Truck Diesel Engine...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Cummins' Next Generation Tier 2, Bin 2 Light Truck Diesel Engine Cummins' Next Generation Tier 2, Bin 2 Light Truck Diesel Engine Development of a new light truck, in-line...

  19. Measurement of the ? ? * distribution of muon pairs with masses between 30 and 500 GeV in 10.4 fb - 1 of p p ¯ collisions

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V.?M.; Abbott, B.; Acharya, B.?S.; Adams, M.; Adams, T.; Agnew, J.?P.; Alexeev, G.?D.; Alkhazov, G.; Alton, A.; Askew, A.; et al

    2015-04-06

    We present a measurement of the distribution of the variable ?*? for muon pairs with masses between 30 and 500 GeV, using the complete run II data set collected by the D0 detector at the Fermilab Tevatron proton-antiproton collider. This corresponds to an integrated luminosity of 10.4 fb?¹ at ?s=1.96 TeV. The data are corrected for detector effects and presented in bins of dimuon rapidity and mass. The variable ?*? probes the same physical effects as the Z/?* boson transverse momentum, but is less susceptible to the effects of experimental resolution and efficiency. These are the first measurements at anymore »collider of the ?*? distributions for dilepton masses away from the Z?l?l? boson mass peak. The data are compared to QCD predictions based on the resummation of multiple soft gluons.« less

  20. Measurement of the ? ? * distribution of muon pairs with masses between 30 and 500 GeV in 10.4 fb - 1 of p p ¯ collisions

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V.?M.; Abbott, B.; Acharya, B.?S.; Adams, M.; Adams, T.; Agnew, J.?P.; Alexeev, G.?D.; Alkhazov, G.; Alton, A.; Askew, A.; Atkins, S.; Augsten, K.; Avila, C.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D.?V.; Banerjee, S.; Barberis, E.; Baringer, P.; Bartlett, J.?F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Bellantoni, L.; Beri, S.?B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P.?C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E.?E.; Borissov, G.; Borysova, M.; Brandt, A.; Brandt, O.; Brock, R.; Bross, A.; Brown, D.; Bu, X.?B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Buszello, C.?P.; Camacho-Pérez, E.; Casey, B.?C.?K.; Castilla-Valdez, H.; Caughron, S.; Chakrabarti, S.; Chan, K.?M.; Chandra, A.; Chapon, E.; Chen, G.; Cho, S.?W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W.?E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Cutts, D.; Das, A.; Davies, G.; de Jong, S.?J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Denisov, D.; Denisov, S.?P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H.?T.; Diesburg, M.; Ding, P.?F.; Dominguez, A.; Dubey, A.; Dudko, L.?V.; Duperrin, A.; Dutt, S.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V.?D.; Enari, Y.; Evans, H.; Evdokimov, V.?N.; Fauré, A.; Feng, L.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H.?E.; Fortner, M.; Fox, H.; Fuess, S.; Garbincius, P.?H.; Garcia-Bellido, A.; García-González, J.?A.; Gavrilov, V.; Geng, W.; Gerber, C.?E.; Gershtein, Y.; Ginther, G.; Gogota, O.; Golovanov, G.; Grannis, P.?D.; Greder, S.; Greenlee, H.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M.?W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J.?M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A.?P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M.?D.; Hirosky, R.; Hoang, T.; Hobbs, J.?D.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Holzbauer, J.?L.; Howley, I.; Hubacek, Z.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A.?S.; Jabeen, S.; Jaffré, M.; Jayasinghe, A.; Jeong, M.?S.; Jesik, R.; Jiang, P.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A.?W.; Juste, A.; Kajfasz, E.; Karmanov, D.; Katsanos, I.; Kaur, M.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y.?N.; Kiselevich, I.; Kohli, J.?M.; Kozelov, A.?V.; Kraus, J.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V.?A.; Lammers, S.; Lebrun, P.; Lee, H.?S.; Lee, S.?W.; Lee, W.?M.; Lei, X.; Lellouch, J.; Li, D.; Li, H.; Li, L.; Li, Q.?Z.; Li, X.; Lim, J.?K.; Lincoln, D.; Linnemann, J.; Lipaev, V.?V.; Lipton, R.; Liu, H.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Luna-Garcia, R.; Lyon, A.?L.; Maciel, A.?K.?A.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V.?L.; Mansour, J.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C.?L.; Meijer, M.?M.; Melnitchouk, A.; Menezes, D.; Mercadante, P.?G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N.?K.; Mulhearn, M.; Nagy, E.; Narain, M.; Nayyar, R.; Neal, H.?A.; Negret, J.?P.; Neustroev, P.; Nguyen, H.?T.; Nunnemann, T.; Orduna, J.; Osman, N.; Osta, J.; Pal, A.; Parashar, N.; Parihar, V.; Park, S.?K.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Pleier, M.-A.; Podstavkov, V.?M.; Popov, A.?V.; Prewitt, M.; Price, D.; Prokopenko, N.; Qian, J.; Qin, Y.; Quadt, A.; Quinn, B.; Ratoff, P.?N.; Razumov, I.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Sajot, G.; Sánchez-Hernández, A.; Sanders, M.?P.; Santos, A.?S.; Savage, G.; Savitskyi, M.; Sawyer, L.; Scanlon, T.; Schamberger, R.?D.; Scheglov, Y.; Schellman, H.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shaw, S.; Shchukin, A.?A.; Simak, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Snow, G.?R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Sonnenschein, L.; Soustruznik, K.; Stark, J.; Stoyanova, D.?A.; Strauss, M.; Suter, L.; Svoisky, P.; Titov, M.; Tokmenin, V.?V.; Tsai, Y.-T.; Tsybychev, D.; Tuchming, B.; Tully, C.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; van Leeuwen, W.?M.; Varelas, N.; Varnes, E.?W.; Vasilyev, I.?A.; Verkheev, A.?Y.; Vertogradov, L.?S.; Verzocchi, M.; Vesterinen, M.; Vilanova, D.; Vokac, P.; Wahl, H.?D.; Wang, M.?H.?L.?S.; Warchol, J.; Watts, G.

    2015-04-01

    We present a measurement of the distribution of the variable ?*? for muon pairs with masses between 30 and 500 GeV, using the complete run II data set collected by the D0 detector at the Fermilab Tevatron proton-antiproton collider. This corresponds to an integrated luminosity of 10.4 fb?¹ at ?s=1.96 TeV. The data are corrected for detector effects and presented in bins of dimuon rapidity and mass. The variable ?*? probes the same physical effects as the Z/?* boson transverse momentum, but is less susceptible to the effects of experimental resolution and efficiency. These are the first measurements at any collider of the ?*? distributions for dilepton masses away from the Z?l?l? boson mass peak. The data are compared to QCD predictions based on the resummation of multiple soft gluons.

  1. Simulated Annealing Based Algorithm for the 2D Bin Packing Problem with Impurities

    E-Print Network [OSTI]

    Kochetov, Yuri

    Simulated Annealing Based Algorithm for the 2D Bin Packing Problem with Impurities B. Beisiegel1 real-world problem originating in the steel industry. The bins are inhomogeneous sheets with impurities;Simulated Annealing Based Algorithm for the 2D Bin Packing Problem with Impurities 3 The oriented tree

  2. 13 Chng 13: D n xut Khi phc Sm Ra bin 13 Chng 13: D n xut Khi phc Sm Ra bin ......................................................................1

    E-Print Network [OSTI]

    .........................................................................................33 13.2.6 Tng cng Mng li Mc cn và Cu h Rùa bin và Phát trin Chng trình ng phó Khn cp Rùa bin.............................................................................................................54 13.2.7 Môi trng b nh hng và các hu qu môi trng do Tng cng Mng li Mc cn và Cu h Rùa bin và Phát Vnh Mexico và Thi hành liên quan bt nhm trong ngh cá tng cng Texas

  3. Psychrometric Bin Analysis for Alternative Cooling Strategies in Data Centers

    SciTech Connect (OSTI)

    Metzger, I.; VanGeet, O.; Rockenbaugh, C.; Dean, J.; Kurnik, C.

    2011-01-01

    Data centers are significant energy users and require continuous cooling to maintain high levels of computing performance. The majority of data centers have direct-expansion cooling which typically accounts for approximately 50% of the energy usage of data centers. However, using typical meteorological year 3 (TMY3) weather data and a simple psychometric bin analysis, alternative cooling strategies using a combination of economizer, evaporative, and supplemental DX cooling have been shown to be applicable in all climate zones in the United States. Average data center cooling energy savings across the U.S. was approximately 80%. Analysis of cooling energy savings is presented for various ASHRAE climate zones. The psychometric bin analysis is conducted for the ASHRAE recommended and allowable operating environment zones, as well as, a modified allowable operating environment. Control strategies are discussed. Finally, examples of energy efficient data centers using alternative cooling strategies are presented.

  4. Test Plan: WIPP bin-scale CH TRU waste tests

    SciTech Connect (OSTI)

    Molecke, M.A.

    1990-08-01

    This WIPP Bin-Scale CH TRU Waste Test program described herein will provide relevant composition and kinetic rate data on gas generation and consumption resulting from TRU waste degradation, as impacted by synergistic interactions due to multiple degradation modes, waste form preparation, long-term repository environmental effects, engineered barrier materials, and, possibly, engineered modifications to be developed. Similar data on waste-brine leachate compositions and potentially hazardous volatile organic compounds released by the wastes will also be provided. The quantitative data output from these tests and associated technical expertise are required by the WIPP Performance Assessment (PA) program studies, and for the scientific benefit of the overall WIPP project. This Test Plan describes the necessary scientific and technical aspects, justifications, and rational for successfully initiating and conducting the WIPP Bin-Scale CH TRU Waste Test program. This Test Plan is the controlling scientific design definition and overall requirements document for this WIPP in situ test, as defined by Sandia National Laboratories (SNL), scientific advisor to the US Department of Energy, WIPP Project Office (DOE/WPO). 55 refs., 16 figs., 19 tabs.

  5. Density and water content of nanoscale solid C-S-H formed in alkali-activated slag (AAS) paste and implications for chemical shrinkage

    SciTech Connect (OSTI)

    Thomas, Jeffrey J., E-mail: jthomas39@slb.com [Schlumberger-Doll Research, Cambridge, MA 02139 (United States); Allen, Andrew J. [National Institute of Standards and Technology, Gaithersburg, MD 20899 (United States); Jennings, Hamlin M. [CSHub, Department of Civil and Environmental Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139 (United States)

    2012-02-15

    Alkali-activated slag (AAS) paste was analyzed using small-angle neutron scattering (SANS). The scattering response indicates that the microstructure consists of a uniform matrix of hydration product with a high surface area studded with unhydrated cores of slag particles. In contrast with portland cement paste, no surface fractal scattering regime was detected, and elevated temperature curing (at 60 Degree-Sign C) had no detectable effect on the microstructure at any length scale studied. The specific surface area of the AAS pastes is about 25% higher than that of a portland cement paste cured under the same conditions. The composition and mass density of the nanoscale solid C-S-H phase formed in the AAS paste was determined using a previously developed neutron scattering method, in conjunction with a hydration model. The result ((CaO){sub 0.99}-SiO{sub 2}-(Al{sub 2}O{sub 3}){sub 0.06}-(H{sub 2}O){sub 0.97}, d = (2.73 {+-} 0.02) g/cm{sup 3}) is significantly lower in calcium and in water as compared to portland cement or pure tricalcium silicate paste. These values were used to calculate the chemical shrinkage that would result from complete hydration of the AAS paste. The result, (12.2 {+-} 1.5) cm{sup 3} of volumetric shrinkage per 100 g of unhydrated cement, is about twice the amount of chemical shrinkage exhibited by normal cement pastes.

  6. Distortion of power law blinking with binning and thresholding

    SciTech Connect (OSTI)

    Amecke, Nicole; Heber, André; Cichos, Frank, E-mail: cichos@physik.uni-leipzig.de [Molecular Nanophotonics Group, Institute of Experimental Physics I, Universität Leipzig, Linnéstraße 5, 04103 Leipzig (Germany)] [Molecular Nanophotonics Group, Institute of Experimental Physics I, Universität Leipzig, Linnéstraße 5, 04103 Leipzig (Germany)

    2014-03-21

    Fluorescence intermittency is a random switching between emitting (on) and non-emitting (off) periods found for many single chromophores such as semiconductor quantum dots and organic molecules. The statistics of the duration of on- and off-periods are commonly determined by thresholding the emission time trace of a single chromophore and appear to be power law distributed. Here we test with the help of simulations if the experimentally determined power law distributions can actually reflect the underlying statistics. We find that with the experimentally limited time resolution real power law statistics with exponents ?{sub on/off} ? 1.6, especially if ?{sub on} ? ?{sub off} would not be observed as such in the experimental data after binning and thresholding. Instead, a power law appearance could simply be obtained from the continuous distribution of intermediate intensity levels. This challenges much of the obtained data and the models describing the so-called power law blinking.

  7. Solid waste bin detection and classification using Dynamic Time Warping and MLP classifier

    SciTech Connect (OSTI)

    Islam, Md. Shafiqul; Hannan, M.A.; Basri, Hassan; Hussain, Aini; Arebey, Maher

    2014-02-15

    Highlights: • Solid waste bin level detection using Dynamic Time Warping (DTW). • Gabor wavelet filter is used to extract the solid waste image features. • Multi-Layer Perceptron classifier network is used for bin image classification. • The classification performance evaluated by ROC curve analysis. - Abstract: The increasing requirement for Solid Waste Management (SWM) has become a significant challenge for municipal authorities. A number of integrated systems and methods have introduced to overcome this challenge. Many researchers have aimed to develop an ideal SWM system, including approaches involving software-based routing, Geographic Information Systems (GIS), Radio-frequency Identification (RFID), or sensor intelligent bins. Image processing solutions for the Solid Waste (SW) collection have also been developed; however, during capturing the bin image, it is challenging to position the camera for getting a bin area centralized image. As yet, there is no ideal system which can correctly estimate the amount of SW. This paper briefly discusses an efficient image processing solution to overcome these problems. Dynamic Time Warping (DTW) was used for detecting and cropping the bin area and Gabor wavelet (GW) was introduced for feature extraction of the waste bin image. Image features were used to train the classifier. A Multi-Layer Perceptron (MLP) classifier was used to classify the waste bin level and estimate the amount of waste inside the bin. The area under the Receiver Operating Characteristic (ROC) curves was used to statistically evaluate classifier performance. The results of this developed system are comparable to previous image processing based system. The system demonstration using DTW with GW for feature extraction and an MLP classifier led to promising results with respect to the accuracy of waste level estimation (98.50%). The application can be used to optimize the routing of waste collection based on the estimated bin level.

  8. Cummins' Next Generation Tier 2, Bin 2 Light Truck Diesel Engine

    Broader source: Energy.gov [DOE]

    Development of a new light truck, in-line 4-cylinder turbocharged diesel engine that will meet Tier 2, Bin 2 emissions and at least a 40% fuel economy benefit over the V-8 gasoline engine it could replace

  9. Cummins Next Generation Tier 2, Bin 2 Light Truck Diesel engine

    Broader source: Energy.gov [DOE]

    Discusses plan, baselining, and modeling, for new light truck 4-cylinder turbocharged diesel meeting Tier 2, Bin 2 emissions and 40 percent better fuel economy than the V-8 gasoline engine it will replace

  10. A compact and reconfigurable silicon nitride time-bin entanglement circuit

    E-Print Network [OSTI]

    C. Xiong; X. Zhang; A. Mahendra; J. He; D. -Y. Choi; C. J. Chae; D. Marpaung; A. Leinse; R. G. Heideman; M. Hoekman; C. G. H. Roeloffzen; R. M. Oldenbeuving; P. W. L. van Dijk; C. Taddei; P. H. W. Leong; B. J. Eggleton

    2015-06-09

    Photonic chip based time-bin entanglement has attracted significant attention because of its potential for quantum communication and computation. Useful time-bin entanglement systems must be able to generate, manipulate and analyze entangled photons on a photonic chip for stable, scalable and reconfigurable operation. Here we report the first time-bin entanglement photonic chip that integrates time-bin generation, wavelength demultiplexing and entanglement analysis. A two-photon interference fringe with an 88.4% visibility is measured (without subtracting any noise), indicating the high performance of the chip. Our approach, based on a silicon nitride photonic circuit, which combines the low-loss characteristic of silica and tight integration features of silicon, paves the way for scalable real-world quantum information processors.

  11. Data Parallel Bin-Based Indexing for Answering Queries on Multi-Core Architectures

    E-Print Network [OSTI]

    Gosink, Luke

    2009-01-01

    DP-BIS) ?rst bins the base data, and then partitions andlocations in the OrBiC Base Data, and Row-ID tables for thesolely on a column’s base data; this smaller data footprint

  12. Theory uncertainties for Higgs mass and other searches using jet bins

    E-Print Network [OSTI]

    Stewart, Iain

    Bounds on the Higgs mass from the Tevatron and LHC are determined using exclusive jet bins to maximize sensitivity. Scale variation in exclusive fixed-order predictions underestimates the perturbative uncertainty for these ...

  13. Diurnal Precipitation Regimes in the Global Tropics* KAZUYOSHI KIKUCHI AND BIN WANG

    E-Print Network [OSTI]

    Wang, Bin

    Diurnal Precipitation Regimes in the Global Tropics* KAZUYOSHI KIKUCHI AND BIN WANG Department tropical precipitation are documented by using two complementary Tropical Rainfall Measuring Mission (TRMM, and phase propagation characteristics of the diurnal precipitation. The oceanic regime is characterized

  14. Naturalness Under Stress: SUSY after 5 fb-1 West Coast LHC Meeting, December, 2011

    E-Print Network [OSTI]

    California at Santa Cruz, University of

    Naturalness Under Stress: SUSY after 5 fb-1 West Coast LHC Meeting, December, 2011 Michael Dine of us in some productive, new directions. Some of the arguments will be bottom up, some top down scale in the TeV MZ energy range. Possibly within two weeks and almost certainly within a year, we

  15. nh Gi Tn Hi Ti Nguyn Thin Nhin do Trn Du Deep Horizon D n ng b bin sng Alabama

    E-Print Network [OSTI]

    nguyên liu ê chn sóng t nhiên hoc nhân to ngn chn ngun sóng, bo v b bin sinh thái, cùng lúc cng to nên

  16. Time-bin entangled photon pair generation from Si micro-ring resonator

    E-Print Network [OSTI]

    Ryota Wakabayashi; Mikio Fujiwara; Ken-ichiro Yoshino; Yoshihiro Nambu; Masahide Sasaki; Takao Aoki

    2015-01-23

    We demonstrate time-bin entanglement generation in telecom wavelength using a 7 {\\mu}m radius Si micro-ring resonator pumped by a continuous wave laser. The resonator structure can enhance spontaneous four wave mixing, leading to a photon pair generation rate of about 90-100 Hz with a laser pump power of as low as -3.92 dBm (0.41 mW). We succeed in observing time-bin entanglement with the visibility over 92%. Moreover, wavelength-tunability of the entangled photon pair is demonstrated by changing the operation temperature.

  17. Decay constants $f_B$ and $f_{B_s}$ from HISQ simulations

    E-Print Network [OSTI]

    Fermilab Lattice; MILC Collaborations; :; A. Bazavov; C. Bernard; C. Bouchard; N. Brown; C. DeTar; D. Du; A. X. El-Khadra; E. D. Freeland; E. Gámiz; Steven Gottlieb; U. M. Heller; J. Komijani; A. S. Kronfeld; J. Laiho; L. Levkova; P. B. Mackenzie; C. Monahan; T. Primer; Heechang Na; E. T. Neil; J. N. Simone; R. L. Sugar; D. Toussaint; R. S. Van de Water; R. Zhou

    2015-11-07

    We give a progress report on a project aimed at a high-precision calculation of the decay constants $f_B$ and $f_{B_s}$ from simulations with HISQ heavy and light valence and sea quarks. Calculations are carried out with several heavy valence-quark masses on ensembles with 2+1+1 flavors of HISQ sea quarks at five lattice spacings and several light sea-quark mass ratios $m_{ud}/m_s$, including approximately physical sea-quark masses. This range of parameters provides excellent control of the continuum limit and of heavy-quark discretization errors. We present a preliminary error budget with projected uncertainties of 2.2~MeV and 1.5~MeV for $f_B$ and $f_{B_s}$, respectively.

  18. Decay constants $f_B$ and $f_{B_s}$ from HISQ simulations

    E-Print Network [OSTI]

    Lattice, Fermilab; Bazavov, A; Bernard, C; Bouchard, C; Brown, N; DeTar, C; Du, D; El-Khadra, A X; Freeland, E D; Gámiz, E; Gottlieb, Steven; Heller, U M; Komijani, J; Kronfeld, A S; Laiho, J; Levkova, L; Mackenzie, P B; Monahan, C; Primer, T; Na, Heechang; Neil, E T; Simone, J N; Sugar, R L; Toussaint, D; Van de Water, R S; Zhou, R

    2015-01-01

    We give a progress report on a project aimed at a high-precision calculation of the decay constants $f_B$ and $f_{B_s}$ from simulations with HISQ heavy and light valence and sea quarks. Calculations are carried out with several heavy valence-quark masses on ensembles with 2+1+1 flavors of HISQ sea quarks at five lattice spacings and several light sea-quark mass ratios $m_{ud}/m_s$, including approximately physical sea-quark masses. This range of parameters provides excellent control of the continuum limit and of heavy-quark discretization errors. We present a preliminary error budget with projected uncertainties of 2.2~MeV and 1.5~MeV for $f_B$ and $f_{B_s}$, respectively.

  19. A Bin Method for Calculating Energy Conservation Retrofit Savings in Commercial Buildings 

    E-Print Network [OSTI]

    Thamilseran, S.; Haberl, J. S.

    1994-01-01

    models do not fit the data adequately. This paper presents a first look at an hourly bin method for calculating energy savings from energy conservation retrofits to HVAC systems based on hourly whole-building electricity, sub-metered motor control center...

  20. On the Security of Some Proxy Signature Hung-Min Sun and Bin-Tsan Hsieh

    E-Print Network [OSTI]

    International Association for Cryptologic Research (IACR)

    On the Security of Some Proxy Signature Schemes Hung-Min Sun and Bin-Tsan Hsieh Department of proxy signature schemes, a proxy signature scheme should provide good security properties. In 1999, Sun own public key with other's public key. To overcome these security flaws, Sun and Hsieh also proposed

  1. On the Security of Some Proxy Signature HungMin Sun and BinTsan Hsieh +

    E-Print Network [OSTI]

    International Association for Cryptologic Research (IACR)

    On the Security of Some Proxy Signature Schemes Hung­Min Sun and Bin­Tsan Hsieh + Department of proxy signature schemes, a proxy signature scheme should provide good security properties. In 1999, Sun own public key with other's public key. To overcome these security flaws, Sun and Hsieh also proposed

  2. Presentation 2.7: Energy and the Forest Products Industry in Malaysia Zulkifli Bin Ahmad

    E-Print Network [OSTI]

    on alternative energy to replace petroleum. Malaysia introduced "biodiesel" as a first step to reduce the usePresentation 2.7: Energy and the Forest Products Industry in Malaysia Zulkifli Bin Ahmad Director of Forest Industries Forestry Department of Peninsular Malaysia E-mail: zulmad@gmail.com Abstract Energy

  3. Coding and Compression: a Happy Union of Theory and Practice Jorma Risssanen \\Lambda Bin Yu y

    E-Print Network [OSTI]

    Yu, Bin

    that followed, information theory provided fundamental limits for communication in general and coding theory is intrinsically statistical. Moreover, the algorithmic theory of information has inspiredCoding and Compression: a Happy Union of Theory and Practice Jorma Risssanen \\Lambda Bin Yu y 1

  4. Some New Adaptive Protocols for the Wireless Relay Channel Bin Zhao and Matthew C. Valenti

    E-Print Network [OSTI]

    Valenti, Matthew C.

    Some New Adaptive Protocols for the Wireless Relay Channel Bin Zhao and Matthew C. Valenti Lane}@csee.wvu.edu Abstract The AWGN capacity is given for several adaptive relaying schemes. A constraint is imposed renewed interest due to its ability to achieve distributed spatial diversity in a manner analogous

  5. Long term laboratory corrosion monitoring of calcine bin set materials exposed to zirconia calcine

    SciTech Connect (OSTI)

    Dirk, W.J.

    1994-06-01

    Corrosion testing of Type 1025 carbon steel, 405, 304, 304L, 316L, and 347 stainless steels, and 6061-T6 aluminum were conducted in synthetic zirconia calcine to model long term corrosion performance of bin set material. Testing was conducted over a period of 17 years. The existing calcine bin set {number_sign}1 is constructed of Type 405 stainless steel, 2 through 4 are constructed of Type 304 stainless steel and 5 through 7 are constructed of Type 304L stainless steel. The highest rate observed for Type 304L stainless steel was 8.1 {times} 10{sup {minus}7} inches per month. This would equal a wall thickness loss of about 5 mils after 500 years of storage. Currently, the established schedule for removal of corrosion test coupons from the calcine storage bins is at the end of the 10th, 100th, 250th, and 450th year of solid storage service. Very low corrosion rates and metal oxide data determined from the long term laboratory test, in conjunction with corrosion rates from the coupon assessment of the second bin set, indicate this schedule should be revised from 10 years to 50 years for the first assessment.

  6. Reaction-time binning: A simple method for increasing the resolving power of ERP averages

    E-Print Network [OSTI]

    Poli, Riccardo

    Reaction-time binning: A simple method for increasing the resolving power of ERP averages RICCARDO-locked, response-locked, and ERP-locked averaging are effective methods for reducing artifacts in ERP analysis. However, they suffer from a magnifying-glass effect: they increase the resolution of specific ERPs

  7. ROME: Road Monitoring and Alert System through Bin Zan Tingting Sun Marco Gruteser Yanyong Zhang

    E-Print Network [OSTI]

    Gruteser, Marco

    1 ROME: Road Monitoring and Alert System through Geocache Bin Zan Tingting Sun Marco Gruteser, NJ 08902-3390 {zanb,sunting,gruteser,yyzhang}@winlab.rutgers.edu Abstract--We present a road from aggregated readings of multiple devices. For example, road monitoring could infer road defects

  8. Comparison of an alternative and existing binning methods to reduce the acquisition duration of 4D PET/CT

    SciTech Connect (OSTI)

    Didierlaurent, David, E-mail: dadidierlaurent@gmail.com; Ribes, Sophie; Caselles, Olivier [SIMAD, LU 50, Université Toulouse III Paul Sabatier, Toulouse 31062 (France); Jaudet, Cyril; Dierickx, Lawrence O.; Zerdoud, Slimane; Brillouet, Severine; Weits, Kathleen [Institut Claudius Regaud, 20-24 Rue du Pont Saint-Pierre, Toulouse 31052 (France); Batatia, Hadj [IRIT-INPT, Université Toulouse III Paul Sabatier, Toulouse 31071 (France); Courbon, Frédéric [GCS CHU-CLCC, Université Toulouse III Paul Sabatier, Toulouse 31052 (France)

    2014-11-01

    Purpose: Respiratory motion is a source of artifacts that reduce image quality in PET. Four dimensional (4D) PET/CT is one approach to overcome this problem. Existing techniques to limiting the effects of respiratory motions are based on prospective phase binning which requires a long acquisition duration (15–25 min). This time is uncomfortable for the patients and limits the clinical exploitation of 4D PET/CT. In this work, the authors evaluated an existing method and an alternative retrospective binning method to reduce the acquisition duration of 4D PET/CT. Methods: The authors studied an existing mixed-amplitude binning (MAB) method and an alternative binning method by mixed-phases (MPhB). Before implementing MPhB, they analyzed the regularity of the breathing patterns in patients. They studied the breathing signal drift and missing CT slices that could be challenging for implementing MAB. They compared the performance of MAB and MPhB with current binning methods to measure the maximum uptake, internal volume, and maximal range of tumor motion. Results: MPhB can be implemented depending on an optimal phase (in average, the exhalation peak phase ?4.1% of the entire breathing cycle duration). Signal drift of patients was in average 35% relative to the breathing amplitude. Even after correcting this drift, MAB was feasible in 4D CT for only 64% of patients. No significant differences appeared between the different binning methods to measure the maximum uptake, internal volume, and maximal range of tumor motion. The authors also determined the inaccuracies of MAB and MPhB to measure the maximum amplitude of tumor motion with three bins (less than 3 mm for movement inferior to 12 mm, up to 6.4 mm for a 21 mm movement). Conclusions: The authors proposed an alternative binning method by mixed-phase binning that halves the acquisition duration of 4D PET/CT. Mixed-amplitude binning was challenging because of signal drift and missing CT slices. They showed that more than three bins were necessary for a more accurate measurement of the maximum amplitude of the tumor motion. However, the current 4D-CT technology limits the increase of the number of bins in 4D PET/CT because of missing CT slices. One can reconstruct 4D PET images with more bins but without attenuation/scatter correction.

  9. The first of a series of high efficiency, high bmep, turbocharged two-stroke cycle diesel engines; the general motors EMD 645FB engine

    SciTech Connect (OSTI)

    Kotlin, J.J.; Dunteman, N.R.; Scott, D.I.; Williams, H.A. Jr.

    1983-01-01

    The current Electro-Motive Division 645 Series turbocharged engines are the Model FB and EC. The FB engine combines the highest thermal efficiency with the highest specific output of any EMD engine to date. The FB Series incorporates 16:1 compression ratio with a fire ring piston and an improved turbocharger design. Engine components included in the FB engine provide very high output levels with exceptional reliability. This paper also describes the performance of the lower rated Model EC engine series which feature high thermal efficiency and utilize many engine components well proven in service and basic to the Model FB Series.

  10. Optimization of Engine-out Emissions from a Diesel Engine to Meet Tier 2 Bin 5 Emission Limits

    Broader source: Energy.gov [DOE]

    Drastic reduction of engine-out emissions and complicated aftertreatment system comprising of oxidation catalyst, particulate filter, and DeNOx catalyst are implemented to meet Tier 2 Bin 5 limits for U.S. market diesel engines.

  11. Global Search for New Physics with 2.0 fb88-1 at CDF

    SciTech Connect (OSTI)

    Aaltonen, T.; Adelman, J.; Akimoto, T.; Albrow, Michael G.; Alvarez Gonzalez, B.; Amerio, S.; Amidei, Dante E.; Anastassov, A.; Annovi, Alberto; Antos, J.; Apollinari, G.; /Fermilab /Purdue U.

    2008-09-01

    Data collected in Run II of the Fermilab Tevatron are searched for indications of new electroweak-scale physics. Rather than focusing on particular new physics scenarios, CDF data are analyzed for discrepancies with the standard model prediction. A model-independent approach (VISTA) considers gross features of the data, and is sensitive to new large cross-section physics. Further sensitivity to new physics is provided by two additional algorithms: a Bump Hunter searches invariant mass distributions for 'bumps' that could indicate resonant production of new particles; and the Sleuth procedure scans for data excesses at large summed transverse momentum. This combined global search for new physics in 2.0 fb{sup -1} of p{bar p} collisions at {radical}s = 1.96 TeV reveals no indication of physics beyond the standard model.

  12. Measurement of the anomalous like-sign dimuon charge asymmetry with 9 fb?¹ of pp? collisions

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; et al

    2011-09-16

    We present an updated measurement of the anomalous like-sign dimuon charge asymmetry Absl for semileptonic b-hadron decays in 9.0 fb?¹ of pp? collisions recorded with the D0 detector at a center-of-mass energy of ?s=1.96 TeV at the Fermilab Tevatron collider. We obtain Absl=(-0.787±0.172(stat)±0.093(syst))%. This result differs by 3.9 standard deviations from the prediction of the standard model and provides evidence for anomalously large CP violation in semileptonic neutral B decay. The dependence of the asymmetry on the muon impact parameter is consistent with the hypothesis that it originates from semileptonic b-hadron decays.

  13. Protein Expression Profile of an Environmentally Important Bacterial Strain: the Chromate Response of Arthrobacter Species Strain FB24

    SciTech Connect (OSTI)

    Henne, Kristene L.; Turse, Joshua E.; Nakatsu, C. H.; Konopka, Allan

    2011-05-03

    The global proteomic response of Arthrobacter sp. strain FB24 to different levels of chromate stress was evaluated with both two-dimensional gel electrophoresis (2-DGE) and liquid chromatography coupled to tandem mass spectrometry (LC/LC-MS/MS) [Henne et al. 2009b]. Proteome coverage of 22% and 71% was obtained with 2-DGE and LC/LC-MS/MS, respectively. The strong response of strain FB24 to chromate suggests a condition of sulfur limitation, which could be driven by competition for the sulfate transporter by the structurally similar chromate ion. Additionally, the involvement of genes hypothesized to be directly involved in chromate resistance in strain FB24 was supported at the protein level.

  14. Coherence and degree of time-bin entanglement from quantum dots

    E-Print Network [OSTI]

    Tobias Huber; Laurin Ostermann; Maximilian Prilmüller; Glenn S. Solomon; Helmut Ritsch; Gregor Weihs; Ana Predojevi?

    2015-06-08

    We report on the generation of time-bin entangled photon pairs from a semiconductor quantum dot via pulsed resonant biexciton generation. Based on theoretical modeling we optimized the duration of the excitation pulse to minimize the laser-induced dephasing and increase the biexciton-to-background single exciton occupation probability. This results in a high degree of entanglement with a concurrence of up to 0.78(6) and a 0.88(3) overlap with a maximally entangled state. Theoretical simulations also indicate a power dependent nature of the dephasing during the laser excitation that limits the coherence of the excitation process.

  15. Hurricane Disturbance Alters Secondary Forest Recovery in Puerto Rico Dan F.B. Flynn1,7

    E-Print Network [OSTI]

    Uriarte, Maria

    Hurricane Disturbance Alters Secondary Forest Recovery in Puerto Rico Dan F.B. Flynn1,7 , Mar structure and composition. How introduced species respond to disturbances such as hurricanes in post-agriculture forest recovery is of particular interest. To examine the effects of hurricane disturbance and previous

  16. Predicting yearly energy savings using BIN weather data with heat-pipe heat exchangers

    SciTech Connect (OSTI)

    Mathur, G.D. [Zexel USA Corp., Decatur, IL (United States)

    1997-12-31

    In an earlier paper, the author had investigated the impact that a heat pipe heat exchanger (HPHE) has on the energy consumption and the peak demand on an existing air conditioning system. A detailed performance investigation was carried out for a number of cities for year round operation of the HVAC system with HPHE. Heating degree days and cooling hours were used for predicting the energy savings with the HPHE. In order to calculate the true energy savings, a more realistic approach is to use the BIN weather data. The author has developed a simulation program that can predict the energy savings by using the BIN weather data. The investigation has been carried out for 33 US cities with widely different climactic conditions and the results are presented in this paper. Economic analysis reveals that a simple retrofit on an existing HVAC system can pay for itself in less than a year. Based on this investigation, it is recommended that electric utilities use this technology as a demand side management strategy for reducing energy and peak demand.

  17. A note on comparing response times in the M/GI/1/FB and M/GI/1/PS queues

    E-Print Network [OSTI]

    the overall mean response time (a.k.a. sojourn time) of the PS and FB queues under an M/GI/1 system. We show from optimal mean response time (a.k.a sojourn time). The Shortest-Remaining-Processing-Time (SRPT have the least attained service (a.k.a age), they time-share the processor via PS. By biasing towards

  18. A note on comparing response times in the M/GI/1/FB and M/GI/1/PS queues

    E-Print Network [OSTI]

    the overall mean response time (a.k.a. sojourn time) of the PS and FB queues under an M/GI/1 system. We show from optimal mean response time (a.k.a sojourn time). The Shortest­Remaining­Processing­Time (SRPT have the least attained service (a.k.a age), they time­share the processor via PS. By biasing towards

  19. Performance evaluation of source extraction in wireless sensor networks Hong-Bin Chen a,b,*, Chi Kong Tse a

    E-Print Network [OSTI]

    Tse, Chi K. "Michael"

    Performance evaluation of source extraction in wireless sensor networks Hong-Bin Chen a,b,*, Chi wireless sensor networks are evaluated. The sensor observations are assumed to be linear instantaneous: Available online 6 May 2008 Keywords: Wireless sensor network Blind source separation Cluster Performance

  20. Hydrogen-doped cubic diamond and the crystal structure of n-diamond Bin Wen a,b,

    E-Print Network [OSTI]

    Melnik, Roderick

    Hydrogen-doped cubic diamond and the crystal structure of n-diamond Bin Wen a,b, , Roderick Melnik. In particular, hydrogen concen- tration dependent elastic constants and lattice parameters for the H-doped diamond have been analyzed. Our results indicate that when the hydrogen concentration is less than 19 at

  1. A New Upper Bound 2.5545 on 2D Online Bin Packing XIN HAN, Dalian University of Technology

    E-Print Network [OSTI]

    Chin, Francis Y.L.

    50 A New Upper Bound 2.5545 on 2D Online Bin Packing XIN HAN, Dalian University of Technology was partially supported by NSFC (10971192). Authors' addresses: X. Han, Software School, Dalian University of Technology, Road 8, Economy and Tech- nology Development Zone, Dalian, P.R. China, 116620; email: hanxin

  2. Preparation of BaPbO3 functional ceramics from leaded waste Bin Li, Shen-Gen Zhang*, Kun Zhang,

    E-Print Network [OSTI]

    Volinsky, Alex A.

    Preparation of BaPbO3 functional ceramics from leaded waste Bin Li, Shen-Gen Zhang*, Kun Zhang, De conductive ceramics from leaded waste. The experimental results show that BaPbO3 powder syn- thesized at 700 in the air. Synthesized BaPbO3 ceramics have high Curie temperature and high-temperature positive temperature

  3. Segmentation and Tracking of Mesoscale Eddies in Numeric Ocean Models Vishal Sood, Bin John, Ramprasad Balasubramanian and Amit Tandon*

    E-Print Network [OSTI]

    Tandon, Amit

    Segmentation and Tracking of Mesoscale Eddies in Numeric Ocean Models Vishal Sood, Bin John suggested that the mesoscale eddies and mesoscale features play a strong role in carrying heat poleward oceanographers an invaluable tool to assess mesoscale eddies and the Lagrangian characteristics of this mesoscale

  4. Cko.efer f. (i.f\\~f':tn\\ltt E'~~CS'\\'~ A~\\ !f~ \\fb a... 'T":~4.r.-t..

    E-Print Network [OSTI]

    Li, Kin-Yin

    QC~-®! Cko.efer f. (i.f\\~f':tn\\ltt E'~~CS'\\'~ A~\\ !f~ \\fb a... 'T":~4.r.-t.. ~c-l.;~. ~e...CA weo

  5. Search for Sneutrino Production in e? Final States in 5.3??fb(?1) of pp-bar Collisions at s?=1.96??TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Clutter, Justace Randall; McGivern, Carrie Lynne; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Abolins, M.; Acharya, B. S.; Adams, M.; Adams, T.

    2010-11-05

    We report the results of a search for R parity violating (RPV) interactions leading to the production of supersymmetric sneutrinos decaying into e? final states using 5.3??fb(?1) of integrated luminosity collected by the ...

  6. Taking Halo-Independent Dark Matter Methods Out of the Bin

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Fox, Patrick J.; Kahn, Yonatan; McCullough, Matthew

    2014-10-30

    We develop a new halo-independent strategy for analyzing emerging DM hints, utilizing the method of extended maximum likelihood. This approach does not require the binning of events, making it uniquely suited to the analysis of emerging DM direct detection hints. It determines a preferred envelope, at a given confidence level, for the DM velocity integral which best fits the data using all available information and can be used even in the case of a single anomalous scattering event. All of the halo-independent information from a direct detection result may then be presented in a single plot, allowing simple comparisons betweenmore »multiple experiments. This results in the halo-independent analogue of the usual mass and cross-section plots found in typical direct detection analyses, where limit curves may be compared with best-fit regions in halo-space. The method is straightforward to implement, using already-established techniques, and its utility is demonstrated through the first unbinned halo-independent comparison of the three anomalous events observed in the CDMS-Si detector with recent limits from the LUX experiment.« less

  7. Generation and Eight-port Homodyne Characterization of Time-bin Qubits for Continuous-variable Quantum Information Processing

    E-Print Network [OSTI]

    Shuntaro Takeda; Takahiro Mizuta; Maria Fuwa; Jun-ichi Yoshikawa; Hidehiro Yonezawa; Akira Furusawa

    2013-02-05

    We experimentally generate arbitrary time-bin qubits using continuous-wave light. The advantage unique to our qubit is its compatibility with deterministic continuous-variable quantum information processing. This compatibility comes from its optical coherence with continuous waves, well-defined spatio-temporal mode, and frequency spectrum within the operational bandwidth of the current continuous-variable technology. We also demonstrate an efficient scheme to characterize time-bin qubits via eight-port homodyne measurement. This enables the complete characterization of the qubits as two-mode states, as well as a flexible analysis equivalent to the conventional scheme based on a Mach-Zehnder interferometer and photon-detection.

  8. Measurement of the W boson helicity in top quark decays using 5.4 fb?¹ of pp? collision data

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; et al

    2011-02-01

    We present a measurement of the helicity of the W boson produced in top quark decays using tt¯ decays in the l+jets and dilepton final states selected from a sample of 5.4 fb?¹ of collisions recorded using the D0 detector at the Fermilab Tevatron pp? collider. We measure the fractions of longitudinal and right-handed W bosons to be f?=0.669±0.102[±0.078(stat.)±0.065(syst.)] and f?=0.023±0.053[±0.041(stat.)±0.034(syst.)], respectively. This result is consistent at the 98% level with the standard model. A measurement with f? fixed to the value from the standard model yields f?=0.010±0.037[±0.022(stat.)±0.030(syst.)].

  9. Search for WH associated production in 5.3 fb -1 of pp¯ collisions at the Fermilab Tevatron

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V.M.; Abbott, B.; Acharya, B.S.; Adams, M.; Adams, T.; Alexeev, G.D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G.A.; et al

    2011-03-01

    We present a search for associated production of Higgs and W bosons in collisions at a center of mass energy of in 5.3 fb -1 of integrated luminosity recorded by the D0 experiment. Multivariate analysis techniques are applied to events containing one lepton, an imbalance in transverse energy, and one or two b-tagged jets to discriminate a potential WH signal from Standard Model backgrounds. We observe good agreement between data and expected backgrounds, and set an upper limit of 4.5 (at 95% confidence level and for mH=115 GeV) on the ratio of the WH cross section multiplied by the branchingmore »fraction of H ? bb¯ to its Standard Model prediction, which is consistent with an expected limit of 4.8.« less

  10. ENERGY ECONOMY CII5fB 81 (R3) (L2) (M2) UDC 728.3 (489) Low-energy houses

    E-Print Network [OSTI]

    solutions as to design, choice of building materials, heating systems, energy sources, etc. (ref. 1). EachENERGY ECONOMY CII5fB 81 (R3) (L2) (M2) UDC 728.3 (489) Low-energy houses: insulation and air tightness by Bjarne Saxhof and Allan A. Nielsen 142 The Hjortekar project of six low energy house designs

  11. Combined search for the Standard Model Higgs boson using up to 4.9 fb[superscript ?1] of pp collision data at ?s = 7 TeV with the ATLAS detector at the LHC

    E-Print Network [OSTI]

    Taylor, Frank E.

    A combined search for the Standard Model Higgs boson with the ATLAS experiment at the LHC using datasets corresponding to integrated luminosities from 1.04 fb[superscript ?1] to 4.9 fb[superscript ?1] of pp collisions ...

  12. Combined CDF and D0 Searches for the Standard Model Higgs Boson Decaying to Two Photons with up to 8.2 fb^-1

    E-Print Network [OSTI]

    The CDF Collaboration; the D0 Collaboration; the Tevatron New Physics; Higgs Working Group

    2011-07-25

    We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in ppbar collisions at the Fermilab Tevatron at sqrt{s}=1.96 TeV, focusing on the decay H\\rightarrow\\gamma\\gamma. We compute upper limits on the Higgs boson production cross section times the decay branching fraction in the range 100Higgs boson. With datasets corresponding to 7.0 fb-1 (CDF) and 8.2 fb-1 (D0), the 95% C.L. upper limits on Higgs boson production is a factor of 10.5 times the SM cross section for a Higgs boson mass of 115 GeV/c^2.

  13. Search for New Heavy Resonances Decaying To t+t^- Pairs at the LHC with Square Root S= 7 TEV (L = 5.0 FB^-1) 

    E-Print Network [OSTI]

    Suarez, Indara

    2015-01-22

    for Heavy Resonances . . . . . . . . . . . . . . . . 17 3. THE LARGE HADRON COLLIDER AND THE CMS DETECTOR . . . 21 3.1 The Large Hadron Collider . . . . . . . . . . . . . . . . . . . . . . . . 21 3.2 The Compact Muon Solenoid Detector...V center-of-mass energy to the CMS detector. CMS recorded 5.55 fb?1 of data. . . . . . . . . . . 23 3.3 Cross-sectional View of the CMS Detector. The subdetectors in or- der from the interaction point outward are the pixel detector, the sili- con tracker...

  14. Search for Randall-Sundrum Gravitons in Dilepton and Diphoton Final States with 1 fb-1 of Data

    SciTech Connect (OSTI)

    Das, Amitabha; /Boston U.

    2007-05-01

    The work presented in this thesis is the search for Randall-Sundrum (RS) gravitons from an analysis of approximately 1 fb{sup -1} data collected with the D0 detector at Fermilab. The standard model has been a great success in explaining all experimental observations in particle physics. However, we also know that it has fundamental problems. One of these problems, called the hierarchy problem, is related to the large difference between the electroweak scale and the Planck scale. The model proposed by Randall and Sundrum presents a possible solution to the hierarchy problem by introducing physics beyond the standard model. Randall and Sundrum's theory postulates the existence of a 4th spatial dimension in addition to the conventional (3+1)-dimensional space. Gravity is localized on a 3+1 dimensional subspace, called a brane (Planck brane) that is separated in this new 4th spatial dimension from the standard model brane. As one moves away from this Planck brane, gravity is exponentially suppressed and this explains why gravity appears so weak at the standard model brane. In the simplest RS model, the only particles that propagate in the extra dimension are gravitons. The graviton manifests itself on the standard model brane as a series of excited states that couple to standard model particles with similar strength as the electroweak interaction. The ground state is the massless graviton and the order of magnitude of the mass of the lowest excited state is expected to be one TeV. The first excited mode of the graviton might be produced resonantly at the Tevatron. Gravitons can decay into fermion-antifermion or diboson pairs. Here I search for gravitons through their decay to e{sup +}e{sup -} and {gamma}{gamma} final states. These final states have similar signatures in our detector and can thus be treated together. After analyzing the data I do not find any excess over standard model expectations and set an upper limit on the production rate of such gravitons. I compare this limit to the production rate predicted by the theory for a range of possible couplings and set mass limits on the lowest excited gravitons state of up to 898 GeV.

  15. Search for the Standard Model Higgs Boson in the Diphoton Decay Channel with 4.9??fb[superscript -1] of pp Collision Data at ?s=7??TeV with ATLAS

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for the standard model Higgs boson is performed in the diphoton decay channel. The data used correspond to an integrated luminosity of 4.9??fb[superscript -1] collected with the ATLAS detector at the Large Hadron ...

  16. Search for Randall-Sundrum Gravitons in Dielectron and Diphoton Final States with 5.4fb-1 of D0 Data

    SciTech Connect (OSTI)

    Zhou, Ning; /Columbia U.

    2010-03-01

    A search for the lightest Kaluza-Klein mode of the graviton in the Randall-Sundrum model with a warped extra dimension is performed in the dielectron and diphoton channels. The data set used for the search corresponds to 5.4 fb{sup -1} of data from p{bar p} collisions at a center-of-mass energy of 1.96 TeV, collected with the D0 detector at the Fermilab Tevatron between July 2002 and Summer 2009. We search for resonances in the invariant mass spectrum of two electromagnetic showers from the decay of the graviton to either electron-positron pairs or photon pairs. To optimize the sensitivity, the dielectron and diphoton channels are analyzed separately, then the results are combined together in the end. We also investigate whether, due to the unique spin-2 nature of the graviton, the angular distribution of the final state particles can be used to significantly enhance the sensitivity of the search. We set 95% confidence level upper limits on the graviton production cross section times branching fraction into electron-positron pairs of between {approx} 7 fb and {approx} 0.5 fb for a range of graviton masses from 220 GeV and 1050 GeV, respectively. Compared with Randall-Sundrum model predictions, these results correspond to lower limits on the lightest graviton mass between 440 GeV and 1040 GeV, for the dimensionless graviton coupling to the Standard Model fields k/{bar M}{sub Pl} in the range from 0.01 to 0.1. In addition, for coupling k/{bar M}{sub Pl} of 0.01, gravitons with masses between 460 GeV and 560 GeV are also excluded at 95% confidence level. These results represent the most sensitive limits to date.

  17. Predicting yearly energy savings using BIN weather data with heat-pipe heat exchangers with indirect evaporative cooling

    SciTech Connect (OSTI)

    Mathur, G.D.

    1998-07-01

    Heat-Pipe Heat-Exchangers (HPHE) are passive systems that have recently seen application in energy recovery (Mathur, 1997). A HPHE consists of individual closed end heat pipe tubes that are charged with a suitable working fluid. In these systems, the working fluid evaporates on one side of the heat exchanger and condenses over the other end of the heat exchanger. The condensed fluid returns back to the evaporator section through the capillary action of the wick. The performance of a HPHE system can be improved by the raising the condenser portion of the heat exchanger which facilitates effective return of the condensate back to the evaporator. HPHE can be used with air conditioning systems as retrofits and in new applications. For retrofit applications, the operating costs are reduced because of the reduction in the energy (kWh) and peak demand (kW) consumptions. For new installations, the heating and cooling equipment can be of smaller capacity which will result in lower equipment and operating costs. During the summer season, indirect evaporative cooling can also be used to further enhance the performance of the air conditioning system. When operated during both the heating and cooling seasons, a HPHE yields four types of savings: (i) Heating equipment savings (ii) Cooling equipment savings (iii) Heating operating savings (iv) Cooling operating savings. Savings in the energy consumption for both heating and cooling were calculated with the HPHE for 30 cities with widely different climactic conditions. The payback periods for most of the cities were less than 1 year. If indirect evaporative cooling is used during the summer season, more energy savings would be realized on an yearly basis along with further reductions in the peak demand. In this paper, the author has simulated the performance of a HPHE with indirect evaporative cooling using the BIN weather data.

  18. Combined CDF and D0 Upper Limits on Standard Model Higgs Boson Production with up to 8.2 fb-1 of Data

    E-Print Network [OSTI]

    The CDF; D0 Collaborations; the TEVNPHWG Working Group

    2011-08-16

    We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in p-pbar collisions at the Fermilab Tevatron at sqrt(s)=1.96 TeV. The results presented here include those channels which are most sensitive to Higgs bosons with mass between 130 and 200 GeV/c^2, namely searches targeted at Higgs boson decays to W+W-, although acceptance for decays into tau+tau- and gamma gamma is included. Compared to the previous Tevatron Higgs search combination, more data have been added and the analyses have been improved to gain sensitivity. We use the MSTW08 parton distribution functions and the latest gg to H theoretical cross section predictions when testing for the presence of a SM Higgs boson. With up to 7.1 fb-1 of data analyzed at CDF, and up to 8.2 fb-1 at D0, the 95% C.L. upper limits on Higgs boson production is a factor of 0.54 times the SM cross section for a Higgs boson mass of 165 GeV/c^2. We exclude at the 95% C.L. the region 158

  19. Combined CDF and D0 Searches for the Standard Model Higgs Boson Decaying to Two Photons with up to 8.2 fb^-1

    SciTech Connect (OSTI)

    Not Available

    2011-07-01

    We combine results from CDF and D0's direct searches for the standard model (SM) Higgs boson (H) produced in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV, focusing on the decay H {yields} {gamma}{gamma}. We compute upper limits on the Higgs boson production cross section times the decay branching fraction in the range 100 < m{sub H} < 150 GeV/c{sup 2}, and we interpret the results in the context of the standard model. We use the MSTW08 parton distribution functions and the latest theoretical cross section predictions when testing for the presence of a SM Higgs boson. With datasets corresponding to 7.0 fb{sup -1} (CDF) and 8.2 fb{sup -1} (D0), the 95% C.L. upper limits on Higgs boson production is a factor of 10.5 times the SM cross section for a Higgs boson mass of 115 GeV/c{sup 2}.

  20. bin.dvi

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos Alamos verifiesValidationENCOAL® MildEffects ofDemonstration

  1. Review for Howard Ochman ---CSH book Microbial Evolution

    E-Print Network [OSTI]

    Roth, John R.

    selection: How natural selection mimics mutability (adaptive mutation) Sophie Maisnier-Patin smaisnierpatin, the conclusion is suspect in the light of recent evidence that revertant colonies are initiated by pre whether or not some adaptive mutations form at a higher rate in response to selection. However the classic

  2. Generation of 1.5-um band time-bin entanglement using spontaneous fiber four-wave mixing and planar lightwave circuit interferometers

    E-Print Network [OSTI]

    Hiroki Takesue; Kyo Inoue

    2005-08-29

    This paper reports 1.5-um band time-bin entanglement generation. We employed a spontaneous four-wave mixing process in a dispersion shifted fiber, with which correlated photon pairs with very narrow bandwidths were generated efficiently. To observe two-photon interference, we used planar lightwave circuit based interferometers that were operated stably without feedback control. As a result, we obtained coincidence fringes with 99 % visibilities after subtracting accidental coincidences, and successfully distributed entangled photons over 20-km standard single-mode fiber without any deterioration in the quantum correlation.

  3. Search for new physics in the dijet mass distribution using 1 fb?¹ of pp collision data at ?s = 7 TeV collected by the ATLAS detector

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aad, G.; Abbott, B.; Abdallah, J.; Abdelalim, A. A.; Abdesselam, A.; Abdinov, O.; Abi, B.; Abolins, M.; Abramowicz, H.; Abreu, H.; et al

    2012-02-01

    Invariant mass distributions of jet pairs (dijets) produced in LHC proton–proton collisions at a centre-of-mass energy ?s = 7 TeV have been studied using a data set corresponding to an integrated luminosity of 1.0 fb?¹ recorded in 2011 by ATLAS. Dijet masses up to ~4 TeV are observed in the data, and no evidence of resonance production over background is found. Limits are set at 95% C.L. for several new physics hypotheses: excited quarks are excluded for masses below 299 TeV, axigluons are excluded for masses below 3.32 TeV, and colour octet scalar resonances are excluded for masses below 1.92more »TeV.« less

  4. Search for the Standard Model Higgs Boson in Associated WH Production in 9.7 fb?¹ of pp? Collisions with the D0 Detector

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Askew, A.; et al

    2012-09-20

    We present a search for the standard model Higgs boson in final states with a charged lepton (electron or muon), missing transverse energy, and two or three jets, at least one of which is identified as a b-quark jet. The search is primarily sensitive to WH?l?bb¯ production and uses data corresponding to 9.7 fb?¹ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron pp¯ Collider at ?s=1.96 TeV. We observe agreement between the data and the expected background. For a Higgs boson mass of 125 GeV, we set a 95% C.L. upper limit on the production ofmore »a standard model Higgs boson of 5.2×?SM, where ?SM is the standard model Higgs boson production cross section, while the expected limit is 4.7×?SM.« less

  5. Search for Diphoton Events with Large Missing Transverse Energy in 6.3 fb-1 of ppbar Collisions using the D0 Detector at the Fermilab Tevatron Collider

    SciTech Connect (OSTI)

    Cooke, Mark Stephen; /Columbia U.

    2010-09-01

    A search for diphoton events with large missing transverse energy produced in p{bar p} collisions at {radical}s = 1.96 TeV is presented. The data were collected with the D0 detector at the Fermilab Tevatron Collider between 2002 and 2010, and correspond to 6.3 fb{sup -1} of integrated luminosity. The observed missing transverse energy distribution is well described by the Standard Model prediction, and 95% C.L. limits are derived on two realizations of theories beyond the Standard Model. In a gauge mediated supersymmetry breaking scenario, the breaking scale {Lambda} is excluded for {Lambda} < 124 TeV. In a universal extra dimension model including gravitational decays, the compactification radius R{sub c} is excluded for R{sub c}{sup -1} < 477 GeV.

  6. Measurement of the CP-violating phase ?sJ/?? using the flavor-tagged decay Bs0?J/ ?? in 8 fb?¹ of pp? collisions

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; et al

    2012-02-22

    We report an updated measurement of the CP-violating phase, ?sJ/??, and the decay-width difference for the two mass eigenstates, ??s, from the flavor-tagged decay B0s?J/??. The data sample corresponds to an integrated luminosity of 8.0 fb?¹ accumulated with the D0 detector using pp? collisions at ?s=1.96 TeV produced at the Fermilab Tevatron collider. The 68% Bayesian credibility intervals, including systematic uncertainties, are ??s=0.163+0.065?0.064 ps?¹ and ?sJ/??=?0.55+0.38?0.36. The p-value for the Standard Model point is 29.8%.

  7. A search for resonant production of tt? pairs in 4.8 fb-1 of integrated luminosity of pp? collisions at ?s=1.96 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aaltonen, T.

    2011-10-27

    We search for resonant production of tt? pairs in 4.8 fb-1 integrated luminosity of pp? collision data at ?s = 1.96 TeV in the lepton+jets decay channel, where one top quark decays leptonically and the other hadronically. A matrix element reconstruction technique is used; for each event a probability density function (pdf) of the tt? candidate invariant mass is sampled. These pdfs are used to construct a likelihood function, whereby the cross section for resonant tt? production is estimated, given a hypothetical resonance mass and width. The data indicate no evidence of resonant production of tt? pairs. A benchmark modelmore »of leptophobic Z' ? tt? is excluded with mZ' « less

  8. Measurement of the WZ and ZZ production cross sections using leptonic final states in 8.6 fb?¹ of pp? collisions

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Aoki, M.; et al

    2012-06-12

    We study the processes pp??WZ?l±?l?l? and pp??ZZ?l?l???¯, where l=e or ?. Using 8.6 fb?¹ of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron collider, we measure the WZ production cross section to be 4.50+0.63–0.66 pb which is consistent with, but slightly larger than, the prediction of the standard model. The ZZ cross section is measured to be 1.64±0.46 pb, in agreement with a prediction of the standard model. Combination with an earlier analysis of the ZZ?l?l?l?l? channel yields a ZZ cross section of 1.44+0.35–0.34 pb.

  9. Search for the Standard Model Higgs Boson in Associated WH Production in 9.7 fb?¹ of pp? Collisions with the D0 Detector

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Askew, A.; Atkins, S.; Augsten, K.; Avila, C.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Buszello, C. P.; Camacho-Pérez, E.; Casey, B. C. K.; Castilla-Valdez, H.; Caughron, S.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; Das, A.; Davies, G.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Feng, L.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garcia-Bellido, A.; García-González, J. A.; García-Guerra, G. A.; Gavrilov, V.; Gay, P.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Howley, I.; Hubacek, Z.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jayasinghe, A.; Jeong, M. S.; Jesik, R.; Jiang, P.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kiselevich, I.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kulikov, S.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lei, X.; Lellouch, J.; Li, D.; Li, H.; Li, L.; Li, Q. Z.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, H.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Nguyen, H. T.; Nunnemann, T.; Orduna, J.; Osman, N.; Osta, J.; Padilla, M.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Sajot, G.; Salcido, P.; Sánchez-Hernández, A.; Sanders, M. P.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shaw, S.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Smith, K. J.; Snow, G. R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Sonnenschein, L.; Soustruznik, K.; Stark, J.; Stoyanova, D. A.; Strauss, M.; Suter, L.; Svoisky, P.; Takahashi, M.; Titov, M.; Tokmenin, V. V.; Tsai, Y.-T.; Tschann-Grimm, K.; Tsybychev, D.; Tuchming, B.; Tully, C.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; van Leeuwen, W. M.; Varelas, N.; Varnes, E. W.

    2012-09-01

    We present a search for the standard model Higgs boson in final states with a charged lepton (electron or muon), missing transverse energy, and two or three jets, at least one of which is identified as a b-quark jet. The search is primarily sensitive to WH?l?bb¯ production and uses data corresponding to 9.7 fb?¹ of integrated luminosity collected with the D0 detector at the Fermilab Tevatron pp¯ Collider at ?s=1.96 TeV. We observe agreement between the data and the expected background. For a Higgs boson mass of 125 GeV, we set a 95% C.L. upper limit on the production of a standard model Higgs boson of 5.2×?SM, where ?SM is the standard model Higgs boson production cross section, while the expected limit is 4.7×?SM.

  10. Combined CDF and D0 Upper Limits on Standard Model Higgs Boson Production with up to 8.6 fb-1 of Data

    E-Print Network [OSTI]

    The CDF; D0 Collaborations; the Tevatron New Phenomena; Higgs Working Group

    2011-09-20

    We combine results from CDF and D0 on direct searches for the standard model (SM) Higgs boson (H) in ppbar collisions at the Fermilab Tevatron at sqrt{s}=1.96 TeV. Compared to the previous Tevatron Higgs boson search combination more data have been added, additional channels have been incorporated, and some previously used channels have been reanalyzed to gain sensitivity. We use the MSTW08 parton distribution functions and the latest theoretical cross sections when comparing our limits to the SM predictions. With up to 8.2 fb-1 of data analyzed at CDF and up to 8.6 fb-1 at D0, the 95% C.L. our upper limits on Higgs boson production are factors of 1.17, 1.71, and 0.48 times the values of the SM cross section for Higgs bosons of mass m_H=115 GeV/c^2, 140 GeV/c^2, and 165 GeV/c^2, respectively. The corresponding median upper limits expected in the absence of Higgs boson production are 1.16, 1.16, and 0.57. There is a small (approx. 1 sigma) excess of data events with respect to the background estimation in searches for the Higgs boson in the mass range 125

  11. Combined CDF and D0 Upper Limits on Standard Model Higgs Boson Production with up to 8.6 fb-1 of Data

    SciTech Connect (OSTI)

    CDF, The; Collaborations, D0; Phenomena, the Tevatron New; Group, Higgs Working

    2011-07-01

    We combine results from CDF and D0 on direct searches for the standard model (SM) Higgs boson (H) in p{bar p} collisions at the Fermilab Tevatron at {radical}s = 1.96 TeV. Compared to the previous Tevatron Higgs boson search combination more data have been added, additional channels have been incorporated, and some previously used channels have been reanalyzed to gain sensitivity. We use the MSTW08 parton distribution functions and the latest theoretical cross sections when comparing our limits to the SM predictions. With up to 8.2 fb{sup -1} of data analyzed at CDF and up to 8.6 fb{sup -1} at D0, the 95% C.L. our upper limits on Higgs boson production are factors of 1.17, 1.71, and 0.48 times the values of the SM cross section for Higgs bosons of mass m{sub H} = 115 GeV/c{sup 2}, 140 GeV/c{sup 2}, and 165 GeV/c{sup 2}, respectively. The corresponding median upper limits expected in the absence of Higgs boson production are 1.16, 1.16, and 0.57. There is a small ({approx} 1{sigma}) excess of data events with respect to the background estimation in searches for the Higgs boson in the mass range 125 < m{sub H} < 155 GeV/c{sup 2}. We exclude, at the 95% C.L., a new and larger region at high mass between 156 < m{sub H} < 177 GeV/c{sup 2}, with an expected exclusion region of 148 < m{sub H} < 180 GeV/c{sup 2}.

  12. University of Southern California, USC Dornsife Office of Pre-Health Advisement, 3641 Watt Way, HNB 120, Los Angeles, CA 90089 (213) 740-4844, E-mail: prehealth@dornsife.usc.edu; Website: http://dornsife.usc.edu/pre-health; FB: www.facebook.com/USCPreHeal

    E-Print Network [OSTI]

    Zhou, Xianghong Jasmine

    ://dornsife.usc.edu/pre-health; FB: www.facebook.com/USCPreHealth The mission of the Office of Pre-Health Advisement, within the Dana

  13. Measurement of the inclusive isolated prompt photons cross section in pp collisions at ?s = 7 TeV with the ATLAS detector using 4.6 fb[superscript -1

    E-Print Network [OSTI]

    Taylor, Frank E.

    A measurement of the cross section for the production of isolated prompt photons in pp collisions at a center-of-mass energy ?s = 7??TeV is presented. The results are based on an integrated luminosity of 4.6??fb[superscript ...

  14. Search for the Production of Narrow tb-bar Resonances in 1.9 fb-1 of pp-bar Collisions at sqrt[s]=1.96 TeV

    E-Print Network [OSTI]

    Xie, Si

    We present new limits on resonant tb? production in pp? collisions at ?s=1.96??TeV, using 1.9??fb[superscript -1] of data recorded with the CDF II detector at the Fermilab Tevatron. We reconstruct a candidate tb? mass ...

  15. Search for Higgs boson production in oppositely charged dilepton and missing energy final states in 9.7??fb(?1) of pp-bar collisions at s?=1.96??TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Chen, Gemma; Clutter, Justace Randall; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Askew, A.; Atkins, S.

    2013-09-17

    We present a search for the Higgs boson in final states with two oppositely charged leptons and large missing transverse energy as expected in H?WW??????? decays. The events are selected from the full Run II data sample of 9.7??fb(?1) of pp...

  16. Search for a Higgs boson in diphoton final states with the D0 detector in 9.6??fb(?1) of pp-bar collisions at s?=1.96??TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Chen, G.; Clutter, Justace Randall; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Askew, A.; Atkins, S.

    2013-09-17

    We present a search for a Higgs boson decaying into a pair of photons based on 9.6??fb(?1) of pp-bar collisions at s?=1.96??TeV collected with the D0 detector at the Fermilab Tevatron Collider. The search employs multivariate techniques...

  17. Search for diphoton events with large missing transverse momentum in 1 fb[superscript -1] of 7 TeV proton–proton collision data with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb[superscript ?1] of proton–proton collision data at ?s = 7 TeV recorded with the ATLAS detector. No excess of events was ...

  18. Search for t[¯ over t] resonances in the lepton plus jets final state with ATLAS using 4.7??fb[superscript -1] of pp collisions at ?s=7??TeV

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for new particles that decay into top quark pairs (tt? ) is performed with the ATLAS experiment at the LHC using an integrated luminosity of 4.7??fb[superscript -1] of proton–proton (pp) collision data collected ...

  19. Search for diphoton events with large missing transverse momentum in 1 fb?¹ of 7 TeV proton–proton collision data with the ATLAS detector

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aad, G.; Abbott, B.; Abdallah, J.; Abdelalim, A.A.; Abdesselam, A.; Abdinov, O.; Abi, B.; Abolins, M.; Abramowicz, H.; Abreu, H.; et al

    2012-04-01

    A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb?¹ of proton–proton collision data at ?s = 7 TeV recorded with the ATLAS detector. No excess of events was observed above the Standard Model prediction and 95% Confidence Level (CL) upper limits are set on the production cross section for new physics. The limits depend on each model parameter space and vary as follows: ? in the context of a generalised model of gauge-mediated supersymmetry breaking (GGM) with a bino-like lightest neutralino, ? in the context of a minimal model of gauge-mediatedmore »supersymmetry breaking (SPS8), and ? in the context of a specific model with one universal extra dimension (UED). A 95% CL lower limit of 805 GeV, for bino masses above 50 GeV, is set on the GGM gluino mass. Lower limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking scale ? and on the UED compactification scale 1/R, respectively. These limits provide the most stringent tests of these models to date.« less

  20. Search for vector-like quark production in the lepton+jets and dilepton+jets final states using 5.4 fb-1 of Run II data

    SciTech Connect (OSTI)

    Caughron, Seth; /Columbia U.

    2010-10-01

    The Standard Model of particle physics provides an excellent description of particle interactions at energies up to {approx}1 TeV, but it is expected to fail above that scale. Multiple models developed to describe phenomena above the TeV scale predict the existence of very massive, vector-like quarks. A search for single electroweak production of such particles in p{anti p} collisions at a center-of-mass energy of 1.96 TeV is performed in the W+jets and Z+jets channels. The data were collected by the D0 detector at the Fermilab Tevatron Collider and correspond to an integrated luminosity of 5.4 fb{sup -1}. Events consistent with a heavy object decaying to a vector boson and a jet are selected. We observe no significant excess in comparison to the background prediction and set 95% confidence level upper limits on production cross sections for vector-like quarks decaying to W+jet and Z+jet. Assuming a vector-like quark -- standard model quark coupling parameter {tilde {kappa}}{sub qQ} of unity, we exclude vector-like quarks with mass below 693 GeV for decays to W+jet and mass below 449 GeV for decays to Z+jet. These represent the most sensitive limits to date.

  1. Search for tt¯ resonances in the lepton plus jets final state with ATLAS using 4.7 fb?¹ of pp collisions at ?s=7 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aad, G.; Abajyan, T.; Abbott, B.; Abdallah, J.; Abdel Khalek, S.; Abdelalim, A. A.; Abdinov, O.; Aben, R.; Abi, B.; Abolins, M.; AbouZeid, O. S.; Abramowicz, H.; Abreu, H.; Abulaiti, Y.; Acharya, B. S.; Adamczyk, L.; Adams, D. L.; Addy, T. N.; Adelman, J.; Adomeit, S.; Adragna, P.; Adye, T.; Aefsky, S.; Aguilar-Saavedra, J. A.; Agustoni, M.; Ahlen, S. P.; Ahles, F.; Ahmad, A.; Ahsan, M.; Aielli, G.; Åkesson, T. P. A.; Akimoto, G.; Akimov, A. V.; Alam, M. A.; Albert, J.; Albrand, S.; Aleksa, M.; Aleksandrov, I. N.; Alessandria, F.; Alexa, C.; Alexander, G.; Alexandre, G.; Alexopoulos, T.; Alhroob, M.; Aliev, M.; Alimonti, G.; Alison, J.; Allbrooke, B. M. M.; Allison, L. J.; Allport, P. P.; Allwood-Spiers, S. E.; Almond, J.; Aloisio, A.; Alon, R.; Alonso, A.; Alonso, F.; Altheimer, A.; Alvarez Gonzalez, B.; Alviggi, M. G.; Amako, K.; Amelung, C.; Ammosov, V. V.; Amor Dos Santos, S. P.; Amorim, A.; Amoroso, S.; Amram, N.; Anastopoulos, C.; Ancu, L. S.; Andari, N.; Andeen, T.; Anders, C. F.; Anders, G.; Anderson, K. J.; Andreazza, A.; Andrei, V.; Anduaga, X. S.; Angelidakis, S.; Anger, P.; Angerami, A.; Anghinolfi, F.; Anisenkov, A.; Anjos, N.; Annovi, A.; Antonaki, A.; Antonelli, M.; Antonov, A.; Antos, J.; Anulli, F.; Aoki, M.; Aperio Bella, L.; Apolle, R.; Arabidze, G.; Aracena, I.; Arai, Y.; Arce, A. T. H.; Arfaoui, S.; Arguin, J-F.; Argyropoulos, S.; Arik, E.; Arik, M.; Armbruster, A. J.; Arnaez, O.; Arnal, V.; Artamonov, A.; Artoni, G.; Arutinov, D.; Asai, S.; Ask, S.; Åsman, B.; Asquith, L.; Assamagan, K.; Astalos, R.; Astbury, A.; Atkinson, M.; Auerbach, B.; Auge, E.; Augsten, K.; Aurousseau, M.; Avolio, G.; Axen, D.; Azuelos, G.; Azuma, Y.; Baak, M. A.; Baccaglioni, G.; Bacci, C.; Bach, A. M.; Bachacou, H.; Bachas, K.; Backes, M.; Backhaus, M.; Backus Mayes, J.; Badescu, E.; Bagnaia, P.; Bai, Y.; Bailey, D. C.; Bain, T.; Baines, J. T.; Baker, O. K.; Baker, S.; Balek, P.; Balli, F.; Banas, E.; Banerjee, P.; Banerjee, Sw.; Banfi, D.; Bangert, A.; Bansal, V.; Bansil, H. S.; Barak, L.; Baranov, S. P.; Barber, T.; Barberio, E. L.; Barberis, D.; Barbero, M.; Bardin, D. Y.; Barillari, T.; Barisonzi, M.; Barklow, T.; Barlow, N.; Barnett, B. M.; Barnett, R. M.; Baroncelli, A.; Barone, G.; Barr, A. J.; Barreiro, F.; Barreiro Guimarães da Costa, J.; Bartoldus, R.; Barton, A. E.; Bartsch, V.; Basye, A.; Bates, R. L.; Batkova, L.; Batley, J. R.; Battaglia, A.; Battistin, M.; Bauer, F.; Bawa, H. S.; Beale, S.; Beau, T.; Beauchemin, P. H.; Beccherle, R.; Bechtle, P.; Beck, H. P.; Becker, K.; Becker, S.; Beckingham, M.; Becks, K. H.; Beddall, A. J.; Beddall, A.; Bedikian, S.; Bednyakov, V. A.; Bee, C. P.; Beemster, L. J.; Beermann, T. A.; Begel, M.; Behar Harpaz, S.; Belanger-Champagne, C.; Bell, P. J.; Bell, W. H.; Bella, G.; Bellagamba, L.; Bellomo, M.; Belloni, A.; Beloborodova, O.; Belotskiy, K.; Beltramello, O.; Benary, O.; Benchekroun, D.; Bendtz, K.; Benekos, N.; Benhammou, Y.; Benhar Noccioli, E.; Benitez Garcia, J. A.; Benjamin, D. P.; Benoit, M.; Bensinger, J. R.; Benslama, K.; Bentvelsen, S.; Berge, D.; Bergeaas Kuutmann, E.; Berger, N.; Berghaus, F.; Berglund, E.; Beringer, J.; Bernat, P.; Bernhard, R.; Bernius, C.; Bernlochner, F. U.; Berry, T.; Bertella, C.; Bertin, A.; Bertolucci, F.; Besana, M. I.; Besjes, G. J.; Besson, N.; Bethke, S.; Bhimji, W.; Bianchi, R. M.; Bianchini, L.; Bianco, M.; Biebel, O.; Bieniek, S. P.; Bierwagen, K.; Biesiada, J.; Biglietti, M.; Bilokon, H.; Bindi, M.; Binet, S.; Bingul, A.; Bini, C.; Biscarat, C.; Bittner, B.; Black, C. W.; Black, J. E.; Black, K. M.; Blair, R. E.; Blanchard, J.-B.; Blazek, T.; Bloch, I.; Blocker, C.; Blocki, J.; Blum, W.; Blumenschein, U.; Bobbink, G. J.; Bobrovnikov, V. S.; Bocchetta, S. S.; Bocci, A.; Boddy, C. R.; Boehler, M.; Boek, J.; Boek, T. T.; Boelaert, N.; Bogaerts, J. A.; Bogdanchikov, A.; Bogouch, A.; Bohm, C.; Bohm, J.; Boisvert, V.; Bold, T.; Boldea, V.; Bolnet, N. M.; Bomben, M.; Bona, M.; Boonekamp, M.; Bordoni, S.; Borer, C.; Borisov, A.; Borissov, G.; Borjanovic, I.; Borri, M.; Borroni, S.; Bortfeldt, J.; Bortolotto, V.; Bos, K.; Boscherini, D.; Bosman, M.; Boterenbrood, H.; Bouchami, J.; Boudreau, J.; Bouhova-Thacker, E. V.; Boumediene, D.; Bourdarios, C.; Bousson, N.; Boutouil, S.; Boveia, A.; Boyd, J.; Boyko, I. R.; Bozovic-Jelisavcic, I.; Bracinik, J.; Branchini, P.; Brandt, A.; Brandt, G.; Brandt, O.; Bratzler, U.; Brau, B.; Brau, J. E.; Braun, H. M.; Brazzale, S. F.; Brelier, B.; Bremer, J.; Brendlinger, K.; Brenner, R.; Bressler, S.; Bristow, T. M.; Britton, D.; Brochu, F. M.; Brock, I.; Brock, R.; Broggi, F.; Bromberg, C.; Bronner, J.; Brooijmans, G.; Brooks, T.; Brooks, W. K.; Brown, G.; Bruckman de Renstrom, P. A.; Bruncko, D.; Bruneliere, R.; Brunet, S.; Bruni, A.; Bruni, G.; Bruschi, M.; Bryngemark, L.

    2013-07-01

    A search for new particles that decay into top quark pairs (tt¯) is performed with the ATLAS experiment at the LHC using an integrated luminosity of 4.7 fb?¹ of proton–proton (pp ) collision data collected at a center-of-mass energy ?s =7 TeV . In the tt¯ ?WbWb decay, the lepton plus jets final state is used, where one W boson decays leptonically and the other hadronically. The tt¯ system is reconstructed using both small-radius and large-radius jets, the latter being supplemented by a jet substructure analysis. A search for local excesses in the number of data events compared to the Standard Model expectation in the tt¯ invariant mass spectrum is performed. No evidence for a tt¯ resonance is found and 95% credibility-level limits on the production rate are determined for massive states predicted in two benchmark models. The upper limits on the cross section times branching ratio of a narrow Z' resonance range from 5.1 pb for a boson mass of 0.5 TeV to 0.03 pb for a mass of 3 TeV. A narrow leptophobic topcolor Z' resonance with a mass below 1.74 TeV is excluded. Limits are also derived for a broad color-octet resonance with ?/m=15.3% . A Kaluza–Klein excitation of the gluon in a Randall–Sundrum model is excluded for masses below 2.07 TeV.

  2. y12 disc 1954 FB

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLosThe 26thI D- 6 0 4 2 r mReducingwhistleblowerxinyufu Ames25

  3. Search for the standard model Higgs boson produced in association with a W± boson with 7.5 fb?¹ integrated luminosity at CDF

    SciTech Connect (OSTI)

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; Artikov, A.; Asaadi, J.; Ashmanskas, W.; Auerbach, B.; Aurisano, A.; Azfar, F.; Badgett, W.; Bae, T.; Barbaro-Galtieri, A.; Barnes, V. E.; Barnett, B. A.; Barria, P.; Bartos, P.; Bauce, M.; Bedeschi, F.; Behari, S.; Bellettini, G.; Bellinger, J.; Benjamin, D.; Beretvas, A.; Bhatti, A.; Bisello, D.; Bizjak, I.; Bland, K. R.; Blumenfeld, B.; Bocci, A.; Bodek, A.; Bortoletto, D.; Boudreau, J.; Boveia, A.; Brigliadori, L.; Bromberg, C.; Brucken, E.; Budagov, J.; Budd, H. S.; Burkett, K.; Busetto, G.; Bussey, P.; Buzatu, A.; Calamba, A.; Calancha, C.; Camarda, S.; Campanelli, M.; Campbell, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Carron, S.; Casal, B.; Casarsa, M.; Castro, A.; Catastini, P.; Cauz, D.; Cavaliere, V.; Cavalli-Sforza, M.; Cerri, A.; Cerrito, L.; Chen, Y. C.; Chertok, M.; Chiarelli, G.; Chlachidze, G.; Chlebana, F.; Cho, K.; Chokheli, D.; Chung, W. H.; Chung, Y. S.; Ciocci, M. A.; Clark, A.; Clarke, C.; Compostella, G.; Convery, M. E.; Conway, J.; Corbo, M.; Cordelli, M.; Cox, C. A.; Cox, D. J.; Crescioli, F.; Cuevas, J.; Culbertson, R.; Dagenhart, D.; d’Ascenzo, N.; Datta, M.; de Barbaro, P.; Dell’Orso, M.; Demortier, L.; Deninno, M.; Devoto, F.; d’Errico, M.; Di Canto, A.; Di Ruzza, B.; Dittmann, J. R.; D’Onofrio, M.; Donati, S.; Dong, P.; Dorigo, M.; Dorigo, T.; Ebina, K.; Elagin, A.; Eppig, A.; Erbacher, R.; Errede, S.; Ershaidat, N.; Eusebi, R.; Farrington, S.; Feindt, M.; Fernandez, J. P.; Field, R.; Flanagan, G.; Forrest, R.; Frank, M. J.; Franklin, M.; Freeman, J. C.; Funakoshi, Y.; Furic, I.; Gallinaro, M.; Garcia, J. E.; Garfinkel, A. F.; Garosi, P.; Gerberich, H.; Gerchtein, E.; Giagu, S.; Giakoumopoulou, V.; Giannetti, P.; Gibson, K.; Ginsburg, C. M.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Goldschmidt, N.; Golossanov, A.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; González, O.; Gorelov, I.; Goshaw, A. T.; Goulianos, K.; Grinstein, S.; Grosso-Pilcher, C.; Group, R. C.; Guimaraes da Costa, J.; Hahn, S. R.; Halkiadakis, E.; Hamaguchi, A.; Han, J. Y.; Happacher, F.; Hara, K.; Hare, D.; Hare, M.; Harr, R. F.; Hatakeyama, K.; Hays, C.; Heck, M.; Heinrich, J.; Herndon, M.; Hewamanage, S.; Hocker, A.; Hopkins, W.; Horn, D.; Hou, S.; Hughes, R. E.; Hurwitz, M.; Husemann, U.; Hussain, N.; Hussein, M.; Huston, J.; Introzzi, G.; Iori, M.; Ivanov, A.; James, E.; Jang, D.; Jayatilaka, B.; Jeon, E. J.; Jindariani, S.; Jones, M.; Joo, K. K.; Jun, S. Y.; Junk, T. R.; Kamon, T.; Karchin, P. E.; Kasmi, A.; Kato, Y.; Ketchum, W.; Keung, J.; Khotilovich, V.; Kilminster, B.; Kim, D. H.; Kim, H. S.; Kim, J. E.; Kim, M. J.; Kim, S. B.; Kim, S. H.; Kim, Y. K.; Kim, Y. J.; Kimura, N.; Kirby, M.; Klimenko, S.; Knoepfel, K.; Kondo, K.; Kong, D. J.; Konigsberg, J.; Kotwal, A. V.; Kreps, M.; Kroll, J.; Krop, D.; Kruse, M.; Krutelyov, V.; Kuhr, T.; Kurata, M.; Kwang, S.; Laasanen, A. T.; Lami, S.; Lammel, S.; Lancaster, M.; Lander, R. L.; Lannon, K.; Lath, A.; Latino, G.; LeCompte, T.; Lee, E.; Lee, H. S.; Lee, J. S.; Lee, S. W.; Leo, S.; Leone, S.; Lewis, J. D.; Limosani, A.; Lin, C.-J.; Lindgren, M.; Lipeles, E.; Lister, A.; Litvintsev, D. O.; Liu, C.; Liu, H.; Liu, Q.; Liu, T.; Lockwitz, S.; Loginov, A.; Lucchesi, D.; Lueck, J.; Lujan, P.; Lukens, P.; Lungu, G.; Lys, J.; Lysak, R.; Madrak, R.; Maeshima, K.; Maestro, P.; Malik, S.; Manca, G.; Manousakis-Katsikakis, A.; Margaroli, F.; Marino, C.; Martínez, M.; Mastrandrea, P.; Matera, K.; Mattson, M. E.; Mazzacane, A.; Mazzanti, P.; McFarland, K. S.; McIntyre, P.; McNulty, R.; Mehta, A.; Mehtala, P.; Mesropian, C.; Miao, T.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondragon, M. N.; Moon, C. S.; Moore, R.; Morello, M. J.; Morlock, J.; Movilla Fernandez, P.; Mukherjee, A.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nakano, I.; Napier, A.; Nett, J.; Neu, C.; Neubauer, M. S.; Nielsen, J.; Nodulman, L.; Noh, S. Y.; Norniella, O.; Oakes, L.; Oh, S. H.; Oh, Y. D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Ortolan, L.; Pagan Griso, S.; Pagliarone, C.; Palencia, E.; Papadimitriou, V.; Paramonov, A. A.; Patrick, J.; Pauletta, G.; Paulini, M.; Paus, C.; Pellett, D. E.; Penzo, A.; Phillips, T. J.; Piacentino, G.; Pianori, E.; Pilot, J.; Pitts, K.; Plager, C.; Pondrom, L.; Poprocki, S.; Potamianos, K.; Prokoshin, F.; Pranko, A.; Ptohos, F.; Punzi, G.; Rahaman, A.; Ramakrishnan, V.; Ranjan, N.; Redondo, I.; Renton, P.; Rescigno, M.; Riddick, T.; Rimondi, F.; Ristori, L.; Robson, A.; Rodrigo, T.; Rodriguez, T.; Rogers, E.; Rolli, S.; Roser, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Safonov, A.; Sakumoto, W. K.

    2012-08-01

    We present a search for the standard model Higgs boson produced in association with a W± boson. This search uses data corresponding to an integrated luminosity of 7.5 fb?¹ collected by the CDF detector at the Tevatron. We select WH?l?bb¯ candidate events with two jets, large missing transverse energy, and exactly one charged lepton. We further require that at least one jet be identified to originate from a bottom quark. Discrimination between the signal and the large background is achieved through the use of a Bayesian artificial neural network. The number of tagged events and their distributions are consistent with the standard model expectations. We observe no evidence for a Higgs boson signal and set 95% C.L. upper limits on the WH production cross section times the branching ratio to decay to bb¯ pairs, ?(pp¯?W±H)×B(H?bb¯), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c² we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c² the upper limit is 3.64 (2.78). The combination of the present search with an independent analysis that selects events with three jets yields more stringent limits ranging from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For 115 and 125 GeV/c² the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.

  4. Search for the standard model Higgs boson produced in association with a W± boson with 7.5 fb?¹ integrated luminosity at CDF

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; et al

    2012-08-01

    We present a search for the standard model Higgs boson produced in association with a W± boson. This search uses data corresponding to an integrated luminosity of 7.5 fb?¹ collected by the CDF detector at the Tevatron. We select WH?l?bb¯ candidate events with two jets, large missing transverse energy, and exactly one charged lepton. We further require that at least one jet be identified to originate from a bottom quark. Discrimination between the signal and the large background is achieved through the use of a Bayesian artificial neural network. The number of tagged events and their distributions are consistent withmore »the standard model expectations. We observe no evidence for a Higgs boson signal and set 95% C.L. upper limits on the WH production cross section times the branching ratio to decay to bb¯ pairs, ?(pp¯?W±H)×B(H?bb¯), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c² we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c² the upper limit is 3.64 (2.78). The combination of the present search with an independent analysis that selects events with three jets yields more stringent limits ranging from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For 115 and 125 GeV/c² the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.« less

  5. Search for tt¯ resonances in the lepton plus jets final state with ATLAS using 4.7 fb?¹ of pp collisions at ?s=7 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aad, G.; Abajyan, T.; Abbott, B.; Abdallah, J.; Abdel Khalek, S.; Abdelalim, A. A.; Abdinov, O.; Aben, R.; Abi, B.; Abolins, M.; et al

    2013-07-23

    A search for new particles that decay into top quark pairs (tt¯) is performed with the ATLAS experiment at the LHC using an integrated luminosity of 4.7 fb?¹ of proton–proton (pp ) collision data collected at a center-of-mass energy ?s =7 TeV . In the tt¯ ?WbWb decay, the lepton plus jets final state is used, where one W boson decays leptonically and the other hadronically. The tt¯ system is reconstructed using both small-radius and large-radius jets, the latter being supplemented by a jet substructure analysis. A search for local excesses in the number of data events compared to themore »Standard Model expectation in the tt¯ invariant mass spectrum is performed. No evidence for a tt¯ resonance is found and 95% credibility-level limits on the production rate are determined for massive states predicted in two benchmark models. The upper limits on the cross section times branching ratio of a narrow Z' resonance range from 5.1 pb for a boson mass of 0.5 TeV to 0.03 pb for a mass of 3 TeV. A narrow leptophobic topcolor Z' resonance with a mass below 1.74 TeV is excluded. Limits are also derived for a broad color-octet resonance with ?/m=15.3% . A Kaluza–Klein excitation of the gluon in a Randall–Sundrum model is excluded for masses below 2.07 TeV.« less

  6. Search for the standard model Higgs boson produced in association with a W± boson with 7.5 fb?¹ integrated luminosity at CDF

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; Artikov, A.; Asaadi, J.; Ashmanskas, W.; Auerbach, B.; Aurisano, A.; Azfar, F.; Badgett, W.; Bae, T.; Barbaro-Galtieri, A.; Barnes, V. E.; Barnett, B. A.; Barria, P.; Bartos, P.; Bauce, M.; Bedeschi, F.; Behari, S.; Bellettini, G.; Bellinger, J.; Benjamin, D.; Beretvas, A.; Bhatti, A.; Bisello, D.; Bizjak, I.; Bland, K. R.; Blumenfeld, B.; Bocci, A.; Bodek, A.; Bortoletto, D.; Boudreau, J.; Boveia, A.; Brigliadori, L.; Bromberg, C.; Brucken, E.; Budagov, J.; Budd, H. S.; Burkett, K.; Busetto, G.; Bussey, P.; Buzatu, A.; Calamba, A.; Calancha, C.; Camarda, S.; Campanelli, M.; Campbell, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Carron, S.; Casal, B.; Casarsa, M.; Castro, A.; Catastini, P.; Cauz, D.; Cavaliere, V.; Cavalli-Sforza, M.; Cerri, A.; Cerrito, L.; Chen, Y. C.; Chertok, M.; Chiarelli, G.; Chlachidze, G.; Chlebana, F.; Cho, K.; Chokheli, D.; Chung, W. H.; Chung, Y. S.; Ciocci, M. A.; Clark, A.; Clarke, C.; Compostella, G.; Convery, M. E.; Conway, J.; Corbo, M.; Cordelli, M.; Cox, C. A.; Cox, D. J.; Crescioli, F.; Cuevas, J.; Culbertson, R.; Dagenhart, D.; d’Ascenzo, N.; Datta, M.; de Barbaro, P.; Dell’Orso, M.; Demortier, L.; Deninno, M.; Devoto, F.; d’Errico, M.; Di Canto, A.; Di Ruzza, B.; Dittmann, J. R.; D’Onofrio, M.; Donati, S.; Dong, P.; Dorigo, M.; Dorigo, T.; Ebina, K.; Elagin, A.; Eppig, A.; Erbacher, R.; Errede, S.; Ershaidat, N.; Eusebi, R.; Farrington, S.; Feindt, M.; Fernandez, J. P.; Field, R.; Flanagan, G.; Forrest, R.; Frank, M. J.; Franklin, M.; Freeman, J. C.; Funakoshi, Y.; Furic, I.; Gallinaro, M.; Garcia, J. E.; Garfinkel, A. F.; Garosi, P.; Gerberich, H.; Gerchtein, E.; Giagu, S.; Giakoumopoulou, V.; Giannetti, P.; Gibson, K.; Ginsburg, C. M.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Goldschmidt, N.; Golossanov, A.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; González, O.; Gorelov, I.; Goshaw, A. T.; Goulianos, K.; Grinstein, S.; Grosso-Pilcher, C.; Group, R. C.; Guimaraes da Costa, J.; Hahn, S. R.; Halkiadakis, E.; Hamaguchi, A.; Han, J. Y.; Happacher, F.; Hara, K.; Hare, D.; Hare, M.; Harr, R. F.; Hatakeyama, K.; Hays, C.; Heck, M.; Heinrich, J.; Herndon, M.; Hewamanage, S.; Hocker, A.; Hopkins, W.; Horn, D.; Hou, S.; Hughes, R. E.; Hurwitz, M.; Husemann, U.; Hussain, N.; Hussein, M.; Huston, J.; Introzzi, G.; Iori, M.; Ivanov, A.; James, E.; Jang, D.; Jayatilaka, B.; Jeon, E. J.; Jindariani, S.; Jones, M.; Joo, K. K.; Jun, S. Y.; Junk, T. R.; Kamon, T.; Karchin, P. E.; Kasmi, A.; Kato, Y.; Ketchum, W.; Keung, J.; Khotilovich, V.; Kilminster, B.; Kim, D. H.; Kim, H. S.; Kim, J. E.; Kim, M. J.; Kim, S. B.; Kim, S. H.; Kim, Y. K.; Kim, Y. J.; Kimura, N.; Kirby, M.; Klimenko, S.; Knoepfel, K.; Kondo, K.; Kong, D. J.; Konigsberg, J.; Kotwal, A. V.; Kreps, M.; Kroll, J.; Krop, D.; Kruse, M.; Krutelyov, V.; Kuhr, T.; Kurata, M.; Kwang, S.; Laasanen, A. T.; Lami, S.; Lammel, S.; Lancaster, M.; Lander, R. L.; Lannon, K.; Lath, A.; Latino, G.; LeCompte, T.; Lee, E.; Lee, H. S.; Lee, J. S.; Lee, S. W.; Leo, S.; Leone, S.; Lewis, J. D.; Limosani, A.; Lin, C.-J.; Lindgren, M.; Lipeles, E.; Lister, A.; Litvintsev, D. O.; Liu, C.; Liu, H.; Liu, Q.; Liu, T.; Lockwitz, S.; Loginov, A.; Lucchesi, D.; Lueck, J.; Lujan, P.; Lukens, P.; Lungu, G.; Lys, J.; Lysak, R.; Madrak, R.; Maeshima, K.; Maestro, P.; Malik, S.; Manca, G.; Manousakis-Katsikakis, A.; Margaroli, F.; Marino, C.; Martínez, M.; Mastrandrea, P.; Matera, K.; Mattson, M. E.; Mazzacane, A.; Mazzanti, P.; McFarland, K. S.; McIntyre, P.; McNulty, R.; Mehta, A.; Mehtala, P.; Mesropian, C.; Miao, T.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondragon, M. N.; Moon, C. S.; Moore, R.; Morello, M. J.; Morlock, J.; Movilla Fernandez, P.; Mukherjee, A.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nakano, I.; Napier, A.; Nett, J.; Neu, C.; Neubauer, M. S.; Nielsen, J.; Nodulman, L.; Noh, S. Y.; Norniella, O.; Oakes, L.; Oh, S. H.; Oh, Y. D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Ortolan, L.; Pagan Griso, S.; Pagliarone, C.; Palencia, E.; Papadimitriou, V.; Paramonov, A. A.; Patrick, J.; Pauletta, G.; Paulini, M.; Paus, C.; Pellett, D. E.; Penzo, A.; Phillips, T. J.; Piacentino, G.; Pianori, E.; Pilot, J.; Pitts, K.; Plager, C.; Pondrom, L.; Poprocki, S.; Potamianos, K.; Prokoshin, F.; Pranko, A.; Ptohos, F.; Punzi, G.; Rahaman, A.; Ramakrishnan, V.; Ranjan, N.; Redondo, I.; Renton, P.; Rescigno, M.; Riddick, T.; Rimondi, F.; Ristori, L.; Robson, A.; Rodrigo, T.; Rodriguez, T.; Rogers, E.; Rolli, S.; Roser, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Safonov, A.; Sakumoto, W. K.

    2012-08-01

    We present a search for the standard model Higgs boson produced in association with a W± boson. This search uses data corresponding to an integrated luminosity of 7.5 fb?¹ collected by the CDF detector at the Tevatron. We select WH?l?bb¯ candidate events with two jets, large missing transverse energy, and exactly one charged lepton. We further require that at least one jet be identified to originate from a bottom quark. Discrimination between the signal and the large background is achieved through the use of a Bayesian artificial neural network. The number of tagged events and their distributions are consistent with the standard model expectations. We observe no evidence for a Higgs boson signal and set 95% C.L. upper limits on the WH production cross section times the branching ratio to decay to bb¯ pairs, ?(pp¯?W±H)×B(H?bb¯), relative to the rate predicted by the standard model. For the Higgs boson mass range of 100 to 150 GeV/c² we set observed (expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For 115 GeV/c² the upper limit is 3.64 (2.78). The combination of the present search with an independent analysis that selects events with three jets yields more stringent limits ranging from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For 115 and 125 GeV/c² the upper limits are 2.65 (2.60) and 4.36 (3.69), respectively.

  7. Time to pull out. And not just from Iraq. -Print Version -International Herald Tribune http://www.iht.com/bin/print_ipub.php?file=/articles/2005/07/15/opinion/eddeutch.php

    E-Print Network [OSTI]

    Deutch, John

    Time to pull out. And not just from Iraq. - Print Version - International Herald Tribune http://www.iht.com/bin/print_ipub.php?file=/articles/2005/07/15/opinion/eddeutch.php Time to pull out. And not just from Iraq. John Deutch The New York. This is true whether we are acting alone, as is largely the case in Iraq, or as part of an international

  8. Search for the standard model Higgs boson in $\\bm{\\ell?}$+jets final states in 9.7~fb$\\bm{^{-1}}$ of $\\bm{p\\bar{p}}$ collisions with the D0 detector

    E-Print Network [OSTI]

    D0 Collaboration

    2013-01-25

    We present, in detail, a search for the standard model Higgs boson, $H$, in final states with a charged lepton (electron or muon), missing energy, and two or more jets in data corresponding to 9.7 fb$^{-1}$ of integrated luminosity collected at a center of mass energy of $\\sqrt{s}$ = 1.96 TeV with the D0 detector at the Fermilab Tevatron $p\\bar{p}$ Collider. The search uses $b$-jet identification to categorize events for improved signal versus background separation and is sensitive to associated production of the $H$ with a $W$ boson, $WH\\to\\ell\

  9. Search for a heavy gauge boson decaying to a charged lepton and a neutrino in 1 fb-1 of pp collisions at ?s=7 TeV using the ATLAS detector

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aad, G.

    2011-11-01

    The ATLAS detector at the LHC is used to search for heavy charged gauge bosons (W'), decaying to a charged lepton (electron or muon) and a neutrino. Results are presented based on the analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 1.04 fb?¹. No excess beyond Standard Model expectations is observed. A W' with Sequential Standard Model couplings is excluded at the 95% confidence level for masses up to 2.15 TeV.

  10. Combined search for the Standard Model Higgs boson using up to 4.9 fb?¹ of pp collision data at ?s = 7 TeV with the ATLAS detector at the LHC

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aad, G.; Abbott, B.; Abdallah, J.; Abdel Khalek, S.; Abdelalim, A. A.; Abdesselam, A.; Abdinov, O.; Abi, B.; Abolins, M.; AbouZeid, O. S.; et al

    2012-03-01

    A combined search for the Standard Model Higgs boson with the ATLAS experiment at the LHC using datasets corresponding to integrated luminosities from 1.04 fb?¹ to 4.9 fb?¹ of pp collisions collected at ?s=7 TeV is presented. The Higgs boson mass ranges 112.9–115.5 GeV, 131–238 GeV and 251–466 GeV are excluded at the 95% confidence level (CL), while the range 124–519 GeV is expected to be excluded in the absence of a signal. An excess of events is observed around mH~126 GeV with a local significance of 3.5 standard deviations (? ). The local significances of H ? ??, Hmore »? ZZ(?) ? ?????????? and H ? WW(?) ? ???????¯, the three most sensitive channels in this mass range, are 2.8?, 2.1? and 1.4?, respectively. The global probability for the background to produce such a fluctuation anywhere in the explored Higgs boson mass range 110–600 GeV is estimated to be ~1.4% or, equivalently, 2.2?.« less

  11. Combined search for the Standard Model Higgs boson using up to 4.9 fb(-1) of pp collision data at root s=7 TeV with the ATLAS detector at the LHC

    SciTech Connect (OSTI)

    Aad G.; Abbott, B; Abdallah, J; Khalek, SA; Abdelalim, AA; Abdesselam, A; Abdinov, O; Abi, B; Abolins, M; AbouZeid, OS; Abramowicz, H; Abreu, H; Acerbia, E; Acharya, BS; Adamczyk, L; Adams, DL; Addy, TN; Adelman, J; Aderholz, M; Adomeit, S; Adragna, P; Ad

    2012-03-29

    A combined search for the Standard Model Higgs boson with the ATLAS experiment at the LHC using datasets corresponding to integrated luminosities from 1.04 fb{sup -1} to 4.9 fb{sup -1} of pp collisions collected at {radical}s = 7 TeV is presented. The Higgs boson mass ranges 112.9-115.5 GeV, 131-238 GeV and 251-466 GeV are excluded at the 95% confidence level (CL), while the range 124-519 GeV is expected to be excluded in the absence of a signal. An excess of events is observed around m{sub H} {approx} 126 GeV with a local significance of 3.5 standard deviations ({sigma}). The local significances of H {yields} {gamma}{gamma}, H {yields} ZZ{sup (*)} {yields} {ell}{sup +}{ell}{sup -}{ell}{prime}{sup +}{ell}{prime}{sup -} and H {yields} WW{sup (*)} {yields} {ell}{sup +}{nu}{ell}{prime}{sup -}{bar {nu}}, the three most sensitive channels in this mass range, are 2.8{sigma}, 2.1{sigma} and 1.4{sigma}, respectively. The global probability for the background to produce such a fluctuation anywhere in the explored Higgs boson mass range 110-600 GeV is estimated to be {approx}1.4% or, equivalently, 2.2{sigma}.

  12. Search for the Standard Model Higgs Boson in ZH?l?l?bb? Production with the D0 Detector in 9.7 fb?¹ of pp? Collisions at ?s=1.96 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Askew, A.; et al

    2012-09-20

    We present a search for the standard model (SM) Higgs boson produced in association with a Z boson in 9.7 fb?¹ of pp? collisions collected with the D0 detector at the Fermilab Tevatron Collider at ?s=1.96 TeV. Selected events contain one reconstructed Z?e?e? or Z????? candidate and at least two jets, including at least one jet identified as likely to contain a b quark. To validate the search procedure, we also measure the cross section for ZZ production in the same final state. It is found to be consistent with its SM prediction. We set upper limits on the ZHmore »production cross section times branching ratio for H?bb? at the 95% C.L. for Higgs boson masses 90?MH?150 GeV. The observed (expected) limit for MH=125 GeV is 7.1 (5.1) times the SM cross section.« less

  13. Measurement of the CP-violating phase ?sJ/?? using the flavor-tagged decay Bs0?J/ ?? in 8 fb?¹ of pp? collisions

    SciTech Connect (OSTI)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Alves, G. A.; Aoki, M.; Arov, M.; Askew, A.; Åsman, B.; Atkins, S.; Atramentov, O.; Augsten, K.; Avila, C.; BackusMayes, J.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Barreto, J.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Begel, M.; Belanger-Champagne, C.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bezzubov, V. A.; Bhat, P. C.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Brooijmans, G.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Burnett, T. H.; Buszello, C. P.; Calpas, B.; Camacho-Pérez, E.; Carrasco-Lizarraga, M. A.; Casey, B. C. K.; Castilla-Valdez, H.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; Das, A.; Davies, G.; De, K.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demarteau, M.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dorland, T.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garcia-Bellido, A.; García-Guerra, G. A.; Gavrilov, V.; Gay, P.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Greenwood, Z. D.; Gregores, E. M.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Haas, A.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hohlfeld, M.; Hubacek, Z.; Huske, N.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jamin, D.; Jayasinghe, A.; Jesik, R.; Johns, K.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kulikov, S.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Kvita, J.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lellouch, J.; Li, L.; Li, Q. Z.; Lietti, S. M.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Mackin, D.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Muanza, G. S.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Novaes, S. F.; Nunnemann, T.; Obrant, G.; Orduna, J.; Osman, N.; Osta, J.; Otero y Garzón, G. J.; Padilla, M.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Parsons, J.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, K.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Piegaia, R.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Polozov, P.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Protopopescu, S.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Rijssenbeek, M.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Safronov, G.; Sajot, G.; Salcido, P.; Sánchez-Hernández, A.; Sanders, M. P.; Sanghi, B.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schliephake, T.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Sirotenko, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Smith, K. J.

    2012-02-22

    We report an updated measurement of the CP-violating phase, ?sJ/??, and the decay-width difference for the two mass eigenstates, ??s, from the flavor-tagged decay B0s?J/??. The data sample corresponds to an integrated luminosity of 8.0 fb?¹ accumulated with the D0 detector using pp? collisions at ?s=1.96 TeV produced at the Fermilab Tevatron collider. The 68% Bayesian credibility intervals, including systematic uncertainties, are ??s=0.163+0.065?0.064 ps?¹ and ?sJ/??=?0.55+0.38?0.36. The p-value for the Standard Model point is 29.8%.

  14. A search for resonant production of tt? pairs in 4.8 fb-1 of integrated luminosity of pp? collisions at ?s=1.96 TeV

    SciTech Connect (OSTI)

    Aaltonen, T; Alvarez Gonzalez, B; Amerio, S; Amidei, D; Anastassov, A; Annovi, A; Antos, J; Apollinari, G; Appel, J A; Apresyan, A; Arisawa, T

    2011-10-27

    We search for resonant production of tt? pairs in 4.8 fb-1 integrated luminosity of pp? collision data at ?s = 1.96 TeV in the lepton+jets decay channel, where one top quark decays leptonically and the other hadronically. A matrix element reconstruction technique is used; for each event a probability density function (pdf) of the tt? candidate invariant mass is sampled. These pdfs are used to construct a likelihood function, whereby the cross section for resonant tt? production is estimated, given a hypothetical resonance mass and width. The data indicate no evidence of resonant production of tt? pairs. A benchmark model of leptophobic Z' ? tt? is excluded with mZ' < 900 GeV at 95% confidence level.

  15. Search for the Production of Narrow t anti-b Resonances in 1.9 fb-1 of p anti-p Collisions at s**(1/2) = 1.96-TeV

    SciTech Connect (OSTI)

    Aaltonen, T.; Adelman, J.; Akimoto, T.; Alvarez Gonzalez, B.; Amerio, S.; Amidei, Dante E.; Anastassov, A.; Annovi, Alberto; Antos, Jaroslav; Apollinari, G.; Apresyan, A.; /Purdue U. /Waseda U.

    2009-02-01

    We present new limits on resonant tb production in ppbar collisions at sqrt(s) = 1.96 TeV, using 1.9 fb{sup -1} of data recorded with the CDF II detector at the Fermilab Tevatron. We reconstruct a putative tb mass in events with a lepton, neutrino candidate, and two or three jets, and search for anomalous tb production as modeled by W{prime} {yields} tb. We set a new limit on a right-handed W{prime} with standard model-like coupling, excluding any mass below 800 GeV at 95% C.L. For any narrow W{prime}-like state with mass above 800 GeV, the cross-section is found to be less than 0.28 pb at 95% C.L. We also present an exclusion of the W{prime} coupling strength versus W{prime} mass.

  16. Search for a Standard Model Higgs boson in the H -> ZZ -> llnunu decay channel using 4.7 fb-1 of sqrt(s) = 7 TeV data with the ATLAS detector

    E-Print Network [OSTI]

    ATLAS Collaboration

    2012-05-30

    A search for a heavy Standard Model Higgs boson decaying via H -> ZZ -> llnunu, where l represents electrons or muons, is presented. It is based on proton-proton collision data at sqrt(s) = 7 TeV, collected by the ATLAS experiment at the LHC during 2011 and corresponding to an integrated luminosity of 4.7 fb^-1. The data agree with the expected Standard Model backgrounds. Upper limits on the Higgs boson production cross section are derived for Higgs boson masses between 200 GeV and 600 GeV and the production of a Standard Model Higgs boson with a mass in the range 319 - 558 GeV is excluded at the 95% confidence level.

  17. Search for the Standard Model Higgs Boson in ZH?l?l?bb? Production with the D0 Detector in 9.7 fb?¹ of pp? Collisions at ?s=1.96 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.; Askew, A.; Atkins, S.; Augsten, K.; Avila, C.; Badaud, F.; Bagby, L.; Baldin, B.; Bandurin, D. V.; Banerjee, S.; Barberis, E.; Baringer, P.; Bartlett, J. F.; Bassler, U.; Bazterra, V.; Bean, A.; Begalli, M.; Bellantoni, L.; Beri, S. B.; Bernardi, G.; Bernhard, R.; Bertram, I.; Besançon, M.; Beuselinck, R.; Bhat, P. C.; Bhatia, S.; Bhatnagar, V.; Blazey, G.; Blessing, S.; Bloom, K.; Boehnlein, A.; Boline, D.; Boos, E. E.; Borissov, G.; Bose, T.; Brandt, A.; Brandt, O.; Brock, R.; Bross, A.; Brown, D.; Brown, J.; Bu, X. B.; Buehler, M.; Buescher, V.; Bunichev, V.; Burdin, S.; Buszello, C. P.; Camacho-Pérez, E.; Casey, B. C. K.; Castilla-Valdez, H.; Caughron, S.; Chakrabarti, S.; Chakraborty, D.; Chan, K. M.; Chandra, A.; Chapon, E.; Chen, G.; Chevalier-Théry, S.; Cho, D. K.; Cho, S. W.; Choi, S.; Choudhary, B.; Cihangir, S.; Claes, D.; Clutter, J.; Cooke, M.; Cooper, W. E.; Corcoran, M.; Couderc, F.; Cousinou, M.-C.; Croc, A.; Cutts, D.; Das, A.; Davies, G.; de Jong, S. J.; De La Cruz-Burelo, E.; Déliot, F.; Demina, R.; Denisov, D.; Denisov, S. P.; Desai, S.; Deterre, C.; DeVaughan, K.; Diehl, H. T.; Diesburg, M.; Ding, P. F.; Dominguez, A.; Dubey, A.; Dudko, L. V.; Duggan, D.; Duperrin, A.; Dutt, S.; Dyshkant, A.; Eads, M.; Edmunds, D.; Ellison, J.; Elvira, V. D.; Enari, Y.; Evans, H.; Evdokimov, A.; Evdokimov, V. N.; Facini, G.; Feng, L.; Ferbel, T.; Fiedler, F.; Filthaut, F.; Fisher, W.; Fisk, H. E.; Fortner, M.; Fox, H.; Fuess, S.; Garcia-Bellido, A.; García-González, J. A.; García-Guerra, G. A.; Gavrilov, V.; Gay, P.; Geng, W.; Gerbaudo, D.; Gerber, C. E.; Gershtein, Y.; Ginther, G.; Golovanov, G.; Goussiou, A.; Grannis, P. D.; Greder, S.; Greenlee, H.; Grenier, G.; Gris, Ph.; Grivaz, J.-F.; Grohsjean, A.; Grünendahl, S.; Grünewald, M. W.; Guillemin, T.; Gutierrez, G.; Gutierrez, P.; Hagopian, S.; Haley, J.; Han, L.; Harder, K.; Harel, A.; Hauptman, J. M.; Hays, J.; Head, T.; Hebbeker, T.; Hedin, D.; Hegab, H.; Heinson, A. P.; Heintz, U.; Hensel, C.; Heredia-De La Cruz, I.; Herner, K.; Hesketh, G.; Hildreth, M. D.; Hirosky, R.; Hoang, T.; Hobbs, J. D.; Hoeneisen, B.; Hogan, J.; Hohlfeld, M.; Howley, I.; Hubacek, Z.; Hynek, V.; Iashvili, I.; Ilchenko, Y.; Illingworth, R.; Ito, A. S.; Jabeen, S.; Jaffré, M.; Jayasinghe, A.; Jeong, M. S.; Jesik, R.; Jiang, P.; Johns, K.; Johnson, E.; Johnson, M.; Jonckheere, A.; Jonsson, P.; Joshi, J.; Jung, A. W.; Juste, A.; Kaadze, K.; Kajfasz, E.; Karmanov, D.; Kasper, P. A.; Katsanos, I.; Kehoe, R.; Kermiche, S.; Khalatyan, N.; Khanov, A.; Kharchilava, A.; Kharzheev, Y. N.; Kiselevich, I.; Kohli, J. M.; Kozelov, A. V.; Kraus, J.; Kulikov, S.; Kumar, A.; Kupco, A.; Kur?a, T.; Kuzmin, V. A.; Lammers, S.; Landsberg, G.; Lebrun, P.; Lee, H. S.; Lee, S. W.; Lee, W. M.; Lei, X.; Lellouch, J.; Li, D.; Li, H.; Li, L.; Li, Q. Z.; Lim, J. K.; Lincoln, D.; Linnemann, J.; Lipaev, V. V.; Lipton, R.; Liu, H.; Liu, Y.; Lobodenko, A.; Lokajicek, M.; Lopes de Sa, R.; Lubatti, H. J.; Luna-Garcia, R.; Lyon, A. L.; Maciel, A. K. A.; Madar, R.; Magaña-Villalba, R.; Malik, S.; Malyshev, V. L.; Maravin, Y.; Martínez-Ortega, J.; McCarthy, R.; McGivern, C. L.; Meijer, M. M.; Melnitchouk, A.; Menezes, D.; Mercadante, P. G.; Merkin, M.; Meyer, A.; Meyer, J.; Miconi, F.; Mondal, N. K.; Mulhearn, M.; Nagy, E.; Naimuddin, M.; Narain, M.; Nayyar, R.; Neal, H. A.; Negret, J. P.; Neustroev, P.; Nguyen, H. T.; Nunnemann, T.; Orduna, J.; Osman, N.; Osta, J.; Padilla, M.; Pal, A.; Parashar, N.; Parihar, V.; Park, S. K.; Partridge, R.; Parua, N.; Patwa, A.; Penning, B.; Perfilov, M.; Peters, Y.; Petridis, K.; Petrillo, G.; Pétroff, P.; Pleier, M.-A.; Podesta-Lerma, P. L. M.; Podstavkov, V. M.; Popov, A. V.; Prewitt, M.; Price, D.; Prokopenko, N.; Qian, J.; Quadt, A.; Quinn, B.; Rangel, M. S.; Ranjan, K.; Ratoff, P. N.; Razumov, I.; Renkel, P.; Ripp-Baudot, I.; Rizatdinova, F.; Rominsky, M.; Ross, A.; Royon, C.; Rubinov, P.; Ruchti, R.; Sajot, G.; Salcido, P.; Sánchez-Hernández, A.; Sanders, M. P.; Santos, A. S.; Savage, G.; Sawyer, L.; Scanlon, T.; Schamberger, R. D.; Scheglov, Y.; Schellman, H.; Schlobohm, S.; Schwanenberger, C.; Schwienhorst, R.; Sekaric, J.; Severini, H.; Shabalina, E.; Shary, V.; Shaw, S.; Shchukin, A. A.; Shivpuri, R. K.; Simak, V.; Skubic, P.; Slattery, P.; Smirnov, D.; Smith, K. J.; Snow, G. R.; Snow, J.; Snyder, S.; Söldner-Rembold, S.; Sonnenschein, L.; Soustruznik, K.; Stark, J.; Stoyanova, D. A.; Strauss, M.; Suter, L.; Svoisky, P.; Takahashi, M.; Titov, M.; Tokmenin, V. V.; Tsai, Y.-T.; Tschann-Grimm, K.; Tsybychev, D.; Tuchming, B.; Tully, C.; Uvarov, L.; Uvarov, S.; Uzunyan, S.; Van Kooten, R.; van Leeuwen, W. M.; Varelas, N.; Varnes, E. W.

    2012-09-01

    We present a search for the standard model (SM) Higgs boson produced in association with a Z boson in 9.7 fb?¹ of pp? collisions collected with the D0 detector at the Fermilab Tevatron Collider at ?s=1.96 TeV. Selected events contain one reconstructed Z?e?e? or Z????? candidate and at least two jets, including at least one jet identified as likely to contain a b quark. To validate the search procedure, we also measure the cross section for ZZ production in the same final state. It is found to be consistent with its SM prediction. We set upper limits on the ZH production cross section times branching ratio for H?bb? at the 95% C.L. for Higgs boson masses 90?MH?150 GeV. The observed (expected) limit for MH=125 GeV is 7.1 (5.1) times the SM cross section.

  18. Measurement of sin(2)?(?)(eff) and Z-light quark couplings using the forward-backward charge asymmetry in pp-bar?Z/?*?e(+)e(?) events with L=5.0??fb(?1) at s?=1.96??TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Carrasco-Lizarraga, M. A.; Clutter, Justace Randall; McGivern, Carrie Lynne; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.

    2011-07-26

    -4 determinations of sin2?‘eff come from the b-quark forward- backward asymmetry at LEP, A0;bFB , with sin2?‘eff ¼ 0:232 21 ? 0:000 29, and the left-right asymmetry at SLD, AlrðSLDÞ, with sin2?‘eff ¼0:23098?0:00026. These two measurements differ from each other... and SLD Collaborations [15]. The comparison is shown in Fig. 6. The most precise measure- ments are the LEP b-quark forward-backward asymmetry, A0;bFB , the SLD left-right asymmetry, AlrðSLDÞ, the LEP ?-lepton polarization measurement, AlðP?Þ, and the SLD...

  19. Adaptation of the modified Bouc–Wen model to compensate for hysteresis in respiratory motion for the list-mode binning of cardiac SPECT and PET acquisitions: Testing using MRI

    SciTech Connect (OSTI)

    Dasari, Paul K. R.; Shazeeb, Mohammed Salman [Department of Radiology, Division of Nuclear Medicine, University of Massachusetts Medical School, Worcester, Massachusetts 01655 and Department of Biomedical Engineering, Worcester Polytechnic Institute, Worcester, Massachusetts 01609 (United States); Könik, Arda; Lindsay, Clifford; Mukherjee, Joyeeta M.; Johnson, Karen L.; King, Michael A., E-mail: Michael.King@umassmed.edu [Department of Radiology, Division of Nuclear Medicine, University of Massachusetts Medical School, Worcester, Massachusetts 01655 (United States)

    2014-11-01

    Purpose: Binning list-mode acquisitions as a function of a surrogate signal related to respiration has been employed to reduce the impact of respiratory motion on image quality in cardiac emission tomography (SPECT and PET). Inherent in amplitude binning is the assumption that there is a monotonic relationship between the amplitude of the surrogate signal and respiratory motion of the heart. This assumption is not valid in the presence of hysteresis when heart motion exhibits a different relationship with the surrogate during inspiration and expiration. The purpose of this study was to investigate the novel approach of using the Bouc–Wen (BW) model to provide a signal accounting for hysteresis when binning list-mode data with the goal of thereby improving motion correction. The study is based on the authors’ previous observations that hysteresis between chest and abdomen markers was indicative of hysteresis between abdomen markers and the internal motion of the heart. Methods: In 19 healthy volunteers, they determined the internal motion of the heart and diaphragm in the superior–inferior direction during free breathing using MRI navigators. A visual tracking system (VTS) synchronized with MRI acquisition tracked the anterior–posterior motions of external markers placed on the chest and abdomen. These data were employed to develop and test the Bouc–Wen model by inputting the VTS derived chest and abdomen motions into it and using the resulting output signals as surrogates for cardiac motion. The data of the volunteers were divided into training and testing sets. The training set was used to obtain initial values for the model parameters for all of the volunteers in the set, and for set members based on whether they were or were not classified as exhibiting hysteresis using a metric derived from the markers. These initial parameters were then employed with the testing set to estimate output signals. Pearson’s linear correlation coefficient between the abdomen, chest, average of chest and abdomen markers, and Bouc–Wen derived signals versus the true internal motion of the heart from MRI was used to judge the signals match to the heart motion. Results: The results show that the Bouc–Wen model generated signals demonstrated strong correlation with the heart motion. This correlation was slightly larger on average than that of the external surrogate signals derived from the abdomen marker, and average of the abdomen and chest markers, but was not statistically significantly different from them. Conclusions: The results suggest that the proposed model has the potential to be a unified framework for modeling hysteresis in respiratory motion in cardiac perfusion studies and beyond.

  20. Search for the standard model Higgs boson produced in association with a Z boson in 7.9 fb[superscript ?1] of p[bar-over p] collisions at ?s = 1.96 TeV using the CDF II detector

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We present a search for the standard model Higgs boson produced in association with a Z boson, using up to 7.9 fb[superscript ?1] of integrated luminosity from p[bar-over p] collisions collected with the CDF II detector. ...

  1. Combined CDF and Dzero Upper Limits on Standard Model Higgs Boson Production at High Mass (155-200 GeV/c2) with 3 fb-1 of data

    E-Print Network [OSTI]

    Tevatron New Phenomena; Higgs working group; CDF Collaboration; D0 Collaboration

    2008-08-05

    We combine results from CDF and DO searches for a standard model Higgs boson in ppbar collisions at the Fermilab Tevatron, at sqrt{s}=1.96 TeV. With 3.0 fb-1 of data analyzed at CDF, and at DO, the 95% C.L. upper limits on Higgs boson production are a factor of 1.2, 1.0 and 1.3 higher than the SM cross section for a Higgs boson mass of m_{H}=$165, 170 and 175 GeV, respectively. We exclude at 95% C.L. a standard model Higgs boson of m_H=170 GeV. Based on simulation, the ratios of the corresponding median expected upper limit to the Standard Model cross section are 1.2, 1.4 and 1.7. Compared to the previous Higgs Tevatron combination, more data and refined analysis techniques have been used. These results extend significantly the individual limits of each experiment and provide new knowledge on the mass of the standard model Higgs boson beyond the LEP direct searches.

  2. Search for Higgs boson production in oppositely charged dilepton and missing energy final states in 9.7 fb-1 of ppbar collisions at sqrts = 1.96 TeV

    E-Print Network [OSTI]

    D0 Collaboration

    2013-01-07

    We present a search for Higgs boson in final states with two oppositely charged leptons and large missing transverse energy as expected in H -> WW -> lvlv decays. The events are selected from the full Run II data sample of 9.7 fb-1 of ppbar collisions collected with the D0 detector at the Fermilab Tevatron Collider at sqrt s = 1.96 TeV. To validate our search methodology, we measure the non-resonant W W production cross section and find sigma_WW = 11.6 +/- 0.7 pb, in agreement with the standard model prediction. In the Higgs boson search, no significant excess above the background expectation is observed. Upper limits at the 95% confidence level on the Higgs boson production cross section are therefore derived. Within the standard model, the Higgs boson mass range 159 Higgs boson production cross sections 4.1 times larger than the standard model expectation, which is compatible with the presence of a Higgs boson at this mass. Within a theoretical framework with a fourth generation of fermions, the mass range 125 Higgs boson couplings, which yields an exclusion of fermiophobic Higgs boson production cross sections 3.1 times larger than the expectation for MH = 125 GeV.

  3. Search for a Higgs boson in diphoton final states with the D0 detector in 9.6 fb-1 of p-pbar collisions at sqrt(s)=1.96 TeV

    E-Print Network [OSTI]

    D0 Collaboration

    2013-01-22

    We present a search for a Higgs boson decaying into a pair of photons based on 9.6 fb-1 of p-pbar collisions at sqrt(s)=1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. The search employs multivariate techniques to discriminate signal from the non-resonant background and is separately optimized for a standard model and a fermiophobic Higgs boson. No significant excess of data above the background prediction is observed and upper limits on the product of the cross section and branching fraction are derived at the 95% confidence level as a function of Higgs boson mass. For a standard model Higgs boson with mass of 125 GeV, the observed (expected) upper limits are a factor of 12.8 (8.7) above the standard model prediction. The existence of a fermiophobic Higgs boson with mass in the 100-113 GeV range is excluded at the 95% confidence level.

  4. Search for the Standard Model Higgs boson in the decay channel H -> ZZ((*)) -> 4l with 4.8 fb(-1) of pp collision data at root s=7 TeV with ATLAS

    SciTech Connect (OSTI)

    Aad G.; Abbott B.; Abdallah J.; Khalek S. Abdel; Abdelalim A. A.; Abdesselam A.; Abdinov O.; Abi B.; Abolins M.; AbouZeid U. S.; Abramowicz H.; Abreu H.; Acerbi E.; Acharya B. S.; Adamczyk L.; Adams D. L.; Addy T. N.; Adelman J.; et al.

    2012-04-12

    This Letter presents a search for the Standard Model Higgs boson in the decay channel H {yields} ZZ{sup (*)} {yields} {ell}{sup +}{ell}{sup -}{ell}{prime}{sup +}{ell}{prime}{sup -}, where {ell}, {ell}{prime} = e or {mu}, using proton-proton collisions at {radical}s = 7 TeV recorded with the ATLAS detector and corresponding to an integrated luminosity of 4.8 fb{sup -1}. The four-lepton invariant mass distribution is compared with Standard Model background expectations to derive upper limits on the cross section of a Standard Model Higgs boson with a mass between 110 GeV and 600 GeV. The mass ranges 134-156 GeV, 182-233 GeV, 256-265 GeV and 268-415 GeV are excluded at the 95% confidence level. The largest upward deviations from the background-only hypothesis are observed for Higgs boson masses of 125 GeV, 244 GeV and 500 GeV with local significances of 2.1, 2.2 and 2.1 standard deviations, respectively. Once the look-elsewhere effect is considered, none of these excesses are significant.

  5. Measurement of the inclusive jet cross-section in proton-proton collisions at $\\sqrt{s}=7$ TeV using 4.5 fb$^{-1}$ of data with the ATLAS detector

    E-Print Network [OSTI]

    ATLAS Collaboration

    2015-10-09

    The inclusive jet cross-section is measured in proton-proton collisions at a centre-of-mass energy of 7 TeV using a data set corresponding to an integrated luminosity of 4.5 fb$^{-1}$ collected with the ATLAS detector at the Large Hadron Collider in 2011. Jets are identified using the anti-$k_t$ algorithm with radius parameter values of 0.4 and 0.6. The double-differential cross-sections are presented as a function of the jet transverse momentum and the jet rapidity, covering jet transverse momenta from 100 GeV to 2 TeV. Next-to-leading-order QCD calculations corrected for non-perturbative effects and electroweak effects, as well as Monte Carlo simulations with next-to-leading-order matrix elements interfaced to parton showering, are compared to the measured cross-sections. A quantitative comparison of the measured cross-sections to the QCD calculations using several sets of parton distribution functions is performed.

  6. Scattering versus polarization Scattering amplitudes: fa, fb

    E-Print Network [OSTI]

    Zhang, Guifu

    · ^y ^hs · ^z ^vs · ^x ^vs · ^y ^vs · ^z " # $ % & ' ! Ci = ^hi · ^x ^vi · ^x hi · ^y ^vi · ^y ^hi · ^z = ^hi · ^xb ^vi · ^xb hi · ^yb ^vi · ^yb ^hi · ^zb ^vi · ^zb " # $ $ $ % & ' ' ' ! ^xb ^yb ^zb " # $ % & ' *x 0 0 0 *y 0 0 0 *z " # $ $ $ % & ' ' ' ^hi · ^xb ^vi · ^xb hi · ^yb ^vi · ^yb ^hi · ^zb ^vi · ^zb

  7. y12 1950-55 FB

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLosThe 26thI D- 6 0 4 2 r mReducingwhistleblowerxinyufu Ames25

  8. Materials Data on CsH7O4 (SG:14) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  9. The Search for VH $\\bf\\to$ VWW Standard Model \\\\ Higgs Production in the Trilepton Signature\\\\ with $\\bf5.9\\fb$ of Data from $\\bf\\ppbar$ Collisions \\\\ at $\\bf\\sqrt{s}=1.96$ GeV

    SciTech Connect (OSTI)

    Nett, Jason Michael; /Wisconsin U., Madison

    2010-06-01

    We present here the search for Standard Model VH {yields} VWW {yields} lll + E{sub T} (missing energy due to neutrinos) production, where V is a W or Z weak vector boson, which uses up to 5.9 fb{sup -1} of integrated luminosity. This analysis has recently added to the CDF high-mass Higgs group three new signal topologies characterized by a tri-lepton signature, which are chosen to isolate the VH {yields} VWW associated production signals in the three-lepton signature. As such, we define three new regions for a WH analysis, a ZH 1-jet analysis, and a ZH {ge} 2-jet analysis with which we expect to contribute an additional {approx} 5.8% (for m{sub H} = 165 GeV) acceptance to the current H {yields} WW dilepton analysis. The ZH trilepton regions are defined by events passing a Z-boson selection: events having at least one lepton pairing (among three possible pairings) with opposite sign, same flavor, and a dilepton invariant mass within [76.0, 106.0] GeV - a {+-} 15 GeV window around the Z-boson mass. The WH trilepton region is then defined as the set of trilepton events that are complement to those chosen by the Z-boson selection. These three new event topologies make a substantial contribution to the H {yields} WW group result. As a measure of the sensitivity of this search, we compute the median expected limit on the at 95% confidence level ('C.L.') on the production cross section (effectively the rate of production) for a Standard Model Higgs boson and report the result as a ratio to the theoretical production cross section. An observed limit ratio of one or less at a given mass would rule out the production of a Standard Model Higgs boson at that mass with 95% confidence. At m{sub H} = 165 GeV, the WH analysis expected limits reach 7.2 times the standard model cross section; the ZH 1-jet analysis is set at 29 times the expected standard model cross section; the ZH {ge} 2-jet analysis is set at 9.9 times the expected standard model cross section; and the combined trilepton analysis is set at 4.9 times the expected standard model cross section. We announce that the combination of this trilepton VH {yields} VWW Higgs boson search and the previous CDF dilepton H {yields} WW search achieves an expected median limit of 1.00 at 165 GeV/c{sup 2}. The expected median limit of 1.00 indicates we anticipate a 50% probability of ruling out the existence of a Standard Model Higgs boson with a mass of 165 GeV/c{sup 2}. This is the first time a single hadron collider experiment has achieved sensitivity to the production of a Standard Model Higgs boson. We do not see evidence for a significant signal of Higgs bosons in the data and place observed limits on the production of a Standard Model Higgs boson of 165 GeV/c{sup 2} at 1.08 times Standard Model production cross section.

  10. PROCEEDINGS Open Access Unsupervised binning of environmental

    E-Print Network [OSTI]

    Chin, Francis Y.L.

    sequencing techniques, traditional research methods based on the isolation and cultivation of microorganisms on reference genomes of known microorganisms and phylogenetic marker genes. Due to the limited availability and alcohol brewing with yeast as well as the fatal pathogen of pulmonary tuber- culosis and cholera

  11. Measurement of sin2 ??eff and Z-light quark couplings using the forward-backward charge asymmetry in pp? -> Z/gamma* -> e+e- events with L=5.0 fb-1 at ?s=1.96 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Abazov, V. M.

    2011-07-26

    We measure the mass dependence of the forward-backward charge asymmetry in 157,553 pp? = Z/?* = e+e- interactions, corresponding to 5.0 fb-1 of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider at ?s = 1.96 TeV. The effective weak mixing angle (??eff) from this process involving predominantly the first generation of quarks is extracted as sin2 ??eff = 0.2309 ± 0.0008 (stat.) ± 0.0006 (syst.). We also present the most precise direct measurement of the vector and axial-vector couplings of u and d quarks to the Z boson.

  12. Analysis of Air Conditioning Effectiveness vs. Outdoor Conditions: Traditional Bins or Joint Frequency Bins

    E-Print Network [OSTI]

    Cohen, B. M.

    1998-01-01

    There are a number of methods used to estimate the effectiveness of air conditioning equipment in handling loads. Full hourly computer simulations are probably the most accurate, but lack flexibility and are more cumbersome ...

  13. FB2 Biologie / Chemie www.uni-bremen.de

    E-Print Network [OSTI]

    Diekmann, Martin

    , differentiation of simple functions, application: extreme value) · Integral calculus (definitions, calculation functions), sequences and series) · Differential calculus of one variable (definitions, calculation rules-chenregeln, Differentiation einfacher Funktionen, Anwendung: Extremwerte) -Integralrechnung (Definitionen, Rechenregeln

  14. FB EcoSolutions LLC | Open Energy Information

    Open Energy Info (EERE)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on QA:QA J-E-1 SECTION J APPENDIX ECoopButtePowerEdisto Electric Coop,Erosion FlumeEventFAOFB EcoSolutions LLC Jump to:

  15. Financial-Based (FB) CRAC (rates/adjustments)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would likeUniverse (Journal Article) |Final Report DocumentRatesFinancialFinancial

  16. FB/SN CRAC Workshops (rates/meetings)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would like submitKansasCommunitiesofExtrans - Permeation Measurement2 0 thFATIGUE

  17. 7600 Sand Point Way Northeast BIN C15700, Building 4

    E-Print Network [OSTI]

    , biomass, and biological composition of walleye pollock in Chiniak and Barnabas Troughs; 3.2 collect nets (e.g. Marinovich, Methot, or bongo nets), acoustic buoy deployments, physical oceanographic data

  18. 102 Computer Ich bin der Geist, der stets verneint,

    E-Print Network [OSTI]

    Meyer, Bertrand

    ). Quality First is fundamentally tied to object technology and design by contract. It's just Cleanroom development. Like Quality First, Cleanroom emphasizes for- mal reasoning. Unlike Quality First, it shuns unit

  19. The volatile compound BinBase mass spectral database

    E-Print Network [OSTI]

    Skogerson, Kirsten; Wohlgemuth, Gert; Barupal, Dinesh K; Fiehn, Oliver

    2011-01-01

    B, Eriksson R: SuperScent-a database of flavors and scents.Sayaed AM: The Pherobase: Database of Insect Pheromones andA public study design database for metabolomics projects.

  20. The Maximum Resource Bin Packing Problem Joan Boyar 1

    E-Print Network [OSTI]

    Larsen, Kim Skak

    Department of Accounting, Finance, and Logistics Aarhus School of Business, Aarhus, Denmark sanw are interesting also when considered from the reverse perspective of trying to maximize the amount of resources that

  1. Smart Bin for Incompatible Waste Items Arnab Sinha

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    in the context of waste management, where considerable volume of waste is present collectively and there may are performed based on the knowledge available locally without looking up from any external sources. Since, the global identification of objects is avoided, preservation of privacy is ensured, which is a concern

  2. NRAO 225 GHz Tipping Radiometer Computer Operation

    E-Print Network [OSTI]

    Groppi, Christopher

    Area Network) . . . . . . . . . . . . 9 3.1.5 Chajnantor Computer Hardware . . . . . . . . . . . . 9 3.csh . . . . . . . . . . . . . . . . . . . . . . . . . . 51 6.6.3 time.csh . . . . . . . . . . . . . . . . . . . . . . . . . . 51 6.6.4 Cdb

  3. Rapid Prototypingof Tools Lee E. Welss, E. Levent Gursoz, F.B. Prim,

    E-Print Network [OSTI]

    Weiss, Lee E.

    by the DefenseAdvanced ResearchAgency underthe Office of Naval Research contract N00014-68-K-0642, in part Flgure3-1: Electrlc Arc Spraylng Figure3-2: ConventionalMold Figure3-3: SprayedTool Process Figure34: SprayedTurblne Blade Mold Figure3-5: SLA MoldPatterns Flgure 36: Parting Plane Model Figure 4-1: Sllclng

  4. CDF note 9640 Search for X ZZ with 3 fb-1

    E-Print Network [OSTI]

    Quigg, Chris

    dilepton pair using the nominal CDF event reconstruction software, we reprocess these events pair of final states from the reprocessed data. The electron criteria listed in Tables I through III

  5. Chiral U(1) Flavor Models and Flavored Higgs Doublets: The Top FB Asymmetry

    Office of Scientific and Technical Information (OSTI)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield MunicipalTechnical Report: Achievements ofCOMPOSITION OF VAPORS FROM BOILINGChemCam on Marsand the

  6. Chiral U(1) Flavor Models and Flavored Higgs Doublets: The Top FB Asymmetry

    Office of Scientific and Technical Information (OSTI)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefieldSulfate Reducing Bacteria (TechnicalTransmission,TextitSciTechin ComplexChi-NuSciTechand the Wjj__

  7. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine

    Broader source: Energy.gov [DOE]

    2013 DOE Hydrogen and Fuel Cells Program and Vehicle Technologies Program Annual Merit Review and Peer Evaluation Meeting

  8. A Domain-Independent Multiplayer Architecture for Training Ahmed BinSubaih

    E-Print Network [OSTI]

    Maddock, Steve

    the games world to address them. Thus we have developed a prototype architecture which makes use a prototype version for traffic accident training for police officers in the Dubai police force. We conclude

  9. Application of a Diesel Fuel Reformer for Tier 2 Bin 5 Emissions...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    2005 Diesel Engine Emissions Reduction (DEER) Conference Presentations and Posters 2005deerbonadies.pdf More Documents & Publications Application of a Diesel Fuel Reformer for...

  10. Ich bin nicht ein Berliner: A Reconsideration of Marsden Hartley's Portrait of a German Officer

    E-Print Network [OSTI]

    Kramer, Sean

    2012-04-01

    ?olitan Museum of Art9 New York. 236 This painting, e x e c u t e d in N o v e m b e r 1914, s h o w s Hartley's assimilat ion of both C u b i s m (the collagelike juxtaposi t ions of v isual f ragments) and G e r m a n E x p r e s s i o n i s m (the coarse... b r u s h w o r k and d r a m a t i c use of br ight colors and b l a c k ) . In 1916 the artist denied that the objects in the paint ing h a d a n y special m e a n i n g (perhaps as a defensive m e a s u r e to w a r d off a n y attacks p r o v...

  11. Sliding Mode Flow Rate Observer Design Song Liu and Bin Yao

    E-Print Network [OSTI]

    Yao, Bin

    with the control valves (i.e., the cylinder internal and external leakage flows, and so on). It is assumed that: a rate information is needed in a lot of applications, such as automated modelling of valve flow mapping

  12. Model Based Fault Detection of an Electro-Hydraulic Cylinder Phanindra Garimella and Bin Yao

    E-Print Network [OSTI]

    Yao, Bin

    in the control valves, nonlinear pressure/flow relations and vari- ation in fluid volumes due to the movement and component wear [9]. Other general nonlinearities such as external disturbances, leakage, and friction cannot

  13. Automated Modelling of Cartridge Valve Flow Mapping Song Liu and Bin Yao

    E-Print Network [OSTI]

    Yao, Bin

    significantly saving energy usage. Unlike costly conventional four-way valves, the cartridge valve has simple poppet-type cartridge valves are the key elements of the energy saving programmable valves, which have and practicality of the proposed novel automated modelling method. I. INTRODUCTION The energy saving programmable

  14. What can you recycle at MIT? All Paper in desk side and blue-top bins

    E-Print Network [OSTI]

    Seager, Sara

    ://web.mit.edu/environment BatteriesBatteries Nickel-cadmium, Button and Lithium batteries. Alkaline batteries can be disposed of in the trash. Nickel-cadmium, Button and Lithium batteries. Alkaline batteries can be disposed of in the trash. Technotrash CDs,diskettes,audio and video tapes Cell phones,pagers,and PDAs Rechargeable batteries Technotrash

  15. Finding Osama Bin Laden: An Application of Biogeographic Theories and Satellite Imagery

    E-Print Network [OSTI]

    2009-01-01

    in the Kurram region of Pakistan, (2) located in the city ofTribal Areas of Northwest Pakistan based on distance-decaymore secular parts of Pakistan or into India, the greater

  16. For some, Bin Laden's death harkens to Hitler's 66 years ago

    E-Print Network [OSTI]

    Fernandez, Eduardo

    become the stuff of sports victories or Twitter-fomented revolutions in the Middle East. For American been forgotten, at least temporarily, in the wake of what the U.S. Navy's Seal Team Six pulled off. "It't taught any more. I do presentations about the war at elementary schools, but most kids don't know

  17. Bin-MAC: A Hybrid MAC for Ultra-Compact Wireless Sensor Nodes Vahid Salmani

    E-Print Network [OSTI]

    Chou, Pai H.

    status monitoring to target tracking. Although many protocols have been proposed in the literature, few

  18. http://www.caycompass.com/cgi-bin/CFPnews.cgi?ID=1020374 Environmental plans outlined

    E-Print Network [OSTI]

    Exeter, University of

    for environmental impact assessments, he said, in order to ensure that environmental consequences are examined to sustainable development. In 2006, Mr. Clifford's Ministry supported the creation of a Sustainable Development and implementation of a National Sustainable Development Strategy, a framework for which is currently being developed

  19. Predicting Extreme Phases of the Indian Summer Monsoon* QINGHUA DING AND BIN WANG

    E-Print Network [OSTI]

    Wang, Bin

    of suppressed convection originating from the equatorial Indian Ocean and the South China Sea precede extremely in this knowledge gap. The boreal summer ISO over India has long been regarded as a source of active and break

  20. On Bulk Loading TPR-Tree Bin Lin and Jianwen Su

    E-Print Network [OSTI]

    Su, Jianwen

    a histogram-based bottom up algorithm (HBU) along with a modified top-down greedy split algo- rithm (TGS show that HBU outperforms both TPR and TGS for all kinds of non-uniform datasets, is relatively stable and compare it with the original TPR- tree bulk loading algorithm and a modified top-down greedy split (TGS

  1. US Tier 2 Bin 2 Diesel Research Progress | Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Light-Duty Diesel EngineTechnology to Meet Future Emissions and Performance Requirements of the U.S. Market Diesel Passenger Car Technology for Low Emissions and CO2 Compliance...

  2. Modelling a CNTFET with Undeposited CNT Defects Geunho Cho, Fabrizio Lombardi, Yong-Bin Kim

    E-Print Network [OSTI]

    Ayers, Joseph

    and manufacturing a CNTFET, additional features such as pitch, number and position of the CNTs must be considered. INDEX TERMS: Defect model, CNT, CNTFET, manufacturing, emerging technologies 1. Introduction The Carbon manufacturing processes. In CNTFETs, ballistic or near-ballistic transport phenomena have been observed under

  3. Materials Data on Th2BiN2 (SG:139) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  4. Materials Data on U2BiN2 (SG:139) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  5. The Method of Improving the Specific Language Focused Shan-Bin Chan

    E-Print Network [OSTI]

    In recent years, more and more CJK (Chinese, Japanese, and Korean) web pages appear in the Internet. The infor- mation in the CJK web page also be- comes more and more important. Web crawler is a kind of tool to retrieve web pages. Previous researches focused on English web crawlers and the web crawler is always

  6. The BMW Approach to Tier2 Bin5 | Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Engine-Efficiency & Emissions Research Conference (DEER 2007). 13-16 August, 2007, Detroit, Michigan. Sponsored by the U.S. Department of Energy's (DOE) Office of FreedomCAR...

  7. Strategies for In-Cylinder Reductions to Reach Bin 2 and LEV...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Can Future Emissions Limits be Met with a Hybrid EGR System Alone? Control Strategy for a Dual Loop EGR System to Meet Euro 6 and Beyond Advanced Diesel Engine Technology...

  8. Application of a Diesel Fuel Reformer for Tier 2 Bin 5 Emissions...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Detroit, Michigan. Sponsored by the U.S. DOE's EERE FreedomCar and Fuel Partnership and 21st Century Truck Programs. 2006deerbonadies.pdf More Documents & Publications...

  9. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:Financing ToolInternationalReportOffice |4-01r2.pdf AL2004-01r2.pdfAL2RiseBabcockInnovation You Can

  10. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine | Department of

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:Financing ToolInternationalReportOffice |4-01r2.pdf AL2004-01r2.pdfAL2RiseBabcockInnovation You

  11. ATP-LD; Cummins Next Generation Tier 2 Bin 2 Diesel Engine | Department of

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:Financing ToolInternationalReportOffice |4-01r2.pdf AL2004-01r2.pdfAL2RiseBabcockInnovation

  12. http://cemp.dri.edu/cgi-bin/cemp_stations.pl?stn=tono&prod=11

    National Nuclear Security Administration (NNSA)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal GasAdministration Medal01 Sandia4)9 Federal RegisterStorm1 34460/%2A en3 Community

  13. http://cemp.dri.edu/cgi-bin/cemp_stations.pl?stn=tono&prod=11

    National Nuclear Security Administration (NNSA)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal GasAdministration Medal01 Sandia4)9 Federal RegisterStorm1 34460/%2A en3 Community1

  14. http://frwebgate.access.gpo.gov/cgi-bin/getdoc.cgi?dbname=106_c

    National Nuclear Security Administration (NNSA)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal GasAdministration Medal01 Sandia4)9 Federal RegisterStorm193-DETERMINING

  15. http://frwebgate.access.gpo.gov/cgi-bin/usc.cgi?ACTION=RETRIEVE

    National Nuclear Security Administration (NNSA)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal GasAdministration Medal01 Sandia4)9 Federal RegisterStorm193-DETERMININGResources by

  16. Demonstration of the Equivalence of Soft and Zero-Bin Subtractions (Journal

    Office of Scientific and Technical Information (OSTI)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefieldSulfate Reducing BacteriaConnectlaser-solid interaction (Journal

  17. Demonstration of the Equivalence of Soft and Zero-Bin Subtractions (Journal

    Office of Scientific and Technical Information (OSTI)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefieldSulfate Reducing BacteriaConnectlaser-solid interaction (JournalArticle) | SciTech Connect

  18. On The Equivalence of Soft and Zero-Bin Subtractions (Journal Article) |

    Office of Scientific and Technical Information (OSTI)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefieldSulfateSciTech ConnectSpeeding access to science information from(Conference)Article) |SciTech

  19. On The Equivalence of Soft and Zero-Bin Subtractions (Journal Article) |

    Office of Scientific and Technical Information (OSTI)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefieldSulfateSciTech ConnectSpeeding access to science information from(Conference)Article)

  20. Hmelo, Bin Hu, Alamgir Karim, Martyn McLachlan, and Ron Jones (by phone)

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would likeUniverse (JournalvivoHigh energyHighland View school4-TP59.01 C5;44Meeting of the CNMS

  1. Characterization of the Dynamics in the Protonic Conductor CsH2PO4 by 17O Solid-State NMR Spectroscopy and First-Principles Calculations: Correlating Phosphate and Protonic Motion

    E-Print Network [OSTI]

    Kim, Gunwoo; Griffin, John M.; Blanc, Frédéric; Haile, Sossina M.; Grey, Clare P.

    2015-03-03

    in the superprotonic phase, proton conductivity arising from structural and dynamic disorder of hydrogen bonds and phosphate anions.6 Understanding this is key to engineering novel, improved electrolytic materials for these applications. In this context, mixed... Hz. Powder averaging was achieved using the ZCW6765 scheme. For all oxygen sites, ?iso, CQ, ?Q, and the Euler angles describing the relative orientations of the electric field gradient (EFG) tensors for the oxygen sites were used as input parameters, the data...

  2. Chemomechanics of calcium leaching of cement-based materials at different scales : the role of CH-dissolution and C-S-H degradation on strength and durability performance of materials and structures

    E-Print Network [OSTI]

    Heukamp, Franz H. (Franz Hoyte), 1973-

    2003-01-01

    Calcium leaching is a durability threat for cement-based materials employed in critical infrastructures, such as Nuclear Waste Storage Systems. This thesis presents a comprehensive study of the material and structural ...

  3. Quantum Mechanical Metric for Internal Cohesion in Cement Crystals

    E-Print Network [OSTI]

    Dharmawardhana, C. C.; Misra, Anil; Ching, Wai-Yim

    2014-12-05

    Calcium silicate hydrate (CSH) is the main binding phase of Portland cement, the single most important structural material in use worldwide. Due to the complex structure and chemistry of CSH at various length scales, the focus has progressively...

  4. THE ERNEST KEMPTON ADAMS FbND FOR PHYSICAL RESEARCH OF COLUMBIA UNM3R!XI'Y

    E-Print Network [OSTI]

    Santos, Juan

    of soil mechanics. Terzaghi's treatment, however, is restricted to the one-dimensional problem of a column (Received October 2.5, 1940) The settlement of soils under load is caused by a phenomenon called consolidation, whose mechanism is known to be in many cases identical with the process of squeezing water out

  5. Ionisation of the Middle Atmosphere by Energetic Particles May-Britt Kallenrode FB Physik, University of Osnabruck

    E-Print Network [OSTI]

    Kallenrode, May-Britt

    . Their relation is described by two kinds of models: proton precipitation in solar energetic particle (SEP] Previous own contribution: development of an Atmospheric Ionization Module (AIMOS) [7] based on a Monte of ion- ization (protons) in selected events [5, 6, 8, 9] Open Questions modeling (and comparison

  6. '('()%0 1 243 57698A@CB(8EDGF24FB(8AHI8A24P

    E-Print Network [OSTI]

    to share and re-use knowledge between the geographical lo- cations. As O'Leary claims, KM is difficult when knowl- edge flows (e.g. face to face communication) are simply not present (O'Leary, 1998). Selected

  7. 3 Rigid Spacecraft Attitude Control Consider a rigid spacecraft with body-fixed frame Fb with origin O at the

    E-Print Network [OSTI]

    Damaren, Christopher J.

    from u to is passive. It follows that the strictly passive feedback, u = -Kd, Kd = KT d > O (2) yields, hence = 0. In order to stabilize this equilibrium, we must feed back in some form. Building on our makes senses in the limit of small angles, since the map from u to = is passive and the above

  8. Combination of searches for anomalous top quark couplings with 5.4 fb(-1) of pp-bar collisions

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Chen, G.; Clutter, Justace Randall; McGivern, Carrie Lynne; Sekaric, Jadranka; Wilson, Graham Wallace; D0 Collaboration; Abazov, V. M.; Abbott, B.; Acharya, B.S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.; Alton, A.; Alverson, G.

    2012-07-09

    , M.-C. Cousinou l, A. Croc o, D. Cutts bt, A. Das ap, G. Davies an, .J. de Jong ad,ae, E. De La Cruz-Burelo ac, F. Déliot o, R. Demina bn, D. Denisov as, S.P. Denisov ai, S. Desai as, . Deterre o, K. DeVaughan bi, H.T. Diehl as, M. Diesburg as, P..., Ferbel bn, F. Fiedler u, F. Filthaut ad,ae, W. Fisher bg, H.E. Fisk as, M. Fortner au, H. Fox am, S. Fuess as, . Garcia-Bellido bn, J.A. García-González ac, G.A. García-Guerra ac,3, V. Gavrilov ag, P. Gay j, W. Geng l,bg, . Gerbaudo bk, C.E. Gerber at, Y...

  9. Bin Li, John O'Loughlin and Lee Gillam (PI) Department of Computing, FEPS, University of Surrey

    E-Print Network [OSTI]

    Gillam, Lee

    Application-Specific Service Level Agreements: Experiments in Clouds and Grids, In Antonopoulos and Gillam Journal of Grid and Utility Computing (IJGUC) ISSN (Online): 1741-8488 - ISSN (Print): 1741-847X. (In, Oxford, UK. [1] Li, B. and Gillam, L. (2009), Grid Service Level Agreements using Financial Risk Analysis

  10. University of Tulsa Technical Report UTULSA-MCS-93-8, May, 1993. A Heuristic for Improved Genetic Bin Packing

    E-Print Network [OSTI]

    Wainwright, Roger L.

    University of Tulsa Technical Report UTULSA-MCS-93-8, May, 1993. A Heuristic for Improved Genetic Sciences, The University of Tulsa, 600 South College Avenue, Tulsa, OK 74104-3189, USA Keywords

  11. TEEVE: The Next Generation Architecture for Tele-immersive Environments Zhenyu Yang, Klara Nahrstedt, Yi Cui, Bin Yu, Jin Liang

    E-Print Network [OSTI]

    Nahrstedt, Klara

    Science SC, 201 N. Goodwin, Urbana, IL 61801 {zyang2, klara}@uiuc.edu Sang-hack Jung, Ruzena Bajscy environments for business and entertainment. This chal- lenge is exacerbated by the amount of data

  12. Indexing and Fast Near-Matching of Billions of Astronomical Objects Bin Fu, Eugene Fink, Garth Gibson, and Jaime Carbonell

    E-Print Network [OSTI]

    . right ascension declination vernal equinox celestial equator south celestial pole north celestial pole

  13. DISC-SkyMap: Indexing and Retrieval of Celestial Objects Bin Fu, Tarush Aggarwal, Eugene Fink, Garth Gibson

    E-Print Network [OSTI]

    Fink, Eugene

    "): Angle from the celestial equator · Right ascension ("longitude"): Angle from the vernal equinox object, we need to identify the closest match (if any) right ascension decli- nation vernal equinox

  14. Thermoacoustic modeling and uncertainty analysis of two-dimensional conductive Jonghoon Bin, William S. Oates, and Kunihiko Taira

    E-Print Network [OSTI]

    Thermoacoustic modeling and uncertainty analysis of two-dimensional conductive membranes Jonghoon-dimensional model for thermoacoustic engines J. Acoust. Soc. Am. 111, 2076 (2002); 10.1121/1.1467675 [This article://scitation.aip.org/termsconditions. Downloaded to ] IP: 146.201.18.83 On: Fri, 13 Feb 2015 15:46:28 #12;Thermoacoustic modeling and uncertainty

  15. Bin BrookThe Magazine of robinson College, Cambridge L E n T 2 0 1 2

    E-Print Network [OSTI]

    Flynn, E. Victor

    Digging Around 2 A new image 4 Fellowship Profile 5 new Highs in Education 7 College Chaplaincy 9 Contents #12;Just Digging Around... Martine Gallie (1981, pictured right) read Archaeology and Anthropology for the association's image. i learned that, as well as patients,doctors are interested in money and golf. Despite

  16. Node Reclamation and Replacement for Long-lived Sensor Networks Bin Tong, Guiling Wang, Wensheng Zhang, and Chuang Wang

    E-Print Network [OSTI]

    Zhang, Wensheng

    @njit.edu Abstract--When deployed for long-term tasks, the energy required to support sensor nodes' activities is far is conserved, once the energy is used up, the network life terminates. Therefore, guaranteeing long- term of WSNs for long-term tasks such as structural health monitoring for bridges and tunnels, border

  17. Superdiffusion and Non-Gaussian Statistics in a Driven-Dissipative 2D Dusty Plasma Bin Liu and J. Goree

    E-Print Network [OSTI]

    Goree, John

    of electrons on a liquid helium surface [1], ions confined magnetically in a Penning trap [2], colloidal suspensions [3], vortex arrays in the mixed state of type- II superconductors [4], and dusty plasmas levitated of simple liquids. Experiments with 2D liquids are fewer, including soft matter systems such as colloidal

  18. Cooperative Bin-Picking with Time-of-Flight Camera and Impedance Controlled DLR Lightweight Robot III

    E-Print Network [OSTI]

    Blanz, Volker

    with sophisticated soft-robotics features. These robots will be able to serve as an uncaged co-worker for humans

  19. Opgave 1 20 Et bin rt tr med heltal i knuderne kan repr senteres som en v rdi af

    E-Print Network [OSTI]

    Brodal, Gerth Stølting

    Deltr s, t:Tree ! Bool der afg r, om s er et deltr af t. En naiv algoritme for dette problem er vil give en tidskompleksitet p Ojtjjsj. En smartere algoritme er kun at unders ge dette for de knuder lgende algoritme er gyldig og korrekt. Algoritme: Heltalskvadratrod Stimulans: n: n0 Respons: r: r2 n r

  20. nh Gi Tn Hi Ti Nguyn Thin Nhin do Trn Du Deep Horizon Khi phc b bin sng v cc

    E-Print Network [OSTI]

    cùng khu lân cn và vnh St. Louis, tt c nm ti ht Jackson, Harrison và Hancock, Mississippi. S Cht lng Truyn thông S Cht lng Môi trng Mississippi, PO 2261, Jackson, Mississippi 39225, Phone 601

  1. Computer aided surgical planning for congenital aural atresia Bin Li*, Dongqing Chen*, Eric Smouha**, andZhengrong Liang*

    E-Print Network [OSTI]

    . The system allows a 3-stage interactive planning in which positioning, marking and drilling simulates in surgical planning. Conventional two-dimensional (2D) CT demonstratesthe key anatomic structures, including

  2. Energy Consumption Simulation and Analysis of Heat Pump Air Conditioning System in Wuhan by the BIN Method 

    E-Print Network [OSTI]

    Wen, Y.; Zhao, F.

    2006-01-01

    to simulate the annual energy consumption of groundwater heat pump systems (GWHPS) for an office building in Wuhan. Its annual energy consumption was obtained and compared with the partner of the air source heat pump systems (ASHPS). The results show...

  3. Shear Viscosity of Two-Dimensional Yukawa Systems in the Liquid State Bin Liu and J. Goree

    E-Print Network [OSTI]

    Goree, John

    with liquids, including liquids near freezing, composed of molecules or particles that interact with a Yukawa a few reports of transport coef- ficients computed for 2D liquids using molecular dynamics (MD simulation uses an equilibrium method to calculate . Under equilibrium conditions, momentum transport arises

  4. frwebgate.access.gpo.gov/cgi-bin/getdoc.cgi?dbname=2008_register&docid=55825.pdf

    Energy Savers [EERE]

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on QA:QA J-E-1 SECTION J APPENDIX E LIST OFAMERICA'S FUTURE.EnergyWooden Rooftops |.doc&#0;8 I N S1-14 for Nuclear

  5. Roles for Wnts and their receptors in topographic mapping and laminar termination

    E-Print Network [OSTI]

    Richman, Alisha

    2011-01-01

    Zhang Y, Meister M, Sanes JR. Laminar restriction of retinalsemaphorin signaling controls laminar stratification in thesignaling in tectal laminar formation. CSH Meeting on Axon

  6. Updated Combination of Searches for the Standard Model Higgs Boson at the D0 Experiment in 9.7 fb-1 of Data

    E-Print Network [OSTI]

    D0 Collaboration

    2012-07-02

    Searches for standard model Higgs boson production at the D0 experiment in ppbar collisions at sqrt(s)=1.96 TeV are carried out for Higgs boson masses (m_H) in the range 100Higgs boson. In absence of a significant excess above the background expectation, 95% confidence level upper limits are set on the production cross section for a standard model Higgs boson. The upper limits are found to be a factor of 2.11 (0.73) times the predicted standard model cross section for m_H=115 (165) GeV. Under the background-only hypothesis, the corresponding expected limit is 1.46 (0.72) times the standard model prediction. At the same confidence level, these analyses exclude a standard model Higgs boson with a mass in the range 159

  7. Data:C2f657fb-1bf4-43a7-bab8-35adf4b59fa0 | Open Energy Information

    Open Energy Info (EERE)

    under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information...

  8. Data:Ffe2fb55-352f-473b-a2dd-50ae8b27f0a6 | Open Energy Information

    Open Energy Info (EERE)

    under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information 2. Demand 3. Energy << Previous 1 2 3 Next >> Basic Information...

  9. TECHNICAL PUBLICATIONS & BOOKS PRESENTED/PUBLISHED GOMES J.S. & ALVES, F.B. (2013): "The Universe of the Oil & Gas Industry From Exploration to Refining", 780

    E-Print Network [OSTI]

    Williams, John M.

    2013-01-01

    Universe of the Oil & Gas Industry ­ From Exploration to Refining", 780 pages University textbook published by PARTEX Oil & Gas, Lisbon, Portugal. ISBN 9789892037783. GOMES J.S. (2012): "New Technologies in the Oil and Gas Industry", edited by J.S. Gomes, published by INTECH open science (www

  10. Search for the standard model Higgs boson in ??+jets final states in 9.7??fb(?1) of pp-bar collisions with the D0 detector

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Chen, G.; Clutter, Justace Randall; Sekaric, Jadranka; Wilson, Graham Wallace; Abazov, V. M.; Abbinante, A.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.

    2013-09-17

    and expected background. We test our method by measuring WZ and ZZ production with Z?bb-bar and find production rates consistent with the standard model prediction. For a Higgs boson mass of 125 GeV, we set a 95% C.L. upper limit on the production of a standard...

  11. Search for the standard model Higgs boson in associated $WH$ production in 9.7 fb$^{-1}$ of $p\\bar{p}$ collisions with the D0 detector

    E-Print Network [OSTI]

    The D0 Collaboration

    2012-09-21

    We present a search for the standard model Higgs boson in final states with a charged lepton (electron or muon), missing transverse energy, and two or three jets, at least one of which is identified as a $b$-quark jet. The search is primarily sensitive to $WH\\to\\ell\

  12. CDF/PHYS/EXO/PUBLIC/10464 An inclusive search for new physics in like-sign dilepton events at CDF with 6.1 fb-1

    E-Print Network [OSTI]

    Quigg, Chris

    a search for new physics in events with two high pT leptons of the same electric charge using data the statistical consistency. Companion notes interpret the sample in terms of supersymmetry [7] and same-sign top quarks [8]. II. DATASET AND SELECTION Events were recorded by CDF II [9, 10], a general purpose detector

  13. Type B Accident Investigation Board Report on the September 1, 1999, Plutonium Intakes at the Savannah River Site FB-Line

    Office of Energy Efficiency and Renewable Energy (EERE)

    This report is an independent product of the Type B Accident Investigation Board appointed by Greg Rudy, Manager, Savannah River Operations Office, U.S. Department of Energy.

  14. Waste Stream Disposal Pharmacy Quick Sheet (6/16/14) Also pharmacy employees must complete SABA "Medication Waste Stream Disposal" Non-hazardous Hazardous Additional Waste

    E-Print Network [OSTI]

    Oliver, Douglas L.

    Additional Waste Disposal Location Green Bins for Non-hazardous waste Black Bins must complete SABA "Medication Waste Stream Disposal" Non-hazardous Hazardous for Hazardous Waste Yellow Trace Chemo Disposal Bin Red Sharps Bins Red

  15. Deploying Systems Interoperability and Customer Choice within Smart Grid

    E-Print Network [OSTI]

    Ghatikar, Girish

    2014-01-01

    twiki- sggrid/bin/view/SmartGrid/PriorityActionPlanssggrid/bin/view/SmartGrid/TTMeetingOnPriceCommunications The

  16. Evaluation of SCR and DOC/CPF Tech in Diesel Exhaust Emission Control to Meet U.S. Tier 2 Bin 5

    Broader source: Energy.gov [DOE]

    The continuous regeneration trap may cause irreversibly negative effects on the NOx removal efficiency of the SCR system.

  17. Cape Cod Times http://www.capecodonline.com/cgi-bin/print/printstory.cgi 1 of 5 6/28/2006 2:17 PM

    E-Print Network [OSTI]

    Bice, Karen L.

    on Cape Cod. The movie chronicles Gore's crusade to raise worldwide awareness about global warming on global warming requested by Congress last fall. The conclusions in the report are based on a broad review changes linked to volcanoes and the scientific work. Natural global warming occurs when carbon dioxide

  18. Non-linear adaptive robust control of electro-hydraulic systems driven by double-rod actuators BIN YAO{*. FANPING BU{ and GEORGE T. C. CHIU{

    E-Print Network [OSTI]

    Yao, Bin

    -linearities due to directional change of valve opening, friction and valve overlap. Aside from the non, directional change of valve opening, friction, and valve overlap. Aside from the non-linear nature uncertainties, such as the external disturbances, leakage, and friction, cannot be modelled exactly and the non

  19. A note on Hardy-Weinberg equilibrium of VNTR data by using the Federal Bureau of Investigation's fixed-bin method

    SciTech Connect (OSTI)

    Devlin, B.; Risch, N. )

    1992-09-01

    To fully utilize the information of VNTR data for forensic inference, the probability of observing the matching suspect and evidentiary profile in a reference population is estimated, usually by assuming independence of alleles within and between loci. This assumption has been challenged on the basis of the observation that there is frequently an excess of single-band phenotypes (SBP) in forensic data bases, which could indicate lack of independence. Nevertheless, another explanation is that the excess SBP are artifacts of laboratory methods. In this report the authors examine the excess of SBP for three VNTR loci studied by the FBI (D17S79 and D2S44, for blacks, and D14S13, for Caucasians). The FBI claims that the excess is due to the effect of null alleles; the null alleles are suspected to be small to be detected. The authors estimate the frequency of null alleles for two loci (D17S79 and D14A13) by comparing, for these loci, the data from the FBI data base and the data from the Lifecodes data base. These comparisons yield information on small fragments because Lifecodes uses the restriction enzyme PstI, which yields larger fragments than does HaeIII, which the FBI uses. For D17S19 in blacks, the authors estimate a null allele frequency of 4.4%, and, for D14S13 in Caucasians, they estimate a frequency of 3.0%. The null-allele frequency for D2S44 in blacks is derived similarly, again being based on analysis of DNA cut with HaeIII and PstI; the estimate of the null-allele frequency for this locus is 1.5%. Using these null-allele frequency estimates and a goodness-of-fit test, the authors show that there is no evidence for deviations from Hardy-Weinberg expectations of genotype probabilities at these loci. 20 refs., 1 fig.

  20. New Inorganic/Organic Coordination Polymers Generated from Bidentate Schiff-Base Yu-Bin Dong, Mark D. Smith, and Hans-Conrad zur Loye*

    E-Print Network [OSTI]

    zur Loye, Hans-Conrad

    ,5-bis(3-pyridyl)-3,4-diaza-2,4-hexadiene (L2) with cadmium and cobalt nitrate hydrates is investigated

  1. Opgave 1 (20%) Et bin#rt tr# med heltal i knuderne kan repr#senteres som en v#rdi af

    E-Print Network [OSTI]

    Brodal, Gerth Stølting

    #rdiprocedure: Proc Deltr#[s, t: Tree] ! (Bool) der afg#r, om s er et deltr# af t. En naiv algoritme for dette problem rod. Det vil give en tidskompleksitet p# O(jtjjsj). En smartere algoritme er kun at unders#ge dette, at f#lgende algoritme er gyldig og korrekt. Algoritme: Heltalskvadratrod Stimulans: n: nâ??0 Respons: r

  2. D n xut Khi phc Sm Giai on IV D n xut Khi phc loi ra bin sm s gip khi

    E-Print Network [OSTI]

    thc trong vùng Vnh tng lng cá th sng sót sau khi b choáng lnh và nhng ln mc cn nguy him. Gim bt nhm". Chng trình giám sát vic dùng li ánh bt tôm hin ti cn c m rng lng ngày giám sát mi nm i vi vic dùng li

  3. Bioconjugated Nanoparticles for DNA Protection from Cleavage Xiao-xiao He, Kemin Wang,* Weihong Tan, Bin Liu, Xia Lin, Chunmei He, Du Li,

    E-Print Network [OSTI]

    Tan, Weihong

    in water-in-oil microemulsion. Briefly, a well- distributed mixture of the two silanes (with volume ratio 1/Biosensing and Chemometrics, College of Chemistry & Chemical Engineering, Institute of Biological Technology, Hunan Uni and 4, plasmid DNA moved in the electric field, and amino-modified silica nanopar- ticles-plasmid DNA

  4. Ergebnisse des Data Mining Cups 2006 nach Hochschulen Datenquelle: http://www.prudsys.de/Service/Downloads/bin/1151676237/DMC2006_Ergebnisliste.pdf

    E-Print Network [OSTI]

    Keysers, Daniel

    Berlin 38 8 119.0 2893.2 139.0 2301.0 Hochschule Wismar 39 1 142.0 2256.0 142.0 2256.0 University 1 172.0 -2440.0 172.0 -2440.0 Johann-Wolfgang-Goethe-Universit¨at Frankfurt am Main Sortierung: Median Scoree zusammengestellt am 04.07.2006 von Daniel Keysers, http://www.iupr.org/~keysers #12;

  5. Contact Mechanics Based Mechanical Characterization of Portland Cement Paste 

    E-Print Network [OSTI]

    Jones, Christopher

    2012-02-14

    Current research interest in multi-scale modeling of cement paste requires accurate characterization of the time-dependent mechanical properties of the material, particularly the C-S-H phase. Nanoindentation is evaluated as a tool for measuring...

  6. A realistic molecular model of cement hydrates

    E-Print Network [OSTI]

    Ulm, Franz-Josef

    Despite decades of studies of calcium-silicate-hydrate (C-S-H), the structurally complex binder phase of concrete, the interplay between chemical composition and density remains essentially unexplored. Together these ...

  7. Development of an electronically tunable ultra-wideband radar imaging sensor and its components 

    E-Print Network [OSTI]

    Han, Jeongwoo

    2006-08-16

    and receiver respectively for timing control. A novel integrated CSH (Coupled-Slotline Hybrid)sampling mixer has been developed along with the design of the strobe pulse generator appropriate for the impulse radar system. The integrated sampling mixer has...

  8. Dynamic behavior of hydration water in calcium-silicate-hydrate gel: A quasielastic neutron scattering spectroscopy investigation

    E-Print Network [OSTI]

    Li, Hua

    The translational dynamics of hydration water confined in calcium-silicate-hydrate (C-S-H) gel was studied by quasielastic neutron scattering spectroscopy in the temperature range from 280 to 230 K. The stretch exponent ...

  9. Modeling of the Aging Viscoelastic Properties of Cement Paste Using Computational Methods 

    E-Print Network [OSTI]

    Li, Xiaodan

    2012-07-16

    Modeling of the time-dependent behavior of cement paste has always been a difficulty. In the past, viscoelastic behavior of cementitious materials has been primarily attributed to the viscoelastic properties of C-S-H ...

  10. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    Through observation of the samples after leaching, it was confirmed that ettringite precipitation increased as the dissolution of the portlandite and the C-S-H gel progressed. EPMA...

  11. Change in pore structure and composition of hardened cement paste...

    Office of Scientific and Technical Information (OSTI)

    Through observation of the samples after leaching, it was confirmed that ettringite precipitation increased as the dissolution of the portlandite and the C-S-H gel progressed. EPMA...

  12. Search for new physics in the dijet mass distribution using 1 fb[superscript ?1] of pp collision data at ?s = 7 TeV collected by the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    Invariant mass distributions of jet pairs (dijets) produced in LHC proton–proton collisions at a centre-of-mass energy ?s = 7 TeV have been studied using a data set corresponding to an integrated luminosity of 1.0 ...

  13. Search for a heavy gauge boson decaying to a charged lepton and a neutrino in 1 fb[superscript ?1] of pp collisions at ?s = 7 TeV using the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    The ATLAS detector at the LHC is used to search for high-mass states, such as heavy charged gauge bosons (W?), decaying to a charged lepton (electron or muon) and a neutrino. Results are presented based on the analysis of ...

  14. Search for the Standard Model Higgs boson in the decay channel H?ZZ(*)?4? with 4.8 fb[superscript -1] of pp collision data at ?s = 7 TeV with ATLAS

    E-Print Network [OSTI]

    Taylor, Frank E.

    This Letter presents a search for the Standard Model Higgs boson in the decay channel H?ZZ(*)??[superscript +]?[superscript ?]??[superscript +]??[superscript ?], where ?,?? = e or ?, using proton–proton collisions at ?s = ...

  15. Search for a standard model Higgs boson in the H?ZZ??[superscript +]?[subscript ?]?[bar over ?] decay channel using 4.7 fb[superscript -1] of ?s = 7 TeV data with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for a Standard Model Higgs boson decaying via H?ZZ??[superscript +]?[superscript ?]?[bar over ?], where ? represents electrons or muons, is presented. It is based on proton–proton collision data at ?s = 7 TeV, ...

  16. Data:B485777c-c4fb-42b3-8d2a-3da95f7c7c10 | Open Energy Information

    Open Energy Info (EERE)

    a-3da95f7c7c10 No revision has been approved for this page. It is currently under review by our subject matter experts. Jump to: navigation, search Loading... 1. Basic Information...

  17. Search for Direct Top Squark Pair Production in Final States with One Isolated Lepton, Jets, and Missing Transverse Momentum in ?s=7??TeV pp Collisions Using 4.7??fb[superscript -1] of ATLAS Data

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search is presented for direct top squark pair production in final states with one isolated electron or muon, jets, and missing transverse momentum in proton-proton collisions at ?s=7??TeV. The measurement is based on ...

  18. Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 4.7??fb?1 of ?s=7??TeV proton-proton collision data

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for squarks and gluinos in final states containing jets, missing transverse momentum and no high-pT electrons or muons is presented. The data represent the complete sample recorded in 2011 by the ATLAS experiment ...

  19. Search for neutral Higgs bosons in the multi-b -jet topology in 5.5 fb-1 of pp-bar collisions at sqrt(s)=1.96 TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Carrasco-Lizarraga, M. A.; Chen, G.; Clutter, Justace Randall; McGivern, Carrie Lynne; Sekaric, Jadranka; Wilson, Graham Wallace; D0 Collaboration; Abazov, V. M.; Abbott, B.; Acharya, B. S.; Adams, M.; Adams, T.; Alexeev, G. D.; Alkhazov, G.

    2011-04-04

    Data recorded by the D0 experiment at the Fermilab Tevatron Collider are analyzed to search for neutral Higgs bosons produced in association with b quarks. The search is performed in the three-b -quark channel using multijet-triggered events...

  20. California’s Energy Future: The View to 2050 - Summary Report

    E-Print Network [OSTI]

    Yang, Christopher

    2011-01-01

    and conventional biodiesel, thus bin 2 and bin 3 technologies such as cellulosic ethanol, renewable diesel and production of drop-in hydrocarbons

  1. California's Energy Future - The View to 2050

    E-Print Network [OSTI]

    2011-01-01

    and conventional biodiesel, thus bin 2 and bin 3 technologies such as cellulosic ethanol, renewable diesel and production of drop-in hydrocarbons

  2. California’s Energy Future: The View to 2050 - Summary Report

    E-Print Network [OSTI]

    Yang, Christopher

    2011-01-01

    ethanol and conventional biodiesel, thus bin 2 and bin 3cane, sugar beet, wheat) Biodiesel from oil crops (e.g. ,hydrocarbons) Algal biodiesel Improved enzymes, catalysts,

  3. California's Energy Future - The View to 2050

    E-Print Network [OSTI]

    2011-01-01

    ethanol and conventional biodiesel, thus bin 2 and bin 3cane, sugar beet, wheat) Biodiesel from oil crops (e.g. ,hydrocarbons) Algal biodiesel Improved enzymes, catalysts,

  4. SU-D-17A-04: The Impact of Audiovisual Biofeedback On Image Quality During 4D Functional and Anatomic Imaging: Results of a Prospective Clinical Trial

    SciTech Connect (OSTI)

    Keall, P; Pollock, S [University of Sydney, Sydney (Australia); Yang, J; Diehn, M; Berger, J; Graves, E; Loo, B [Stanford University, Stanford, CA (United States); Yamamoto, T [UC Davis School of Medicine, Sacramento, CA (United States)

    2014-06-01

    Purpose: The ability of audiovisual (AV) biofeedback to improve breathing regularity has not previously been investigated for functional imaging studies. The purpose of this study was to investigate the impact of AV biofeedback on 4D-PET and 4D-CT image quality in a prospective clinical trial. We hypothesized that motion blurring in 4D-PET images and the number of artifacts in 4D-CT images are reduced using AV biofeedback. Methods: AV biofeedback is a real-time, interactive and personalized system designed to help a patient self-regulate his/her breathing using a patient-specific representative waveform and musical guides. In an IRB-approved prospective clinical trial, 4D-PET and 4D-CT images of 10 lung cancer patients were acquired with AV biofeedback (AV) and free breathing (FB). The 4D-PET images in 6 respiratory bins were analyzed for motion blurring by: (1) decrease of GTVPET and (2) increase of SUVmax in 4-DPET compared to 3D-PET. The 4D-CT images were analyzed for artifacts by: (1) comparing normalized cross correlation-based scores (NCCS); and (2) quantifying a visual assessment score (VAS). A two-tailed paired t-test was used to test the hypotheses. Results: The impact of AV biofeedback on 4D-PET and 4D-CT images varied widely between patients, suggesting inconsistent patient comprehension and capability. Overall, the 4D-PET decrease of GTVPET was 2.0±3.0cm3 with AV and 2.3±3.9cm{sup 3} for FB (p=0.61). The 4D-PET increase of SUVmax was 1.6±1.0 with AV and 1.1±0.8 with FB (p=0.002). The 4D-CT NCCS were 0.65±0.27 with AV and 0.60±0.32 for FB (p=0.32). The 4D-CT VAS was 0.0±2.7 (p=ns). Conclusion: A 10-patient study demonstrated a statistically significant reduction of motion blurring of AV over FB for 1/2 functional 4D-PET imaging metrics. No difference between AV and FB was found for 2 anatomic 4D-CT imaging metrics. Future studies will focus on optimizing the human-computer interface and including patient training sessions for improved comprehension and capability. Supported by NIH/NCI R01 CA 093626, Stanford BioX Interdisciplinary Initiatives Program, NHMRC Australia Fellowship, and Kwanjeong Educational Foundation. GE Healthcare provided the Respiratory Gating Toolbox for 4D-PET image reconstruction. Stanford University owns US patent #E7955270 which is unlicensed to any commercial entity.

  5. News from the University of Hawaii 10-Campus System http://www.hawaii.edu/cgi-bin/uhnews?20060523162411 1 of 2 3/5/2008 12:34 PM

    E-Print Network [OSTI]

    Alam, Maqsudul

    in the College of Engineering on electromagnetics and wave propagation, including an ultra-wideband, low`i medical student Joseph Aoki received the Achievement Rewards for College Scientists­Honolulu Scholar honored at a recent ARCS-Honoloulu banquet. ARCS helps meet the country's need for scientists

  6. News from the University of Hawaii 10-Campus System http://www.hawaii.edu/cgi-bin/uhnews?20030520085516 1 of 1 3/5/2008 12:48 PM

    E-Print Network [OSTI]

    Alam, Maqsudul

    News from the University of Hawaii 10-Campus System http://www.hawaii Policy copyright ©2007 University of Hawai`i The University of Hawai`i is an Equal Opportunity Employer Quick links to campus homepages: Manoa | Hilo | West O`ahu | Hawai`i | Honolulu | Kapi`olani | Kaua

  7. Characterizing Offshore Earthquakes at Hawaii Recorded by the First... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 5/18/09 5:26 PM

    E-Print Network [OSTI]

    Laske, Gabi

    Characterizing Offshore Earthquakes at Hawaii Recorded by the First... http://www33B-1383 TI: Characterizing Offshore Earthquakes at Hawaii Recorded by the First PLUME Temporary Ocean-Bottom Seismometer Network AU: * Anchieta, M C EM: mariaa@hawaii.edu AF: University of Hawaii

  8. Body-wave tomography at Hawaii from the first PLUME deployment... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 5/18/09 5:25 PM

    E-Print Network [OSTI]

    Laske, Gabi

    Body-wave tomography at Hawaii from the first PLUME deployment... http://www33B-1380 TI: Body-wave tomography at Hawaii from the first PLUME deployment of ocean-bottom seismometers AU: * Wolfe, C J EM: cecily@soest.hawaii.edu AF: University of Hawaii at Manoa, 1680 East

  9. Mantle Anisotropy Beneath the Hawaiian Islands from Measurements... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 5/18/09 5:27 PM

    E-Print Network [OSTI]

    Laske, Gabi

    :27 PM west of Kauai to east of Hawaii. Ten portable land stations were operated for a period spanning: Wolfe, C J EM: cecily@soest.hawaii.edu AF: University of Hawaii at Manoa, 1680 East-West Road, Honolulu

  10. New Polymer Coatings Prevent Corrosion -Science: The Post Chro... http://www.postchronicle.com/cgi-bin/artman/exec/view.cgi?archive... 1 of 2 2/6/09 10:33 AM

    E-Print Network [OSTI]

    Braun, Paul

    New Polymer Coatings Prevent Corrosion - Science: The Post Chro... http://www Polymer Coatings Prevent Corrosion by Staff U.S. scientists say they are developing new polymer coatings researchers said applications for the coatings range from automotive paints and marine varnishes to the thick

  11. Kolmogorov Versus Iroshnikov-Kraichnan Spectra: Consequences for... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 1/31/08 1:23 PM

    E-Print Network [OSTI]

    Ng, Chung-Sang

    . In addition to a self-consistent treatment of pickup ions, we also include in our study the effects of finite AN: SH23A-1151 TI:Kolmogorov Versus Iroshnikov-Kraichnan Spectra: Consequences for Ion Heating phenomenology. Recent studies of a solar wind heating model based on Kolmogorov spectral scaling have produced

  12. 2006 LWS TR & T Solar Wind Focused Science Topic Team: The ... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 11/14/06 11:27 AM

    E-Print Network [OSTI]

    Ng, Chung-Sang

    2006 LWS TR & T Solar Wind Focused Science Topic Team: The ... http://www=ng HR: 0800h AN: SH11A-0371 TI: 2006 LWS TR & T Solar Wind Focused Science Topic Team: The Beginnings AU;2006 LWS TR & T Solar Wind Focused Science Topic Team: The ... http://www

  13. Random Scattering and Anisotropic Turbulence of Shear-Alfven Wa... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 1 3/10/05 11:44 AM

    E-Print Network [OSTI]

    Ng, Chung-Sang

    in the Solar Wind and the Interstellar Medium AU: Ng, C S EM: chung-sang-ng@uiowa.edu AF: The University in the interstellar medium and the solar wind. The model is motivated by observations that show significant deviations

  14. Kolmogorov Versus Iroshnikov-Kraichnan Spectra: Consequences for... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 1/31/08 1:23 PM

    E-Print Network [OSTI]

    Ng, Chung-Sang

    in the Solar Wind AU:* Ng, C EM:chung-sang.ng@unh.edu AF:Center for Integrated Computation and Analysis observed in the solar wind provides a strong, if indirect, observational constraint on the relevant phenomenology. Recent studies of a solar wind heating model based on Kolmogorov spectral scaling have produced

  15. Anisotropic MHD/EMHD Turbulence in the Solar Wind and the Inte... http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 1 3/10/05 11:25 AM

    E-Print Network [OSTI]

    Ng, Chung-Sang

    Anisotropic MHD/EMHD Turbulence in the Solar Wind and the Inte... http://www-0284 TI: Anisotropic MHD/EMHD Turbulence in the Solar Wind and the Interstellar Medium AU 03824 United States AB: The solar wind and the interstellar medium is permeated by large-scale magnetic

  16. Navigate to http://cris.csrees.usda.gov/cgi-bin/starfinder/0?path=crisassist.txt&id=anon&pass=&OK=OK 1. Select `Any' or specific project type (e.g. Multistate Projects)

    E-Print Network [OSTI]

    Watson, Craig A.

    . Enter Department prefix or CRIS project number (e.g. FLA-FOR) 3. Select status--hold `Ctrl' key--Select all except Terminated 4. Select 500 5. Hit `Search) change `Project Type' to Multistate 14. In `Term. Date' column, if project

  17. BGK Waves: Nonlinear Saturated States in Space Plasmas? http://www.agu.org/cgi-bin/SFgate/SFgate?language=English&verb... 1 of 2 1/31/08 1:23 PM

    E-Print Network [OSTI]

    Ng, Chung-Sang

    in the theory of Bernstein-Greene-Kruskal (BGK) waves, motivated by recent identifications of electrostatic solutions that depend only on energy do not exist [Phys. Rev. Lett., 95, 245004, 2005]. However, if there exists an ignorable coordinate and solutions depend on both energy and a constant of the motion

  18. 05/23/2006 08:53 PMInnovation & Technology News -Fusion reactor shows its metal -22/05/2006 Page 1 of 3http://abc.net.au/cgi-bin/common/printfriendly.pl?/science/news/tech/InnovationRepublish_1644106.htm

    E-Print Network [OSTI]

    Nature Physics. In fusion, atomic nuclei are fused together to release energy, as opposed to fission are rammed together to form the charged gas plasma, contained inside a doughnut-shaped chamber called

  19. ABQJOURNAL NORTH/OPINION: Obama Focusing on Wrong Energyhttp://www.abqjournal.com/cgi-bin/print_it.pl?page=/north/opinion/... 1 of 3 2/25/10 3:54 PM

    E-Print Network [OSTI]

    . · Clean coal is an unproven technology with potentially serious environmental problems Obama wisely stated that we should stimulate the economy by investing in clean energy technologies. Unfortunately, he then presented a list of four technologies that the lobbyists want him to support, rather than

  20. Page 1 of 4 http://frwebgate2.access.gpo.gov/cgi-bin/TEXTgate.cgi?WAISdocID=P7DWxT/1/1/0&WAISactio... 3/8/2011

    E-Print Network [OSTI]

    Bandettini, Peter A.

    -76] ======================================================================= DEPARTMENT OF HEALTH AND HUMAN SERVICES Office of the Secretary Annual Update of the HHS Poverty Guidelines of the Department of Health and Human Services (HHS) poverty guidelines to account for last calendar year's increase about poverty figures for immigration forms, the Hill-Burton Uncompensated Services Program

  1. INTERFACING AUTOCAD WITH MAGNETIC DESIGN

    E-Print Network [OSTI]

    Sorin, M.

    2010-01-01

    more procedures, namely, fbI, fbll, eatblank, car4str, andwritten by Michael Helm. fbI finds the next blank in theprocedures car4str, cdr4str, fbI, fbll, and eatblank (which

  2. California’s Energy Future: The View to 2050 - Summary Report

    E-Print Network [OSTI]

    Yang, Christopher

    2011-01-01

    offshore tur- bines ”Third generation” PV High-altitude wind Bin Natural Gas Storage Combustion turbine

  3. California's Energy Future - The View to 2050

    E-Print Network [OSTI]

    2011-01-01

    offshore tur- bines ”Third generation” PV High-altitude wind Bin Natural Gas Storage Combustion turbine

  4. Cleans UpUTS: Help Reduce Waste and Improve Recycling

    E-Print Network [OSTI]

    Tsang Wai Hung "Ivor"

    will need to take your garbage and food waste to the central bins. Food waste (such as tea bags, coffee grounds, fruit and vegetable peels, bread, meat and rice) will go into a green-lidded bin and general/photocopier). · Cleaners will empty all central red bins on a daily basis and green bins on a twice-daily basis. It doesn

  5. University, Introduction

    E-Print Network [OSTI]

    Anderson, Charles W.

    through bin then ``rolled'' so that air is forced downward. # Costs: # Fuel for burners. # Electricity

  6. BENCHMARKING THE ACCURACY OF INERTIAL SENSORS IN CELL PHONES

    E-Print Network [OSTI]

    An, Bin

    2012-01-01

    PHONES by Bin An Many ubiquitous computing applications relyfor a variety of ubiquitous computing applications. Perhaps

  7. Measurement of the top-quark mass in the fully hadronic decay channel from ATLAS data at ?s=7 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aad, G.; Abbott, B.; Abdallah, J.; Khalek, S. Abdel; Abdinov, O.; Aben, R.; Abi, B.; Abolins, M.; AbouZeid, O. S.; Abramowicz, H.; et al

    2015-04-23

    In this study, the mass of the top quark is measured in a data set corresponding to 4.6 fb-1 of proton–proton collisions with centre-of-mass energy ?s=7 TeV collected by the ATLAS detector at the LHC. Events consistent with hadronic decays of top–antitop quark pairs with at least six jets in the final state are selected. The substantial background from multijet production is modelled with data-driven methods that utilise the number of identified b-quark jets and the transverse momentum of the sixth leading jet, which have minimal correlation. The top-quark mass is obtained from template fits to the ratio of three-jetmore »to dijet mass. The three-jet mass is calculated from the three jets produced in a top-quark decay. Using these three jets the dijet mass is obtained from the two jets produced in the W boson decay. The top-quark mass obtained from this fit is thus less sensitive to the uncertainty in the energy measurement of the jets. A binned likelihood fit yields a top-quark mass of mt=175.1±1.4(stat.) ±1.2(syst.) GeV.« less

  8. Search for standard model Higgs boson production in association with a W boson using a matrix element technique at CDF in pp? collisions at ?s=1.96 TeV

    SciTech Connect (OSTI)

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; Artikov, A.; Asaadi, J.; Ashmanskas, W.; Auerbach, B.; Aurisano, A.; Azfar, F.; Badgett, W.; Bae, T.; Barbaro-Galtieri, A.; Barnes, V. E.; Barnett, B. A.; Barria, P.; Bartos, P.; Bauce, M.; Bedeschi, F.; Behari, S.; Bellettini, G.; Bellinger, J.; Benjamin, D.; Beretvas, A.; Bhatti, A.; Bisello, D.; Bizjak, I.; Bland, K. R.; Blumenfeld, B.; Bocci, A.; Bodek, A.; Bortoletto, D.; Boudreau, J.; Boveia, A.; Brigliadori, L.; Bromberg, C.; Brucken, E.; Budagov, J.; Budd, H. S.; Burkett, K.; Busetto, G.; Bussey, P.; Buzatu, A.; Calamba, A.; Calancha, C.; Camarda, S.; Campanelli, M.; Campbell, M.; Canelli, F.; Carls, B.; Carlsmith, D.; Carosi, R.; Carrillo, S.; Carron, S.; Casal, B.; Casarsa, M.; Castro, A.; Catastini, P.; Cauz, D.; Cavaliere, V.; Cavalli-Sforza, M.; Cerri, A.; Cerrito, L.; Chen, Y. C.; Chertok, M.; Chiarelli, G.; Chlachidze, G.; Chlebana, F.; Cho, K.; Chokheli, D.; Chung, W. H.; Chung, Y. S.; Ciobanu, C. I.; Ciocci, M. A.; Clark, A.; Clarke, C.; Compostella, G.; Convery, M. E.; Conway, J.; Corbo, M.; Cordelli, M.; Cox, C. A.; Cox, D. J.; Crescioli, F.; Cuevas, J.; Culbertson, R.; Dagenhart, D.; d’Ascenzo, N.; Datta, M.; de Barbaro, P.; Dell’Orso, M.; Demortier, L.; Deninno, M.; Devoto, F.; d’Errico, M.; Di Canto, A.; Di Ruzza, B.; Dittmann, J. R.; D’Onofrio, M.; Donati, S.; Dong, P.; Dorigo, M.; Dorigo, T.; Ebina, K.; Elagin, A.; Eppig, A.; Erbacher, R.; Errede, S.; Ershaidat, N.; Eusebi, R.; Farrington, S.; Feindt, M.; Fernandez, J. P.; Field, R.; Flanagan, G.; Forrest, R.; Frank, M. J.; Franklin, M.; Freeman, J. C.; Funakoshi, Y.; Furic, I.; Gallinaro, M.; Garcia, J. E.; Garfinkel, A. F.; Garosi, P.; Gerberich, H.; Gerchtein, E.; Giagu, S.; Giakoumopoulou, V.; Giannetti, P.; Gibson, K.; Ginsburg, C. M.; Giokaris, N.; Giromini, P.; Giurgiu, G.; Glagolev, V.; Glenzinski, D.; Gold, M.; Goldin, D.; Goldschmidt, N.; Golossanov, A.; Gomez, G.; Gomez-Ceballos, G.; Goncharov, M.; González, O.; Gorelov, I.; Goshaw, A. T.; Goulianos, K.; Grinstein, S.; Grosso-Pilcher, C.; Group, R. C.; Guimaraes da Costa, J.; Hahn, S. R.; Halkiadakis, E.; Hamaguchi, A.; Han, J. Y.; Happacher, F.; Hara, K.; Hare, D.; Hare, M.; Harr, R. F.; Hatakeyama, K.; Hays, C.; Heck, M.; Heinrich, J.; Herndon, M.; Hewamanage, S.; Hocker, A.; Hopkins, W.; Horn, D.; Hou, S.; Hughes, R. E.; Hurwitz, M.; Husemann, U.; Hussain, N.; Hussein, M.; Huston, J.; Introzzi, G.; Iori, M.; Ivanov, A.; James, E.; Jang, D.; Jayatilaka, B.; Jeon, E. J.; Jindariani, S.; Jones, M.; Joo, K. K.; Jun, S. Y.; Junk, T. R.; Kamon, T.; Karchin, P. E.; Kasmi, A.; Kato, Y.; Ketchum, W.; Keung, J.; Khotilovich, V.; Kilminster, B.; Kim, D. H.; Kim, H. S.; Kim, J. E.; Kim, M. J.; Kim, S. B.; Kim, S. H.; Kim, Y. K.; Kim, Y. J.; Kimura, N.; Kirby, M.; Klimenko, S.; Knoepfel, K.; Kondo, K.; Kong, D. J.; Konigsberg, J.; Kotwal, A. V.; Kreps, M.; Kroll, J.; Krop, D.; Kruse, M.; Krutelyov, V.; Kuhr, T.; Kurata, M.; Kwang, S.; Laasanen, A. T.; Lami, S.; Lammel, S.; Lancaster, M.; Lander, R. L.; Lannon, K.; Lath, A.; Latino, G.; LeCompte, T.; Lee, E.; Lee, H. S.; Lee, J. S.; Lee, S. W.; Leo, S.; Leone, S.; Lewis, J. D.; Limosani, A.; Lin, C.-J.; Lindgren, M.; Lipeles, E.; Lister, A.; Litvintsev, D. O.; Liu, C.; Liu, H.; Liu, Q.; Liu, T.; Lockwitz, S.; Loginov, A.; Lucchesi, D.; Lueck, J.; Lujan, P.; Lukens, P.; Lungu, G.; Lys, J.; Lysak, R.; Madrak, R.; Maeshima, K.; Maestro, P.; Malik, S.; Manca, G.; Manousakis-Katsikakis, A.; Margaroli, F.; Marino, C.; Martínez, M.; Mastrandrea, P.; Matera, K.; Mattson, M. E.; Mazzacane, A.; Mazzanti, P.; McFarland, K. S.; McIntyre, P.; McNulty, R.; Mehta, A.; Mehtala, P.; Mesropian, C.; Miao, T.; Mietlicki, D.; Mitra, A.; Miyake, H.; Moed, S.; Moggi, N.; Mondragon, M. N.; Moon, C. S.; Moore, R.; Morello, M. J.; Morlock, J.; Movilla Fernandez, P.; Mukherjee, A.; Muller, Th.; Murat, P.; Mussini, M.; Nachtman, J.; Nagai, Y.; Naganoma, J.; Nakano, I.; Napier, A.; Nett, J.; Neu, C.; Neubauer, M. S.; Nielsen, J.; Nodulman, L.; Noh, S. Y.; Norniella, O.; Oakes, L.; Oh, S. H.; Oh, Y. D.; Oksuzian, I.; Okusawa, T.; Orava, R.; Ortolan, L.; Pagan Griso, S.; Pagliarone, C.; Palencia, E.; Papadimitriou, V.; Paramonov, A. A.; Patrick, J.; Pauletta, G.; Paulini, M.; Paus, C.; Pellett, D. E.; Penzo, A.; Phillips, T. J.; Piacentino, G.; Pianori, E.; Pilot, J.; Pitts, K.; Plager, C.; Pondrom, L.; Poprocki, S.; Potamianos, K.; Prokoshin, F.; Pranko, A.; Ptohos, F.; Punzi, G.; Rahaman, A.; Ramakrishnan, V.; Ranjan, N.; Redondo, I.; Renton, P.; Rescigno, M.; Riddick, T.; Rimondi, F.; Ristori, L.; Robson, A.; Rodrigo, T.; Rodriguez, T.; Rogers, E.; Rolli, S.; Roser, R.; Ruffini, F.; Ruiz, A.; Russ, J.; Rusu, V.; Safonov, A.

    2012-04-01

    This paper presents a search for standard model Higgs boson production in association with a W boson using events recorded by the CDF experiment in a data set corresponding to an integrated luminosity of 5.6 fb?¹. The search is performed using a matrix element technique in which the signal and background hypotheses are used to create a powerful discriminator. The discriminant output distributions for signal and background are fit to the observed events using a binned likelihood approach to search for the Higgs boson signal. We find no evidence for a Higgs boson, and 95% confidence level (C.L.) upper limits are set on ?(pp??WH)×B(H?bb¯). The observed limits range from 3.5 to 37.6 relative to the standard model expectation for Higgs boson masses between mH=100 GeV/c² and mH=150 GeV/c². The 95% C.L. expected limit is estimated from the median of an ensemble of simulated experiments and varies between 2.9 and 32.7 relative to the production rate predicted by the standard model over the Higgs boson mass range studied.

  9. Measurement of the inclusive 3-jet production differential cross section in proton-proton collisions at 7 TeV and determination of the strong coupling constant in the TeV range

    SciTech Connect (OSTI)

    Khachatryan, Vardan

    2015-05-01

    This paper presents a measurement of the inclusive 3-jet production differential cross section at a proton-proton centre-of-mass energy of 7 TeV using data corresponding to an integrated luminosity of 5 fb$^{-1}$ collected with the CMS detector. The analysis is based on the three jets with the highest transverse momenta. The cross section is measured as a function of the invariant mass of the three jets in a range of 445-3270 GeV and in two bins of the maximum rapidity of the jets up to a value of 2. A comparison between the measurement and the prediction from perturbative QCD at next-to-leading order is performed. Within uncertainties, data and theory are in agreement. The sensitivity of the observable to parameters of the theory such as the parton distribution functions of the proton and the strong coupling constant $\\alpha_S$ is studied. A fit to all data points with 3-jet masses larger than 664 GeV gives a value of the strong coupling constant of $\\alpha_S(M_\\mathrm{Z})$ = 0.1171 $\\pm$ 0.0013 (exp) $^{+0.0073}_{-0.0047}$ (theo).

  10. Measurement of the inclusive 3-jet production differential cross section in proton-proton collisions at 7 TeV and determination of the strong coupling constant in the TeV range

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Khachatryan, Vardan

    2015-05-01

    This paper presents a measurement of the inclusive 3-jet production differential cross section at a proton-proton centre-of-mass energy of 7 TeV using data corresponding to an integrated luminosity of 5 fb$^{-1}$ collected with the CMS detector. The analysis is based on the three jets with the highest transverse momenta. The cross section is measured as a function of the invariant mass of the three jets in a range of 445-3270 GeV and in two bins of the maximum rapidity of the jets up to a value of 2. A comparison between the measurement and the prediction from perturbative QCD atmore »next-to-leading order is performed. Within uncertainties, data and theory are in agreement. The sensitivity of the observable to parameters of the theory such as the parton distribution functions of the proton and the strong coupling constant $\\alpha_S$ is studied. A fit to all data points with 3-jet masses larger than 664 GeV gives a value of the strong coupling constant of $\\alpha_S(M_\\mathrm{Z})$ = 0.1171 $\\pm$ 0.0013 (exp) $^{+0.0073}_{-0.0047}$ (theo).« less

  11. Search for Standard Model Higgs Boson Production in Association with a $W$ Boson Using a Matrix Element Technique at CDF in $p\\bar{p}$ Collisions at $\\sqrt{s} = 1.96$ TeV

    SciTech Connect (OSTI)

    Aaltonen, T.; Alvarez Gonzalez, B.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J.A.; Arisawa, T.; Artikov, A.; /Dubna, JINR /Texas A-M

    2011-12-01

    This paper presents a search for standard model Higgs boson production in association with a W boson using events recorded by the CDF experiment in a dataset corresponding to an integrated luminosity of 5.6 fb{sup -1}. The search is performed using a matrix element technique in which the signal and background hypotheses are used to create a powerful discriminator. The discriminant output distributions for signal and background are fit to the observed events using a binned likelihood approach to search for the Higgs boson signal. We find no evidence for a Higgs boson, and 95% confidence level (C.L.) upper limits are set on {sigma}(p{bar p} {yields} WH) x {Beta}(H {yields} b{bar b}). The observed limits range from 3.5 to 37.6 relative to the standard model expectation for Higgs boson masses between m{sub H} = 100 GeV/c{sup 2} and m{sub H} = 150 GeV/c{sup 2}. The 95% C.L. expected limit is estimated from the median of an ensemble of simulated experiments and varies between 2.9 and 32.7 relative to the production rate predicted by the standard model over the Higgs boson mass range studied.

  12. Measurement of the charge asymmetry in highly boosted top-quark pair production in $\\sqrt{s} =$ 8 TeV $pp$ collision data collected by the ATLAS experiment

    E-Print Network [OSTI]

    The ATLAS collaboration

    2015-01-01

    A measurement of the charge asymmetry reflecting the different rapidity distribution of top and anti-top quarks in the production of high invariant mass top-quark pairs is presented using 20.3 fb$^{-1}$ of $\\sqrt{s}$ = 8 TeV proton-proton collisions collected by the ATLAS experiment at the LHC. The analysis is based on an event reconstruction and selection criteria, specifically designed for highly boosted top quarks, that uses jet substructure to identify the top-quark candidate, which decays to a fully hadronic final state. The charge asymmetry in a fiducial region with large invariant mass of the top-quark pair ($m_{t\\bar{t}} > $ 0.75 TeV) and an absolute rapidity difference within -2 $< \\Delta |y| <$ 2 is measured to be 4.2 $\\pm$ 3.2%, in agreement with the Standard Model prediction at next-to-leading order. A differential measurement in three $t\\bar{t}$ mass bins is also presented.

  13. Search for standard model Higgs boson production in association with a W boson using a matrix element technique at CDF in pp? collisions at ?s=1.96 TeV

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aaltonen, T.; Álvarez González, B.; Amerio, S.; Amidei, D.; Anastassov, A.; Annovi, A.; Antos, J.; Apollinari, G.; Appel, J. A.; Arisawa, T.; et al

    2012-04-02

    This paper presents a search for standard model Higgs boson production in association with a W boson using events recorded by the CDF experiment in a data set corresponding to an integrated luminosity of 5.6 fb?¹. The search is performed using a matrix element technique in which the signal and background hypotheses are used to create a powerful discriminator. The discriminant output distributions for signal and background are fit to the observed events using a binned likelihood approach to search for the Higgs boson signal. We find no evidence for a Higgs boson, and 95% confidence level (C.L.) upper limitsmore »are set on ?(pp??WH)×B(H?bb¯). The observed limits range from 3.5 to 37.6 relative to the standard model expectation for Higgs boson masses between mH=100 GeV/c² and mH=150 GeV/c². The 95% C.L. expected limit is estimated from the median of an ensemble of simulated experiments and varies between 2.9 and 32.7 relative to the production rate predicted by the standard model over the Higgs boson mass range studied.« less

  14. Measurement of three-jet production cross-sections in pp collisions at 7 TeV centre-of-mass energy using the ATLAS detector

    E-Print Network [OSTI]

    ATLAS Collaboration

    2015-05-26

    Double-differential three-jet production cross-sections are measured in proton-proton collisions at a centre-of-mass energy of $\\sqrt{s} = 7$ TeV using the ATLAS detector at the Large Hadron Collider. The measurements are presented as a function of the three-jet mass $(m_{jjj})$, in bins of the sum of the absolute rapidity separations between the three leading jets $(|Y^\\ast|)$. Invariant masses extending up to 5 TeV are reached for $8integrated luminosity of 4.51 fb$^{-1}$. Jets are identified using the anti-$k_t$ algorithm with two different jet radius parameters, R=0.4 and R=0.6. The dominant uncertainty in these measurements comes from the jet energy scale. Next-to-leading-order QCD calculations corrected to account for non-perturbative effects are compared to the measurements. Good agreement is found between the data and the theoretical predictions based on most of the available sets of parton distribution functions, over the full kinematic range, covering almost seven orders of magnitude in the measured cross-section values.

  15. Measurement of the double differential diject mass cross section in pp(bar) collisions at sqrt(s) = 1.96 TeV

    SciTech Connect (OSTI)

    Rominsky, Mandy Kathleen; /Oklahoma U.

    2009-07-01

    This thesis presents the analysis of the double differential dijet mass cross section, measured at the D0 detector in Batavia, IL, using p{bar p} collisions at a center of mass energy of {radical}s = 1.96 TeV. The dijet mass was calculated using the two highest p{sub T} jets in the event, with approximately 0.7 fb{sup -1} of data collected between 2004 and 2005. The analysis was presented in bins of dijet mass (M{sub JJ}) and rapidity (y), and extends the measurement farther in M{sub JJ} and y than any previous measurement. Corrections due to detector effects were calculated using a Monte Carlo simulation and applied to data. The errors on the measurement consist of statistical and systematic errors, of which the Jet Energy Scale was the largest. The final result was compared to next-to-leading order theory and good agreement was found. These results may be used in the determination of the proton parton distribution functions and to set limits on new physics.

  16. Factors affecting the porridge quality of sorghum and pearl millet 

    E-Print Network [OSTI]

    Kante, Assa

    1987-01-01

    kernels were Dorado, SC303, and SC283 with a hardness index of 92. 0X, 91. 3X, and 91. 0X, respectively; the softest cultivar was SC90 (58. 7X). Den- sity was significantly correlated with grain hardness (r=0. 61, Table Bl). Endosperm texture ranged... Presence of Teste Endosperm Textureb Density (gm/cc)c Hardness Indexc Hilling Yieldc 083541 Tx430 CSH63e CSH63d 0265-14 SC170 083541 TAH428 80265 80283 80296 80253 80261 SC90 ATx623 e BTx623 SSS610 ATx623 80605 80303 Dorado...

  17. FM File Manager Page 1 Revision 1.0 COPYRIGHT (C) 1982 BY LOGICAL SYSTEMS, INC.

    E-Print Network [OSTI]

    Mann, Tim

    ) ....................................... 9 28 FB (Use Flag Bit) .................................. 9 28 CFB (Clear Flag Bit

  18. Canting in polarization plane Backscattering

    E-Print Network [OSTI]

    Zhang, Guifu

    " % & ' ( ) * ! A = cos2 " + sin2 # sin2 "! = Afa + Bfb ( fa " fb ) BC ( fa " fb ) BC Cfb + Dfa # $ % & ' ( ! B = cos2 " + sin2 # sin2 " ! = Afa + Bfb ( fa " fb ) BC ( fa " fb ) BC Cfb + Dfa # $ % & ' ( ! B = cos2 " sin2 · Gaussian pdf Statistical polarization signatures ! fhh 2 = Afa + Bfb( ) Afa * + Bfb * ( ) ! p(",#) = p

  19. Sr radionuclide in cement: An atomistic modeling study Mostafa Youssef a

    E-Print Network [OSTI]

    Yildiz, Bilge

    Docking 90 Sr radionuclide in cement: An atomistic modeling study Mostafa Youssef a , Roland J: Available online xxxx Keywords: Molecular simulation Cement Nuclear waste storage Mechanical properties a b crystalline analog, the 9 Å-tobermorite. C­S­H is the major binding phase of cement. Strontium was shown

  20. Conventional sawing window Earlysawing

    E-Print Network [OSTI]

    . The concrete is plastic. · During dormancy, as silicates (alite [C3 S] and belite [C2 S]) slowly dissolve-saturated with calcium ions (from dissolving alite [C3 S] primarily), fiber-like C-S-H and crystalline CH start to form with development of the air-void system. That is because high LOI fly ashes contain unburned carbon that absorbs

  1. CaCl 2 -Accelerated Hydration of Tricalcium Silicate: A STXM Study Combined with 29 Si MAS NMR

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Li, Qinfei; Ge, Yong; Geng, Guoqing; Bae, Sungchul; Monteiro, Paulo J. M.

    2015-01-01

    The effect of calcium chloride (CaCl 2 ) on tricalcium silicate (C 3 S) hydration was investigated by scanning transmission X-ray microscopy (STXM) with Near Edge X-ray Absorption Fine Structure (NEXAFS) spectra and 29 Si MAS NMR. STXM is demonstrated to be a powerful tool for studying the chemical composition of a cement-based hydration system. The Ca L 3,2 -edge NEXAFS spectra obtained by examining C 3 S hydration in the presence of CaCl 2 showed that this accelerator does not change the coordination of calcium in the calcium silicate hydrate (C-S-H), which is the primary hydration product. Omore »K-edge NEXAFS is also very useful in distinguishing the chemical components in hydrated C 3 S. Based on the Ca L 3,2 -edge spectra and chemical component mapping, we concluded that CaCl 2 prefers to coexist with unhydrated C 3 S instead of C-S-H. In Si K-edge NEXAFS analysis, CaCl 2 increases the degree of silicate polymerization of C-S-H in agreement with the 29 Si CP/MAS NMR results, which show that the presence of CaCl 2 in hydrated C 3 S considerably accelerates the formation of middle groups ( Q 2 ) and branch sites ( Q 3 ) in the silicate chains of C-S-H gel at 1-day hydration. « less

  2. R. Dale et al. (Eds.): IJCNLP 2005, LNAI 3651, pp. 357 365, 2005. Springer-Verlag Berlin Heidelberg 2005

    E-Print Network [OSTI]

    Heidelberg 2005 Finding Taxonomical Relation from an MRD for Thesaurus Extension SeonHwa Choi and HyukRo Park-757, Korea csh123@dreamwiz.com, hyukro@chonnam.ac.kr Abstract. Building a thesaurus is very costly and time-consuming task. To alleviate this problem, this paper proposes a new method for extending a thesaurus by adding

  3. Synthesis and characterization of hafnium and molybdenum bifunctional initiators for the preparation of triblock copolymers

    E-Print Network [OSTI]

    Gabert, Andrea Jennifer

    2007-01-01

    Chapter 1. Three monofunctional mixed alkyl hafnium complexes containing the (MesNpy)2 ligand ([(MesitylNCH2)2CMe(2-CsH4N)]2) were synthesized. (MesNpy)Hf(Neo)R ((2b), R = Me; Neo = CH2CMe2Ph) and (MesNpy)Hf(CH2TMS)(R), ...

  4. Effect of temperature on the hydration of Portland cement blended with siliceous fly ash

    SciTech Connect (OSTI)

    Deschner, Florian; Lothenbach, Barbara; Winnefeld, Frank; Neubauer, Jürgen

    2013-10-15

    The effect of temperature on the hydration of Portland cement pastes blended with 50 wt.% of siliceous fly ash is investigated within a temperature range of 7 to 80 °C. The elevation of temperature accelerates both the hydration of OPC and fly ash. Due to the enhanced pozzolanic reaction of the fly ash, the change of the composition of the C–S–H and the pore solution towards lower Ca and higher Al and Si concentrations is shifted towards earlier hydration times. Above 50 °C, the reaction of fly ash also contributes to the formation of siliceous hydrogarnet. At 80 °C, ettringite and AFm are destabilised and the released sulphate is partially incorporated into the C–S–H. The observed changes of the phase assemblage in dependence of the temperature are confirmed by thermodynamic modelling. The increasingly heterogeneous microstructure at elevated temperatures shows an increased density of the C–S–H and a higher coarse porosity. -- Highlights: •The reaction of quartz powder at 80 °C strongly enhances the compressive strength. •Almost no strength increase of fly ash blended OPC at 80 °C was found after 2 days. •Siliceous hydrogarnet is formed upon the reaction of fly ash at high temperatures. •Temperature dependent change of the system was simulated by thermodynamic modelling. •Destabilisation of ettringite above 50 °C correlates with sulphate content of C–S–H.

  5. A nanoscale numerical model of calcium silicate hydrate P.C. Fonseca a,

    E-Print Network [OSTI]

    Andrade, Jose

    to pre- dict the bulk properties of cement and concrete, such as shrinkage, creep, permeability and the properties of structural concrete are not fully under- stood. Models are becoming increasingly important, and cracking. C­S­H is responsible for much of the cohesive proper- ties in concrete but the chemical origin

  6. OpenADR Advances

    E-Print Network [OSTI]

    Holmberg, David G.

    2014-01-01

    twiki-­? sggrid/bin/view/SmartGrid/WebHome.   13. NIST  at:   http://www.nist.gov/smartgrid/upload/NIST_Framework_sggrid/bin/view/SmartGrid/SGIPCatalogOfStandards.     19.

  7. Stat.3 (Statistische Synopse): bersicht ber die Standard-Methoden Wahrscheinlichkeits-Verteilungen

    E-Print Network [OSTI]

    . Hierzu plotten wir jeweils #12;2 Diskretes Histogramm Mit dem MATLAB-Befehl Anz=hist(spike,max(spike)/bin); zählen wir die Spikezahlen pro bin und können dafür das empirische Histogramm ausgeben: hist(Anz,15) Zum

  8. Supplementary material for "Does the size distribution of mineral dust aerosols depend on the wind speed at emission?"

    E-Print Network [OSTI]

    Meskhidze, Nicholas

    Supplementary material for "Does the size distribution of mineral dust aerosols depend on the wind by truncating those bins. I do so by assuming that the sub-bin distribution follows the power law found by both

  9. Breaking the Curse of Cardinality on Bitmap Indexes

    E-Print Network [OSTI]

    Wu, Kesheng

    2008-01-01

    and query processing costs of binned indexes with OrBiC. Ourquery processing cost of the projection index is always Nof our binned index with OrBiC costs less than 4 × 10 8

  10. IC performance prediction system 

    E-Print Network [OSTI]

    Ramakrishnan, Venkatakrishnan

    1996-01-01

    In a mixed-product semiconductor foundry, optimization of product binning, packaging, product quantity control and rapid problem diagnosis are all critical to economic success. Binning is the placement of chips into several different specification...

  11. Evaluation of SCR and DOC/CPF Tech in Diesel Exhaust Emission...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Control to Meet U.S. Tier 2 Bin 5 Evaluation of SCR and DOCCPF Tech in Diesel Exhaust Emission Control to Meet U.S. Tier 2 Bin 5 The continuous regeneration trap may cause...

  12. H2 Internal Combustion Engine Research Towards 45% efficiency...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Internal Combustion Engine Research Towards 45% efficiency and Tier2-Bin5 emissions H2 Internal Combustion Engine Research Towards 45% efficiency and Tier2-Bin5 emissions 2009 DOE...

  13. Werkcollege from 23 September Astronomial databases -SDSS CasJobs

    E-Print Network [OSTI]

    Peletier, Reynier

    Brinchmann, Leiden Observatory for IAC 2010 Modern Data Mining and Virtual Observatory 1 Astronomical and bin this in bins of 0.2 in feha. The metal abundance that you find is the logarithm of the iron (Fe

  14. Optimization of Engine-out Emissions from a Diesel Engine to...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Engine-out Emissions from a Diesel Engine to Meet Tier 2 Bin 5 Emission Limits Optimization of Engine-out Emissions from a Diesel Engine to Meet Tier 2 Bin 5 Emission Limits...

  15. The economics of cell phone reuse and recycling

    E-Print Network [OSTI]

    Geyer, Roland; Doctori Blass, Vered

    2010-01-01

    from drop-off bins to prepaid envelopes or boxes. There areindividual shipping, such as prepaid shipping envelopes. The

  16. California's Energy Future - The View to 2050

    E-Print Network [OSTI]

    2011-01-01

    Energy System Component Analysis Bin Wind Onshore, shallow offshorewind, solar, biomass, geothermal, hydro, and marine energy offshore.

  17. Minimizing Mould Growth in Cold Rooms Why does mould growth occur in Cold Rooms?

    E-Print Network [OSTI]

    Chan, Hue Sun

    , textiles, or other porous materials inside the cold room. Styrofoam is okay. Store files in plastic bins

  18. California's Energy Future - The View to 2050

    E-Print Network [OSTI]

    2011-01-01

    Floating (deepwater) offshore tur- bines ”Third generation” PV High-altitude wind Bin Natural Gas Storage Combustion turbine

  19. California’s Energy Future: The View to 2050 - Summary Report

    E-Print Network [OSTI]

    Yang, Christopher

    2011-01-01

    Floating (deepwater) offshore tur- bines ”Third generation” PV High-altitude wind Bin Natural Gas Storage Combustion turbine

  20. Long-Term Planning for Nuclear Energy Systems Under Deep Uncertainty

    E-Print Network [OSTI]

    Kim, Lance Kyungwoo

    2011-01-01

    NUCLEAR ENERGY SYSTEM MODEL of the interim storage bin, the inventory of an isotope depends on the contribution

  1. MsatAllele notes MsatAllele_1.02 R package

    E-Print Network [OSTI]

    Borges, Rita

    MsatAllele notes MsatAllele_1.02 R package To visualize the scoring and binning of microsatelliteAllele is an R package intended to help the visualization and binning of scored microsatellite fragment sizes need to be binned to integer codes). The packages performs several data manipulations on an R data base

  2. Cost Sharing What is Cost Sharing?

    E-Print Network [OSTI]

    California at San Diego, University of

    into COEUS x OPAFS establishes project related IFIS fund and index numbers x Department tracks cost sharing sharing using various data fields (bin, fund, PI, index, etc.) x Create a Bin Generate a bin where cost1 Cost Sharing What is Cost Sharing? x Cost sharing is a commitment to use university resources

  3. The Annals of Applied Probability 2005, Vol. 15, No. 3, 17331764

    E-Print Network [OSTI]

    that there are n bins, and balls arrive in a Poisson process at rate n, where > 0 is a constant. Upon arrival independent exponential lifetimes with unit mean. We show that the system converges rapidly to its equilibrium "immigration­death" balls-and- bins model. We concentrate on the maximum bin load, which may be the quantity

  4. 10/1/2014 Micro-windmill research encourages innovation -The Shorthorn : News http://www.theshorthorn.com/news/micro-windmill-research-encourages-innovation/article_d477da18-48fb-11e4-a7ee-001a4bcf6878.html?mode=print 1/2

    E-Print Network [OSTI]

    Chiao, Jung-Chih

    microns and a diameter of 1.8 millimeters, the micro-windmill has the potential capacity to power cellphones and wireless sensors in ways solar energy cannot. The diameter of a strand of human hair is about

  5. 2/1/2014 Tinywindmills mayone daypower cell phones http://www.eetindia.co.in/articleLogin.do?artId=8800694132&fromWhere=/ART_8800694132_1800008_NT_36244fb4.HTM&catId=1800008&newsType=NT&pag... 1/3

    E-Print Network [OSTI]

    Chiao, Jung-Chih

    of the University of Texas created what is said to be the world's smallest wind turbine that could one day power. *Verify code: Power/Alternative Energy Tiny windmills may one day power cell phones KeywordsA, linear regulator Micropower 3-Sensor Combination Including Acceleration and Temperature Whitepaper SAS

  6. Combining weak-lensing tomography and spectroscopic redshift surveys

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Cai, Yan -Chuan; Bernstein, Gary

    2012-05-11

    Redshift space distortion (RSD) is a powerful way of measuring the growth of structure and testing General Relativity, but it is limited by cosmic variance and the degeneracy between galaxy bias b and the growth rate factor f. The cross-correlation of lensing shear with the galaxy density field can in principle measure b in a manner free from cosmic variance limits, breaking the f-b degeneracy and allowing inference of the matter power spectrum from the galaxy survey. We analyze the growth constraints from a realistic tomographic weak lensing photo-z survey combined with a spectroscopic galaxy redshift survey over the samemore »sky area. For sky coverage fsky = 0.5, analysis of the transverse modes measures b to 2-3% accuracy per ?z = 0.1 bin at z –2 are measured in the lensing survey and all halos with M > Mmin = 1013h–1M? have spectra. For the gravitational growth parameter parameter ? (f = ??m), combining the lensing information with RSD analysis of non-transverse modes yields accuracy ?(?) ? 0.01. Adding lensing information to the RSD survey improves \\sigma(\\gamma) by an amount equivalent to a 3x (10x) increase in RSD survey area when the spectroscopic survey extends down to halo mass 1013.5 (1014) h–1 M?. We also find that the ?(?) of overlapping surveys is equivalent to that of surveys 1.5-2 times larger if they are separated on the sky. This gain is greatest when the spectroscopic mass threshold is 1013 -1014 h–1 M?, similar to LRG surveys. The gain of overlapping surveys is reduced for very deep or very shallow spectroscopic surveys, but any practical surveys are more powerful when overlapped than when separated. As a result, the gain of overlapped surveys is larger in the case when the primordial power spectrum normalization is uncertain by > 0.5%.« less

  7. Search for R-Parity Violating Decays of Sneutrinos to e?, ??, and e? Pairs in pp? Collisions at ?s=1.96??TeV

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We present a search for supersymmetric neutrino ?˜ production using the Tevatron pp? collision data collected with the CDF II detector and corresponding to an integrated luminosity of 1??fb-1 [fb superscript -1]. We focus ...

  8. RoboCup 2004 Thomas Rofer

    E-Print Network [OSTI]

    Stryk, Oskar von

    RoboCup 2004 Thomas R¨ofer Tim Laue Center for Computing Technology, FB 3 Informatik, Universit Stefan Uhrig Fachgebiet Simulation und Systemoptimierung, FB 20 Informatik, Technische Universit

  9. HORTSCIENCE 47(3):391394. 2012. Fruit Phosphorous and Nitrogen

    E-Print Network [OSTI]

    Crisosto, Carlos H.

    browning, total phenolic concentration, postharvest consumer quality Abstract. Fruit flesh browning (FB activity, polyphenol oxidase activity, total phenolics, and fruit FB potential were evaluated. Nutrient of oxidative degradation of pheno- lic compounds by polyphenol oxidase (PPO), which leads to production

  10. Protist, Vol. 162, 8599, January 2011 http://www.elsevier.de/protis

    E-Print Network [OSTI]

    Katz, Laura

    Program in Organismic and Evolutionary Biology, University of Massachusetts, Amherst, MA 01003, USA bFB Organismische

  11. Mathematiques Projective modules in the intersection cohomology

    E-Print Network [OSTI]

    Malle, Gunter

    Germain, 5 rue Thomas Mann, 75205 Paris CEDEX 13, France. bFB Mathematik, TU Kaiserslautern, Postfach 3049

  12. ELSEVIER PIh S0032-3861(97)10388-3 Polymer Vol. 39 No. 17, pp. 4081-4088, 1998

    E-Print Network [OSTI]

    North Texas, University of

    , University of North Texas, Denton, TX 76203-5308, USA bFB-6, Physical Chemistry, Gerhard Mercator University

  13. Realizability Models Refuting Ishihara's Boundedness Peter Lietza

    E-Print Network [OSTI]

    Haller-Dintelmann, Robert

    Nordendstr. 11, D-60318 Frankfurt, Germany bFB4 Mathematik, TU Darmstadt, Schloßgartenstr. 7, D-64289 Darmstadt

  14. Boundary Forces in lattice Boltzmann: Analysis of Momentum Exchange algorithm

    E-Print Network [OSTI]

    a Michael Junk b a Fraunhofer ITWM, Fraunhofer-Platz 1 D-67663, Kaiserslautern, Germany bFB Mathematik und

  15. 9/25/13 Big Red & Shiny: Bringing the War Home: Omer Fast's "5,000 Feet Is the Best" www.bigredandshiny.com/cgi-bin/BRS.cgi?section=article&issue=BLOG&article=2013-08-25-050938356596801456&printView=true 1/2

    E-Print Network [OSTI]

    Snider, Barry B.

    Force Predator Drone operator, reclining on a bed in a Las Vegas hotel room. He is being interviewed by a journalist, but not a real journalist. And he isn't really a retired drone pilot either. He's an actor. We place. His interviews with the actual drone operator provide a narrative backbone onto which are hooked

  16. arXiv:1109.0460v2[hep-ph]10Jul2012 SU(3) breaking corrections to the D, D

    E-Print Network [OSTI]

    Weise, Wolfram

    ¨unchen, D-85747 Garching, Germany 2 School of Physics and Nuclear Energy Engineering, Beihang University can predict quantitatively the ratios of fD s /fD , fBs /fB, and fB s /fB taking into account heavy should be testable in future lattice QCD simula- tions, providing a stringent test of our understanding

  17. NOx reduction with the use of feedlot biomass as a reburn fuel 

    E-Print Network [OSTI]

    Goughnour, Paul Gordon

    2009-05-15

    composted FB (LA PC FB) with equivalence ratio ranging from 1 to 1.15. The results of these experiments show that NOx levels can be reduced by as much as 90% - 95 % when firing pure LA PC FB and results are almost independent of. The reburn fuel was injected...

  18. Attitudes and Experiences of Dental Hygiene Faculty Regarding Interactions with Current Undergraduate Dental Hygiene Students on Facebook 

    E-Print Network [OSTI]

    Wyatt, Leigh A

    2014-11-24

    Facebook (FB) currently boasts over 1 billion active monthly users. Forty-eight percent of 18-43 year olds access FB when they wake up; furthermore, since the end of 2012, the number of FB users ages 45-54 increased 45%. It is no surprise, then...

  19. Thermodynamics and cement science

    SciTech Connect (OSTI)

    Damidot, D.; Lothenbach, B.; Herfort, D.; Glasser, F.P.

    2011-07-15

    Thermodynamics applied to cement science has proved to be very valuable. One of the most striking findings has been the extent to which the hydrate phases, with one conspicuous exception, achieve equilibrium. The important exception is the persistence of amorphous C-S-H which is metastable with respect to crystalline calcium silicate hydrates. Nevertheless C-S-H can be included in the scope of calculations. As a consequence, from comparison of calculation and experiment, it appears that kinetics is not necessarily an insuperable barrier to engineering the phase composition of a hydrated Portland cement. Also the sensitivity of the mineralogy of the AFm and AFt phase compositions to the presence of calcite and to temperature has been reported. This knowledge gives a powerful incentive to develop links between the mineralogy and engineering properties of hydrated cement paste and, of course, anticipates improvements in its performance leading to decreasing the environmental impacts of cement production.

  20. New insights into water bonding during early tricalcium silicate hydration with quasielastic neutron scattering

    SciTech Connect (OSTI)

    Gutberlet, T., E-mail: gutberlet@cbm.bv.tum.de [Centre for Building Materials (CBM), Technische Universität München, Baumbachstraße 7, 81245 Munich (Germany); Hilbig, H.; Beddoe, R.E. [Centre for Building Materials (CBM), Technische Universität München, Baumbachstraße 7, 81245 Munich (Germany)] [Centre for Building Materials (CBM), Technische Universität München, Baumbachstraße 7, 81245 Munich (Germany); Lohstroh, W. [Forschungs-Neutronenquelle Heinz Maier-Leibnitz (FRM II), Technische Universität München, Lichtenbergstraße 1, 85748 Garching (Germany)] [Forschungs-Neutronenquelle Heinz Maier-Leibnitz (FRM II), Technische Universität München, Lichtenbergstraße 1, 85748 Garching (Germany)

    2013-09-15

    New information on the water bonding during the first 36 h of hydration of tricalcium silicate was obtained using the high neutron flux at the sample position of the time-of-flight spectrometer (TOFTOF), FRM II in Garching, Germany, together with {sup 29}Si NMR and X-ray diffraction measurements. A rapid increase in the amount of constrained water was observed at the beginning of the induction period. This is attributed to the formation of an early C-S-H with a large specific surface area (around 800 m{sup 2}/g). During subsequent hydration, the amount of constrained water, as given by the total surface area of the hydration products, is controlled by (a) the formation of new metastable early C-S-H which increases total surface area and (b) polymerisation processes which reduce total surface area. The relative contribution of these processes varies during hydration.

  1. Pushing schedule derivation method

    SciTech Connect (OSTI)

    Henriquez, B. [Compania Siderurgica Huachipato S.A., Talcahuano (Chile)

    1996-12-31

    The development of a Pushing Schedule Derivation Method has allowed the company to sustain the maximum production rate at CSH`s Coke Oven Battery, in spite of having single set oven machinery with a high failure index as well as a heat top tendency. The stated method provides for scheduled downtime of up to two hours for machinery maintenance purposes, periods of empty ovens for decarbonization and production loss recovery capability, while observing lower limits and uniformity of coking time.

  2. Peromyscus perfulvus (Rodentia: Cricetidae) CORNELIO SA NCHEZ-HERNA NDEZ, GARY D. SCHNELL, AND MARIA DE LOURDES ROMERO-ALMARAZ

    E-Print Network [OSTI]

    Hayssen, Virginia

    Nacional Auto´noma de Me´xico, A.P. 70-153, Coyoaca´n, Me´xico, Distrito Federal, 04510, Me´xico (CS-H) Sam 73072, USA; gschnell@ou.edu (GDS) Escuinapa No. 92 bis. Col. Pedregal de Santo Domingo, C.P. 04360, Me´xico, Distrito Federal, Me´xico (MLR-A) Abstract: Peromyscus perfulvus Osgood, 1945, is a medium-sized rodent

  3. Incorporation of reactive magnesia and quicklime in sustainable binders for soil stabilisation

    E-Print Network [OSTI]

    Gu, Kai; Jin, Fei; Al-Tabbaa, Abir; Shi, Bin; Liu, Chun; Gao, Lei

    2015-05-27

    strength, volume stability, durability and permeability. The primary mechanism of soil stabilisation with PC is through the hydration of PC which leads to the formation of cementitious calcium silicate hydrates (C-S-H), calcium aluminate hydrates (C... which leads to expansion and cracking of cement and concrete through the delayed hydration. Reactive MgOs have much higher reactivity than dead burned MgO and hence faster hydration rate. On the other hand, given the different origins and production...

  4. Development of a Biomarker and Clay Based Remediation Strategy for Populations at Risk for Fumonisin Toxicosis 

    E-Print Network [OSTI]

    Robinson, Abraham

    2012-07-16

    F. nygamai FA1-3, FB1-5, FAK1, FBK1, FC1,4, FP1-3, PH1a-b 7200 530 140 F. dlamini FB1 82 NT NT F. napiforme FB1 480 NT NT F. pseudonygamai FB1-2 Tr Tr NT F. andiyazi FB1 Tr ND NT Section Elegans F. oxysporum FC1,3-4, N...-acetyl-FC1,iso-FC1, N-acetyl-iso-FC1, OH-FC1, N-acetyl-OH-FC1 NT NT NT F. oxysporum var. redolens FB1-3 300 6 0.9 Section Arthrosporiella F. polyphialidicum FB1 500 NT NT NT, not tested. Tr, trace amounts (1 to 4 ng g -1) were detected. ND...

  5. Resource conservation and recovery act draft hazardous waste facility permit: Waste Isolation Pilot Plant (WIPP). Attachments: Volume 4 of 4

    SciTech Connect (OSTI)

    Not Available

    1993-08-01

    Volume IV contains the following attachments for Module IV: VOC monitoring plan for bin-room tests (Appendix D12); bin emission control and VOC monitoring system drawings; bin scale test room ventilation drawings; WIPP supplementary roof support system, underground storage area, room 1, panel 1, DOE/WIPP 91-057; and WIPP supplementary roof support system, room 1, panel 1, geotechnical field data analysis bi-annual report, DOE/WIPP 92-024.

  6. 3/21/09 11:36 PMAbstract Print View Page 1 of 2http://www.abstractsonline.com/plan/AbstractPrintView.aspx?mID=19...4f7c-91b5-bfa105d6f144&cKey=fb7a90dc-52c3-44c1-9223-a211de73b7a4

    E-Print Network [OSTI]

    Shenoy, Krishna V.

    in this application the system includes a lithium ion battery pack and a separate clock chip, the INI chip can also. Using the available space inside the aluminum enclosure for a 2000 mA-hr battery pack, this device can

  7. PHYSICAL REVIEW B 91, 024511 (2015) Multistability and condensation of exciton-polaritons below threshold

    E-Print Network [OSTI]

    Nori, Franco

    2015-01-01

    threshold Jiun-Yi Lien,1,2,* Yueh-Nan Chen,1, Natsuko Ishida,3 Hong-Bin Chen,1 Chi-Chuan Hwang,2 and Franco

  8. Interoperable and Secure Communication for Cyber Physical Systems in the Energy Grid

    E-Print Network [OSTI]

    Lee, Eun Kyu

    2014-01-01

    twiki-sggrid/bin/view/SmartGrid/ SGIPSemanticModelSGAC. [4]periods [42]. http://www.iec.ch/smartgrid/standards/ http://

  9. A transilient matrix for moist convection

    E-Print Network [OSTI]

    Romps, D.

    2012-01-01

    eddies, and compen- sating subsidence) binned by origin andof q by compensating subsidence. The third term describespossible z , compensating subsidence, and turbulent di?usion

  10. IACT Conference Proceedings, Abstracts, Presentations, and Poster...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Interfacial Catalysis for Hydrogen Production," Jeffrey Greeley, Bin Liu, Rees Rankin, Zhi-Jian Zhao, and Zhenhua Zeng, 2014 ACS Annual Meeting, March 16, 2014, Dallas, TX. "In...

  11. California's Energy Future - The View to 2050

    E-Print Network [OSTI]

    2011-01-01

    Analysis Bin Wind Onshore, shallow offshore tur- bineswind, solar, biomass, geothermal, hydro, and marine energy offshore.offshore tur- bines ”Third generation” PV High-altitude wind

  12. California’s Energy Future: The View to 2050 - Summary Report

    E-Print Network [OSTI]

    Yang, Christopher

    2011-01-01

    Analysis Bin Wind Onshore, shallow offshore tur- bineswind, solar, biomass, geothermal, hydro, and marine energy offshore.offshore tur- bines ”Third generation” PV High-altitude wind

  13. Road-crossing restoration on alluvial creeks in the Klamath National Forest, California

    E-Print Network [OSTI]

    Lawrence, Justin E

    2008-01-01

    colonization upstream and downstream of the road-crossingsthis data into upstream and downstream bins to estimate thetaken from traps upstream and downstream of the roads.

  14. SAFETY, GUIDELINES & ETIQUETTE Most programs will be held rain or shine. We assume you will come unless we hear from you.

    E-Print Network [OSTI]

    Lawrence, Deborah

    to use the recycling bins (located in Picnic Area and at Peetwood Pavilion) for plastic, glass, and cans. Reduce, Reuse, and RECYCLE! #12;

  15. Optimal Filters for High-Speed Compressive Detection in ...

    E-Print Network [OSTI]

    2013-02-14

    ... medicine and biology, pharmacy, counterfeit detection, and national security. .... bins, and P is a matrix that describes this energy distribution: Pij is the ...

  16. California’s Energy Future: The View to 2050 - Summary Report

    E-Print Network [OSTI]

    Yang, Christopher

    2011-01-01

    generation or advanced nuclear technology. 17 “Nuclear Powerour energy needs. Bin Nuclear Technology Coal or Natural Gas4A. Summary of technology readiness for nuclear and CCS. The

  17. California's Energy Future - The View to 2050

    E-Print Network [OSTI]

    2011-01-01

    generation or advanced nuclear technology. 17 “Nuclear Powerour energy needs. Bin Nuclear Technology Coal or Natural Gas4A. Summary of technology readiness for nuclear and CCS. The

  18. Independent Oversight Assessment of the Nuclear Safety Culture...

    Office of Environmental Management (EM)

    the safety basis documents containing no mitigated accident scenarios. There are no criteriarequirements for addressing beyond design basis events. Accident binning is...

  19. Measures of galaxy environment - II. Rank-ordered mark correlations

    E-Print Network [OSTI]

    2013-01-01

    ? r colour (right) mark CFs (upper panels), with additionalmock catalogue. Lower panel: CFs for luminosity bins ?20 CFs measured from SDSS DR7 (

  20. Assessment of Building Energy-Saving Policies and Programs in China During the 11th Five Year Plan

    E-Print Network [OSTI]

    Zhou, Nan

    2011-01-01

    and/or require energy efficiency in buildings during the 11to strengthen energy efficiency in buildings. This BuildingHao Bin. 2009. “Building Energy Efficiency Evaluation and

  1. Advanced Technology Light Duty Diesel Aftertreatment System ...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    More Documents & Publications Passive Catalytic Approach to Low Temperature NOx Emission Abatement Cummins' Next Generation Tier 2, Bin 2 Light Truck Diesel Engine...

  2. Don't always blame the photons: Relationships between deprotection blur, LER, and shot noise in EUV photoresists

    E-Print Network [OSTI]

    Anderson, Christopher N.

    2009-01-01

    A. Wuest, K. Dean, “Photons, electrons and acid yields inDon’t always blame the photons: relationships betweenbins, more absorbed photons per bin, better counting

  3. Improving earthquake source spectrum estimation using multitaper techniques

    E-Print Network [OSTI]

    Prieto, Germán A.

    2007-01-01

    bins of similar seismic moment, a process that averages thefailure process, some energy is radiated as seismic waves (seismic parameters that describe the earthquake rupture process.

  4. NEXT ASSEMBLY DWG. TYPE SOCORRO, NEW MEXICO 87801

    E-Print Network [OSTI]

    Groppi, Christopher

    11 12 13 14 15 16 17 18 19 20 21 22 23 24 J7 PWR IN -6.5 BIN +6.5 BIN +16.5 BIN -16.5 BIN MOSI MISO MOSI SCLK +5_A+5_A -5_A-5_A MFM- MFM+CFM+ CFM- MISO MOSI SCLK AGCV PWR MCoarseV CCoarseV MFMV CFMV DDSCS2 DDSCS3 M52+ M52- CSMONADC CSMONTEMP CSPROM WP CSAGCDAC FS EOC AGCV PWR AIN10 Master In Slave Out

  5. Comparing VM-Placement Algorithms for On-Demand Clouds K. Mills, J. Filliben and C. Dabrowski

    E-Print Network [OSTI]

    of the Eucalyptus open-source code [6] and the online bin-packing literature [7-8]. Eucalyptus inspired us

  6. Bob Scowcroft: Executive Director, Organic Farming Research Foundation

    E-Print Network [OSTI]

    Reti, Irene H.

    2010-01-01

    inventing really neat compost bins, and Jeavons and Rip haddo nothing but cover crop and compost now. So don’t you guys

  7. WORM DAY!!! UConn Master Composter Program

    E-Print Network [OSTI]

    Alpay, S. Pamir

    WORM DAY!!! UConn Master Composter Program MAKE YOUR OWN VERMI-COMPOST BIN ­ YOU BRING THE MATERI;WORM DAY!!! UConn Master Composter Program Registration Form Name

  8. Joining of Advanced Thermoplastics

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    PP biocomposite - Used in the Ford Flex 3rd row bin and lid * Advantages - With little increase in density, many properties can be improved: * decreased permeability to vapors...

  9. Further improvement of conventional diesel NOx aftertreatment concepts as pathway for SULEV

    Broader source: Energy.gov [DOE]

    Discusses possible improvement potential and various pathways for LNT after-treatment systems for diesel applications to comply with Tier 2 Bin 5 and SULEV regulations

  10. Benefits and Drawbacks of Compression Ratio Reduction in PCCI Combustion Application in an Advanced LD Diesel Engine

    Broader source: Energy.gov [DOE]

    Study of the effect of compression ratio on performance of light duty diesel operating with PCCI calibration, near EURO6/Tier 2 Bin 5 NOx limits.

  11. California's Energy Future - The View to 2050

    E-Print Network [OSTI]

    2011-01-01

    altitude wind Bin Natural Gas Storage Combustion turbineand natural gas) with carbon capture and storage (CCS) andof natural gas for load balancing: electricity storage and

  12. California’s Energy Future: The View to 2050 - Summary Report

    E-Print Network [OSTI]

    Yang, Christopher

    2011-01-01

    altitude wind Bin Natural Gas Storage Combustion turbineand natural gas) with carbon capture and storage (CCS) andof natural gas for load balancing: electricity storage and

  13. The Potential of Cellulosic Ethanol Production from Municipal Solid Waste: A Technical and Economic Evaluation

    E-Print Network [OSTI]

    Shi, Jian; Ebrik, Mirvat; Yang, Bin; Wyman, Charles E.

    2009-01-01

    collected from the West Valley Material Recovery Facilitywas conducted at the West Valley MRF and Transfer Station (from green bins In the West Valley MRF and Transfer Station

  14. RSTT

    Energy Science and Technology Software Center (OSTI)

    002410WKSTN00 Code for Calculating Regional Seismic Travel Time  https://na22.nnsa.doe.gov/cgi-bin/prod/nemr 

  15. The effects of mapping CT images to Monte Carlo materials on GEANT4 proton simulation accuracy

    SciTech Connect (OSTI)

    Barnes, Samuel; McAuley, Grant; Slater, James; Wroe, Andrew

    2013-04-15

    Purpose: Monte Carlo simulations of radiation therapy require conversion from Hounsfield units (HU) in CT images to an exact tissue composition and density. The number of discrete densities (or density bins) used in this mapping affects the simulation accuracy, execution time, and memory usage in GEANT4 and other Monte Carlo code. The relationship between the number of density bins and CT noise was examined in general for all simulations that use HU conversion to density. Additionally, the effect of this on simulation accuracy was examined for proton radiation. Methods: Relative uncertainty from CT noise was compared with uncertainty from density binning to determine an upper limit on the number of density bins required in the presence of CT noise. Error propagation analysis was also performed on continuously slowing down approximation range calculations to determine the proton range uncertainty caused by density binning. These results were verified with Monte Carlo simulations. Results: In the presence of even modest CT noise (5 HU or 0.5%) 450 density bins were found to only cause a 5% increase in the density uncertainty (i.e., 95% of density uncertainty from CT noise, 5% from binning). Larger numbers of density bins are not required as CT noise will prevent increased density accuracy; this applies across all types of Monte Carlo simulations. Examining uncertainty in proton range, only 127 density bins are required for a proton range error of <0.1 mm in most tissue and <0.5 mm in low density tissue (e.g., lung). Conclusions: By considering CT noise and actual range uncertainty, the number of required density bins can be restricted to a very modest 127 depending on the application. Reducing the number of density bins provides large memory and execution time savings in GEANT4 and other Monte Carlo packages.

  16. Measurement of the inclusive jet cross section in proton-antiproton collisions at the center-of-mass energy of 1.96 TeV

    SciTech Connect (OSTI)

    Voutilainen, Mikko Antero; /Helsinki Inst. of Phys. /Helsinki U. of Tech. /Nebraska U. /Saclay

    2008-07-01

    This thesis studies the high-energy collisions of protons and antiprotons. The data used in the measurement were collected during 2004-2005 with the D0 detector at the Tevatron Collider of the Fermi National Accelerator Laboratory and correspond to 0.7 fb{sup -1} of integrated luminosity. High energy hadron collisions usually produce collimated sprays of particles called jets. The energy of the jets is measured using a liquid Argon-Uranium calorimeter and the production angle is determined with the help of silicon microstrip and scintillating fiber trackers. The inclusive jet cross section in proton-antiproton collisions is measured as a function of jet transverse momentum p{sub T} in six bins of jet rapidity at the center-of-mass energy {radical}s = 1.96 TeV. The measurement covers jet transerve momenta from 50 GeV up to 600 GeV and jet rapidities up to |y| = 2.4. The data are collected using a set of seven single jet triggers. Event and jet cuts are applied to remove non-physical backgrounds and cosmic-ray interactions. The data are corrected for jet energy calibration, cut and trigger efficiencies and finite jet p{sub T} resolution. The corrections are determined from data and the methods are tested with Monte Carlo simulation. The main experimental challenges in the measurement are the calibration of jet energies and the determination of the jet p{sub T} resolution. New methods are developed for the jet energy calibration that take into account physical differences between the {gamma}+jet and dijet calibration samples arising from quark and gluon jet differences. The uncertainty correlations are studied and provided as a set of uncertainty sources. The production of particle jets in hadron collisions is described by the theory of quantum chromodynamics (QCD). When the transverse jet momentum is large, the contributions from long-distance physics processes are small and the production rates of jets can be predicted by perturbative QCD. The inclusive jet cross section in p{bar p} collisions at large p{sub T} is directly sensitive to the strong coupling constant ({alpha}{sub s}) and the parton distribution functions (PDFs) of the proton. This measurement can be used to constrain the PDFs, in particular the gluon PDF at high proton momentum fraction x, and to look for quark substructure at the TeV scale. The data are compared to the theory predictions with perturbative QCD in the next-to-leading order precision and a good agreement between data and theory is observed.

  17. Observations and Measurements of Orbitally Excited L=1 B Mesons at the D0 Experiment

    SciTech Connect (OSTI)

    Williams, Mark Richard James; /Lancaster U.

    2008-09-01

    This thesis describes investigations of the first set of orbitally excited (L = 1) states for both the B{sub d}{sup 0} and B{sub s}{sup 0} meson systems (B**{sub d} and B**{sub s}). The data sample corresponds to 1.35 fb{sup -1} of integrated luminosity, collected in 2002-2006 by the D0 detector, during the Run IIa operation of the Tevatron p{bar p} colliding beam accelerator. The B**{sub d} states are fully reconstructed in decays to B{sup (*)+} {pi}{sup -}, with B{sup (*)+} {yields} {gamma} J/{psi}K{sup +}, J/{psi} {yields} {mu}{sup +}{mu}{sup -}, yielding 662 {+-} 91 events, and providing the first strong evidence for the resolution of two narrow resonances, B{sub 1} and B*{sub 2}. The masses are extracted from a binned {chi}{sup 2} fit to the invariant mass distribution, giving M(B{sub 1}) = 5720.7 {+-} 2.4(stat.) {+-} 1.3(syst.) {+-} 0.5 (PDG) MeV/c{sup 2} and M(B*{sub 2}) = 5746.9 {+-} 2.4(stat.) {+-} 1.0(syst.) {+-} 0.5(PDG) MeV/c{sup 2}. The production rate of narrow B**{sub d} {yields} B{pi} resonances relative to the B{sup +} meson is determined to be [13.9 {+-} 1.9(stat.) {+-} 3.2(syst.)]%. The same B{sup +} sample is also used to reconstruct the analogous states in the B{sub s}{sup 0} system, in decays B**{sub s} {yields} B{sup (*)+} K{sup -}. A single resonance in the invariant mass distribution is found with a statistical significance of 5{sigma}, interpreted as the B*{sub s2} state. The mass is determined to be M(B*{sub s2}) = 5839.6 {+-} 1.1(stat.) {+-} 0.4(syst.) {+-} 0.5(PDG) MeV/c{sup 2}, and the production rate of B*{sub s2} {yields} BK resonances is measured to be a fraction (2.14 {+-} 0.43 {+-} 0.24)% of the corresponding rate for B{sup +} mesons. Alternative fitting hypotheses give inconclusive evidence for the presence of the lighter B{sub s1} meson.

  18. Islamic Republic of Afghanistan

    E-Print Network [OSTI]

    Takada, Shoji

    of Iran Aghajari Oil & Gas Production Company (AOGPC) B,C,N 20 Islamic Republic of Iran Aluminat Places The World Islamic Front for Jihad against Jews and Crusaders Usama Bin Laden Network Usama Bin of Afghanistan Islamic Republic of Pakistan Ummah Tameer E-Nau (UTN) N 4 United Arab Emirates Energy Global

  19. Islamic Republic of Afghanistan

    E-Print Network [OSTI]

    Takada, Shoji

    Oil & Gas Production Company (AOGPC) B,C,N 20 Islamic Republic of Iran Aluminat Aluminat Production Places The World Islamic Front for Jihad against Jews and Crusaders Usama Bin Laden Network Usama Bin of Afghanistan Islamic Republic of Pakistan Ummah Tameer E-Nau (UTN) N 4 United Arab Emirates Energy Global

  20. Validation of a Building Simulation Tool Using Field Data for Three Identical Configuration Full-Serve Restaurants Using Different HVAC Systems 

    E-Print Network [OSTI]

    Brillhart, P. L.; Worek, W. M.

    2000-01-01

    Philadelphia, PA, National Renewable Energy Laboratory (NREL) hour-by-hour bin TMY2 meteorological data was used for Philadelphia to model the annual outdoor conditions experienced by each site. Output was provided in the form of humidity bins, monthly energy...

  1. UC Campus Merced Finishes UCM 131 Context -Private Offices Code Name

    E-Print Network [OSTI]

    Oviedo, Néstor J.

    Under Bin/Shelf Lighting - LED LED LED Shelf Light Desk Lighting LED Soto Markerboard Code Name Static - LED LED LED Shelf Light Desk Lighting LED Soto Markerboard Code Name Static Markerboard 110 Series 4606 Mist Task Lighting Code Name Under Bin/Shelf Lighting - Standard Florescent Standard Shelf Light

  2. Compost 101Turn this year's trash into next year's treasure

    E-Print Network [OSTI]

    Hutcheon, James M.

    Compost 101Turn this year's trash into next year's treasure Filling and Maintaining Compost Georgia://ceps.georgiasouthern.edu/garden This brochure is funded in part by a grant from a Museums for America Grant. Types of Composting Bins To fill your compost bin, alternate brown and green materials. Keep in mind that the ideal ratio is three

  3. Nonlinear Adaptive Robust Control Theory and Applications

    E-Print Network [OSTI]

    Yao, Bin

    Engineering, Purdue University 5 Different Types of Race Car Drivers #12;Copyright by Bin Yao, School Engineering Purdue University West Lafayette, IN47907 #12;Copyright by Bin Yao, School of Mechanical Engineering, Purdue University 2 OUTLINE MotivationMotivation General ARC Design Philosophy and Structure

  4. SHOPPING GENIE Ethernet cables must

    E-Print Network [OSTI]

    Cantlon, Jessica F.

    regulations. You may not bring your own. SPACE HEATERS & WIN- DOW AIR CONDITION- ERS are simply not al- lowed room. STORAGE BINS Bins that can fit under a bed or are stackable are ideal for space saving are settled be- fore buying a rug. Assess the space available. Keep in mind that rugs do require additional

  5. UBC Social Ecological Economic Development Studies (SEEDS) Student Report Rapidly Renewable Materials

    E-Print Network [OSTI]

    in the LEED qualification. It is believed that using RRMs can reduce our demand on finite raw material Materials: Wool And Cork Bin Ou-Yang David Tan Ritesh Bhan University of British Columbia APSC 262 March 31 RAPIDLY RENEWABLE MATERIALS: WOOL AND CORK Done by: Bin Ou-Yang David Tan Ritesh Bhan #12;i ABSTRACT

  6. North Carolina State University, Campus Box 7409, Raleigh, NC 27695 | 919-515-3480 | www.ncsc.ncsu.edu | 1/14 Advancing Clean Energy for a Sustainable Economy

    E-Print Network [OSTI]

    city/44 hwy, Bin 5 Honda Civic Natural Gas 1.8L, Auto, Natural Gas 27 city/38 hwy, Bin 2 Honda Civic-515-3480 | www.cleantransportation.org Green Vehicle Guide: Best vehicles by size class for 2014 The U.S. Environmental Protection Agency (EPA) Green Vehicle Guide provides fuel economy estimates and tailpipe emission

  7. North Carolina State University, Campus Box 7409, Raleigh, NC 27695 | 919-515-3480 | www.ncsc.ncsu.edu | 7/18/13 Advancing Clean Energy for a Sustainable Economy

    E-Print Network [OSTI]

    hwy, Bin 5 Honda Civic Natural Gas 1.8L, Auto, Natural Gas 27 city/38 hwy, Bin 2 Honda Civic Hybrid 1-515-3480 | www.cleantransportation.org Green Vehicle Guide: Best vehicles by size class for 2013 The U.S. Environmental Protection Agency (EPA) Green Vehicle Guide provides fuel economy estimates and tailpipe emission

  8. North Carolina State University, Campus Box 7409, Raleigh, NC 27695 | 919-515-3480 | www.nccleantech.ncsu.edu | 1/14 Advancing Clean Energy for a Sustainable Economy

    E-Print Network [OSTI]

    driving simulations. Air Pollution and Greenhouse Gas Scores (GHG) allow comparison between all vehicle city/44 hwy, Bin 5 Honda Civic Natural Gas 1.8L, Auto, Natural Gas 27 city/38 hwy, Bin 2 Honda Civic.cleantransportation.org Green Vehicle Guide: Best vehicles by size class for 2014 The U.S. Environmental Protection Agency (EPA

  9. Calculating exclusion limits for Weakly Interacting Massive Particle direct detection experiments without background subtraction

    E-Print Network [OSTI]

    Anne M Green

    2001-10-04

    Competitive limits on the weakly interacting massive particle (WIMP) spin-independent scattering cross section are currently being produced by 76Ge detectors originally designed to search for neutrinoless double beta decay, such as the Heidelberg-Moscow and IGEX experiments. In the absence of background subtraction, limits on the WIMP interaction cross section are set by calculating the upper confidence limit on the theoretical event rate, given the observed event rate. The standard analysis technique involves calculating the 90% upper confidence limit on the number of events in each bin, and excluding any set of parameters (WIMP mass and cross-section) which produces a theoretical event rate for any bin which exceeds the 90% upper confidence limit on the event rate for that bin. We show that, if there is more than one energy bin, this produces exclusion limits that are actually at a lower degree of confidence than 90%, and are hence erroneously tight. We formulate criteria which produce true 90% confidence exclusion limits in these circumstances, including calculating the individual bin confidence limit for which the overall probability that no bins exceeds this confidence limit is 90% and calculating the 90% minimum confidence limit on the number of bins which exceed their individual bin 90% confidence limits. We then compare the limits on the WIMP cross-section produced by these criteria with those found using the standard technique, using data from the Heidelberg-Moscow and IGEX experiments.

  10. Parametric On-Line Packing x F. K. Miyazawa y Y. Wakabayashi z

    E-Print Network [OSTI]

    | C. Postal 6176 | 13083-970 | Campinas{SP | Brazil. z Instituto de Matem#19;atica e Estat#19~ao Paulo{SP | Brazil. #12; 1. Strip Packing Problem (SPP): Given a list L of rectangles, and a rectangle, and rectangles of unit dimensions R = (1; 1), called bins, pack the rectangles of L into a minimum number of bins

  11. Mon. Not. R. Astron. Soc. 415, 7782 (2011) doi:10.1111/j.1365-2966.2011.18648.x Is GeV emission from Gamma-Ray Bursts of external shock origin?

    E-Print Network [OSTI]

    Zhang, Bing

    2011-01-01

    from Gamma-Ray Bursts of external shock origin? Amanda Maxham, Bin-Bin Zhang and Bing Zhang Department February 22; in original form 2010 December 30 ABSTRACT Recent observations of Gamma-Ray Bursts (GRBs (080916C, 090510, 090902B and 090926A) jointly detected by Fermi LAT and Gamma-ray Burst Monitor (GBM

  12. Proportional Fairness for Overlapping Cells in Wireless Networks

    E-Print Network [OSTI]

    Chan, Mun Choon

    Proportional Fairness for Overlapping Cells in Wireless Networks Bin Bin Chen Department allocation in a multiple cell environment. This paper extends existing Proportional Fairness model for wired proportional fairness framework for wired networks [4] and single wireless cell [3], to the con- text

  13. University of Kentucky Demonstration of an Automated Control

    E-Print Network [OSTI]

    Tilbury, Dawn

    -directionM-power off onCCW onCW onCWonCCW pos. pos. pos L-on R-on homeL-bin R-bin R-onR-on R-on R-on L-onL-on L-on L

  14. GN Wave theory and TEBEM for Wave-Body Interaction

    E-Print Network [OSTI]

    GN Wave theory and TEBEM for Wave-Body Interaction Dr. BinBin Zhao and Professor Wenyang Duan of simulating irregular nonlinear water wave interaction with arbitrary floating bodies, the Green-Naghdi wave corners. The results show that the high-level GN theory can predict wave transformation over uneven seabed

  15. SIMULATION OF ENERGY SELECTIVE X-RAY IMAGES FOR MATERIAL DIS-CRIMINATION

    E-Print Network [OSTI]

    Hickman, Mark

    SIMULATION OF ENERGY SELECTIVE X-RAY IMAGES FOR MATERIAL DIS- CRIMINATION Rune S Thing1 , Syen J model can be applied to any material combination and any number of energy bins. Figure: Top row Carlo model is presented to evaluate the clinical benefits of optimal energy bins in spectral X

  16. UBC Social Ecological Economic Development Studies (SEEDS) Student Report Integrating Vermicomposting into AMS SUB Operations -Phase 3 -Compiled presentations

    E-Print Network [OSTI]

    SPACE FOR FOOD WASTE, CARBON SOURCE, WORM BIN FINDINGS - EXECUTION #12; ENGAGE STAFF CHANGE ATTITUDES & BEHAVIOURS SPECIFIC FOOD WASTE BINS FOR WORMS TRAINING & SUPPORT SIGNAGE FINDINGS - EXECUTION #12;Where Campus (in-vessel unit) 25% is recycled #12;#12;#12;#12;COMPOST ALL FOOD WASTE RECOMMENDATION

  17. UCSF LivingGreen Catering Best Practices 1 UCSF Living Green Catering Best Practices August 20, 2011

    E-Print Network [OSTI]

    Soloveichik, David

    and composting bins with proper signage in the meeting room and where food will be served. Before your event boxes are wasteful even though they are recyclable. 8. Serve food on trays that are reusable rather recycling and composting bins with signage. When you order your venue, specify that you will need recycling

  18. UBC Social Ecological Economic Development Studies (SEEDS) Student Report Karl Kong, Pei Wen Lei, Yabo Li, Rain Yuan Rain Tian

    E-Print Network [OSTI]

    that are currently used to collect food scraps at UBC are cleaned at the Composting Facility located at the south, Yabo Li, Rain Yuan Rain Tian AN INVETIGATION INTO ORGANIC WASTE BIN LINERS APSC 262 April 10, 2014 1036 Technology and Society Instructor Name: Paul Winkelman AN INVETIGATION INTO ORGANIC WASTE BIN LINERS

  19. 3219.ps

    E-Print Network [OSTI]

    extracted and used in a guided local search metaheuristic approach to ..... The offline problem is defined in terms of n bins B and each bin b ? B has a capacity ..... munication Technologies in Tourism 2005, Proceedings of ENTER, 149–159.

  20. Microstructural Examination to Aid in Understanding Friction Bonding Fabrication Technique for Monolithic Nuclear Fuel

    SciTech Connect (OSTI)

    Karen L. Shropshire

    2008-04-01

    Monolithic nuclear fuel is currently being developed for use in research reactors, and friction bonding (FB) is a technique being developed to help in this fuel’s fabrication. Since both FB and monolithic fuel are new concepts, research is needed to understand the impact of varying FB fabrication parameters on fuel plate characteristics. This thesis research provides insight into the FB process and its application to the monolithic fuel design by recognizing and understanding the microstructural effects of varying fabrication parameters (a) FB tool load, and (b) FB tool face alloy. These two fabrication parameters help drive material temperature during fabrication, and thus the material properties, bond strength, and possible formation of interface reaction layers. This study analyzed temperatures and tool loads measured during those FB processes and examined microstructural characteristics of materials and bonds in samples taken from the resulting fuel plates. This study shows that higher tool load increases aluminum plasticization and forging during FB, and that the tool face alloy helps determine the tool’s heat extraction efficacy. The study concludes that successful aluminum bonds can be attained in fuel plates using a wide range of FB tool loads. The range of tool loads yielding successful uranium-aluminum bonding was not established, but it was demonstrated that such bonding can be attained with FB tool load of 48,900 N (11,000 lbf) when using a FB tool faced with a tungsten alloy. This tool successfully performed FB, and with better results than tools faced with other materials. Results of this study correlate well with results reported for similar aluminum bonding techniques. This study’s results also provide support and validation for other nuclear fuel development studies and conclusions. Recommendations are offered for further research.

  1. ENERGY & ENVIRONMENT DIVISION. ANNUAL REPORT FY 1980

    E-Print Network [OSTI]

    Authors, Various

    2010-01-01

    solar systems, and anaerobic digesters, F.B. Lucarelli, J.the anaerobic di- gester. The gas mixture from the digester

  2. Thin Servers with Smart Pipes: Designing SoC Accelerators for Memcached

    E-Print Network [OSTI]

    Wenisch, Thomas F.

    .lim@hp.com David Meisner Facebook meisner@fb.com Ali G. Saidi ARM R&D ali.saidi@arm.com Parthasarathy Ranganathan

  3. Optimization Methods and Software Vol. 18, No. 4, August 2003, pp. 395415

    E-Print Network [OSTI]

    Neumaier, Arnold

    YAMAMOTOa, aInstitute of Policy and Planning Sciences, University of Tsukuba, Tsukuba 305-8573, Japan; bFB4

  4. Higgs boson search at ATLAS

    E-Print Network [OSTI]

    Scott Snyder; for the ATLAS Collaboration

    2012-09-04

    The status of the ATLAS Higgs boson search using about 5 fb^-1 of data recorded in 2011 is summarized. Proceedings from Physics at the LHC 2012 (Vancouver).

  5. Flexible Distributed Energy & Water from Waste for the Food ...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Chemical Pharmaceutical 19% Fermentation 7% Food & Beverage 35% Sewage 4% Pulp and Paper 9% Source: Biothane (approx 500 installations) F&B Key Industrial Market * Small scale...

  6. ENERGY AND ENVIRONMENT DIVISION ANNUAL REPORT 1978

    E-Print Network [OSTI]

    Cairns, E.L.

    2011-01-01

    of Refuse Derived Fuel (RDF) from MSW, Direct combustion ofrefuse derived fuel (RDF) systems, and direct combustionDirect combustion RDF = Refuse-derived fuels FB = Fluidized-

  7. A search for new physics with Z bosons, jets, and missing transverse energy at CMS

    E-Print Network [OSTI]

    Andrews, Warren T.

    2012-01-01

    4.1.1 Jets and MET . . . . . . . . . . . . . . . . . . . . .Models: MET and Jets . . . . . . . . . . 4.7 Simplifiedyields for the preselection with N jets ? 3 for 4.98 fb ?

  8. Development of Simplified Probabilistic Risk Assessment Model for Seismic Initiating Event

    SciTech Connect (OSTI)

    S. Khericha; R. Buell; S. Sancaktar; M. Gonzalez; F. Ferrante

    2012-06-01

    ABSTRACT This paper discusses a simplified method to evaluate seismic risk using a methodology built on dividing the seismic intensity spectrum into multiple discrete bins. The seismic probabilistic risk assessment model uses Nuclear Regulatory Commission’s (NRC’s) full power Standardized Plant Analysis Risk (SPAR) model as the starting point for development. The seismic PRA models are integrated with their respective internal events at-power SPAR model. This is accomplished by combining the modified system fault trees from the full power SPAR model with seismic event tree logic. The peak ground acceleration is divided into five bins. The g-value for each bin is estimated using the geometric mean of lower and upper values of that particular bin and the associated frequency for each bin is estimated by taking the difference between upper and lower values of that bin. The component’s fragilities are calculated for each bin using the plant data, if available, or generic values of median peak ground acceleration and uncertainty values for the components. For human reliability analysis (HRA), the SPAR HRA (SPAR-H) method is used which requires the analysts to complete relatively straight forward worksheets that include the performance shaping factors (PSFs). The results are then used to estimate human error probabilities (HEPs) of interest. This work is expected to improve the NRC’s ability to include seismic hazards in risk assessments for operational events in support of the reactor oversight program (e.g., significance determination process).

  9. The physics case of DAFNE-2

    E-Print Network [OSTI]

    G. Venanzoni

    2007-10-18

    We present the physics case of DAFNE-2, an $e^+e^-$ collider expected to deliver 20-50 fb$^{-1}$ at the $\\phi(1020)$ peak, and $\\sim$ 5 fb$^{-1}$ in the energy region between 1 and 2.5 GeV.

  10. Observation of an Excited B[± over c] Meson State with the ATLAS Detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for excited states of the B[± over c] meson is performed using 4.9??fb[superscript ?1] of 7 TeV and 19.2??fb[superscript ?1] of 8 TeV pp collision data collected by the ATLAS experiment at the LHC. A new state is ...

  11. Search for the Standard Model Higgs boson in the two photon decay channel with the ATLAS detector at the LHC

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for the Standard Model Higgs boson in the two photon decay channel is reported, using 1.08 fb?11.08 fb[superscript ?1] of proton–proton collision data at a centre-of-mass energy of 7 TeV recorded by the ATLAS ...

  12. Observation and examination of a Higgs boson in the ZZ to four lepton channel

    E-Print Network [OSTI]

    Ralph, Duncan (Duncan Kelley)

    2014-01-01

    Results are presented on 5.1 fb- 1 of proton-proton collisions at a center of mass energy of 7 TeV and 19.7 fb- 1 at 8 TeV in a search for decays of the Standard Model (SM) Higgs boson to two Z bosons to four charged ...

  13. Combined search for the Standard Model Higgs boson in pp collisions at ?s=7??TeV with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A combined search for the Standard Model Higgs boson with the ATLAS detector at the LHC is presented. The data sets used correspond to integrated luminosities from 4.6??fb[superscript -1] to 4.9??fb[superscript -1] of ...

  14. Search for the associated production of the Higgs boson with a top-quark pair

    E-Print Network [OSTI]

    CMS Collaboration

    A search for the standard model Higgs boson produced in association with a top-quark pair (tt¯H) is presented, using data samples corresponding to integrated luminosities of up to 5.1 fb?1 and 19.7 fb?1 collected in pp ...

  15. Design Methodology for Unmannded Aerial Vehicle (UAV) Team Coordination

    E-Print Network [OSTI]

    Cummings, Mary "Missy"

    1 Design Methodology for Unmannded Aerial Vehicle (UAV) Team Coordination F.B. da Silva S.D. Scott-mail: halab@mit.edu #12;2 Design Methodology for Unmannded Aerial Vehicle (UAV) Team Coordination by F.B. da Silva, S.D. Scott, and M.L. Cummings Executive Summary Unmanned Aerial Vehicle (UAV) systems, despite

  16. Molecular Characterization of MADS-BOX Transcription Factors and Analysis of Field Population Diversity in the Maize Pathogen Fusarium verticillioides 

    E-Print Network [OSTI]

    Ortiz, Carlos S

    2013-04-10

    (FB1), the most prevalent fumonisin in nature, was first identified in 1988 and has been found to be toxic to human and animals. The gene cluster for FB1 biosynthesis and some environmental conditions responsible for the toxin production are known...

  17. CDF Note 10625 Search for the Standard Model Higgs boson in +

    E-Print Network [OSTI]

    Fermilab

    CDF Note 10625 Search for the Standard Model Higgs boson in + - + jets final state with 8.3fb-1 a search for the Standard Model Higgs boson in + - + jets final state, using CDF Run II data with an integrated luminosity of 8.3 fb-1 . The Signal considered in this search is four Higgs boson production

  18. Measurement of Higgs boson production and properties in the WW decay channel with leptonic final states

    E-Print Network [OSTI]

    Apyan, Aram

    A search for the standard model Higgs boson decaying to a W-boson pair at the LHC is reported. The event sample corresponds to an integrated luminosity of 4.9 fb[superscript ?1] and 19.4 fb[superscript ?1] collected with ...

  19. Improved Search for a Higgs Boson Produced in Association with Z?l+l- in pp? Collisions at ?s=1.96??TeV

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We search for the standard model Higgs boson produced with a Z boson in 4.1??fb-1 [fb superscript -1] of integrated luminosity collected with the CDF II detector at the Tevatron. In events consistent with the decay of the ...

  20. Digitally controlled low frequency square wave electronic ballast

    E-Print Network [OSTI]

    , and the Boost converter is commonly used. However the boost output DC voltage has to be set to be greater tha and the second is a full-bridge converter (FB) used for both ignition and square wave drive. Ignition is achieved as a resonant inverter. After ignition the converter operates as a LFSW inverter by controlling the FB to act

  1. Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A measurement of the production processes of the recently discovered Higgs boson is performed in the two-photon final state using 4.5??fb[superscript ?1] of proton-proton collisions data at ?s=7??TeV and 20.3??fb[superscript ...

  2. S A P D O C U M E N T N U M B E R S IF THE FINANCE

    E-Print Network [OSTI]

    Weaver, Harold A. "Hal"

    S A P D O C U M E N T N U M B E R S IF THE FINANCE DOCUMENT STARTS WITH AND IS AND DOC TYPE Transactions Enter Asset Transaction FB03 Any Finance or Sponsored Transactional Reports such as: CO Monthly long AB Automatic Clearing Automatic Clearing FB03 Any Finance or Sponsored Transactional Reports

  3. BOREHOLE RADAR OBSERVER SHEET Site: Date

    E-Print Network [OSTI]

    Barrash, Warren

    walkaway: Start Pos (t0 Search): Step: End Pos.: FB sample: t0 delay: (iii) Downhole walkaway: Start Pos.: Step: End Pos.: (iv) Airwave record: Separation: Number of Traces: FB sample: t0 delay: (v) Level run: Stacks: Start Pos.: Step: End Pos.: Acquisition Parameters: Antenna frequency: Transmitter power

  4. Fixed bed gasification studies on coal-feedlot biomass and coal-chicken litter biomass under batch mode operation 

    E-Print Network [OSTI]

    Priyadarsan, Soyuz

    2002-01-01

    &M University Boiler Burner Laboratory, and was fired with a) coal, b) feedlot biomass (FB), c) chicken litter biomass (LB), d) high ash feedlot biomass (HFB), e) coal: FB blend (CFB), f) coal: LB blend (CLB), g) coal: HFB blend (CHFB), and h) LB: HFB blend...

  5. Characterizing Facebook's Memcached Yuehai Xu (Wayne State University, Facebook) yhxu@wayne.edu

    E-Print Network [OSTI]

    Frachtenberg, Eitan

    Characterizing Facebook's Memcached Workload Yuehai Xu (Wayne State University, Facebook) yhxu@wayne.edu Eitan Frachtenberg (Facebook) etc@fb.com Song Jiang (Wayne State University) sjiang@wayne.edu Mike Paleczny (Facebook) mpal@fb.com Abstract This article analyzes the workload of Memcached at Facebook, one

  6. Psychology 204 Spring 2007. Tuesdays 5 7:30 PM Industrial Psychology & Organizational Development

    E-Print Network [OSTI]

    Sanders, Matthew

    will spontaneously occur based on students' particular interests. Abbreviations are given for the require readings: Surveys and related diagnostic techniques. 2/20 Creativity in individual, group, and organizational on leadership (MEP 9; F&B: 14- 15). 4/10 Negotiation and conflict resolution (F&B 10). 4/17 Modifying

  7. Frequency(#Seedlings&Saplings) Substrate Cover (%)

    E-Print Network [OSTI]

    Brown, Sally

    30 35 40 0-10 11-20 21-30 31-40 41-50 51-60 61-70 Frequency Basal Area Bins (m2/ha) All Species 0 5 10 15 20 25 30 35 40 0-10 11-20 21-30 31-40 41-50 51-60 60-100 Frequency Basal Area Bins (m2/ha) P. menziesii 0 5 10 15 20 25 30 35 40 45 0-10 11-20 21-30 31-40 41-50 51-60 60-100 Frequency Basa Area Bins (m2

  8. Effect of blast furnace slag on self-healing of microcracks in cementitious materials

    SciTech Connect (OSTI)

    Huang, Haoliang; Ye, Guang; Damidot, Denis

    2014-06-01

    The physico-chemical process of self-healing in blast furnace slag cement paste was investigated in this paper. With a high slag content i.e., 66% in cement paste and saturated Ca(OH)? solution as activator, it was found that the reaction products formed in cracks are composed of C-S-H, ettringite, hydrogarnet and OH–hydrotalcite. The fraction of C-S-H in the reaction products is much larger than the other minerals. Large amount of ettringite formed in cracks indicates the leaching of SO??² ions from the bulk paste and consequently the recrystallization. Self-healing proceeds fast within 50 h and then slows down. According to thermodynamic modeling, when the newly formed reaction products are carbonated, the filling fraction of crack increases first and then decreases. Low soluble minerals such as silica gel, gibbsite and calcite are formed. Compared to Portland cement paste, the potential of self-healing in slag cement paste is higher when the percentage of slag is high. Highlights: • Self-healing reaction products in slag cement paste were characterized. • Self-healing reaction products formed in time were quantified with image analysis. • Self-healing in slag cement paste was simulated with a reactive transport model. • Effect of carbonation on self-healing was investigated by thermodynamic modeling. • Effect of slag on self-healing was discussed based on experiments and simulation.

  9. Microstructural and compositional change of NaOH-activated high calcium fly ash by incorporating Na-aluminate and co-existence of geopolymeric gel and C-S-H(I)

    SciTech Connect (OSTI)

    Oh, Jae Eun; Moon, Juhyuk; Oh, Sang-Gyun; Clark, Simon M.; Monteiro, Paulo J.M.

    2012-05-15

    This study explores the reaction products of alkali-activated Class C fly ash-based aluminosilicate samples by means of high-resolution synchrotron X-ray diffraction (HSXRD), scanning electron microscope (SEM), and compressive strength tests to investigate how the readily available aluminum affects the reaction. Class C fly ash-based aluminosilicate raw materials were prepared by incorporating Na-aluminate into the original fly ashes, then alkali-activated by 10 M NaOH solution. Incorporating Na-aluminate reduced the compressive strength of samples, with the reduction magnitude relatively constant regardless of length of curing period. The HSXRD provides evidence of the co-existence of C-S-H with geopolymeric gels and strongly suggests that the C-S-H formed in the current system is C-S-H(I). The back-scattered electron images suggest that the C-S-H(I) phase exists as small grains in a finely intermixed form with geopolymeric gels. Despite providing extra source of aluminum, adding Na-aluminate to the mixes did not decrease the Si/Al ratio of the geopolymeric gel.

  10. Activity and Evolution of Vapor Deposited Pt-Pd Oxygen Reduction Catalysts for Solid Acid Fuel Cells

    SciTech Connect (OSTI)

    Papandrew, Alexander B; Chisholm, Calum R; Zecevic, strahinja; Veith, Gabriel M; Zawodzinski, Thomas A

    2013-01-01

    The performance of hydrogen fuel cells based on the crystalline solid proton conductor CsH2PO4 is circumscribed by the mass activity of platinum oxygen reduction catalysts in the cathode. Here we report on the first application of an alloy catalyst in a solid acid fuel cell, and demonstrate an activity 4.5 times greater than Pt at 0.8 V. These activity enhancements were obtained with platinum-palladium alloys that were vapor-deposited directly on CsH2PO4 at 210 C. Catalyst mass activity peaks at a composition of 84 at% Pd, though smaller activity enhancements are observed for catalyst compositions exceeding 50 at% Pd. Prior to fuel cell testing, Pd-rich catalysts display lattice parameter expansions of up to 2% due to the presence of interstitial carbon. After fuel cell testing, a Pt-Pd solid solution absent of lattice dilatation and depleted in carbon is recovered. The structural evolution of the catalysts is correlated with catalyst de-activation.

  11. Does a dissolution-precipitation mechanism explain concrete creep in moist environments?

    E-Print Network [OSTI]

    Isabella Pignatelli; Aditya Kumar; Rouhollah Alizadeh; Yann Le Pape; Mathieu Bauchy; Gaurav Sant

    2015-08-28

    Long-term creep (i.e., deformation under sustained load) is a significant material response that needs to be accounted for in concrete structural design. However, the nature and origin of creep remains poorly understood, and controversial. Here, we propose that concrete creep at RH (relative humidity) > 50%, but fixed moisture-contents (i.e., basic creep), arises from a dissolution-precipitation mechanism, active at nanoscale grain contacts, as is often observed in a geological context, e.g., when rocks are exposed to sustained loads, in moist environments. Based on micro-indentation and vertical scanning interferometry experiments, and molecular dynamics simulations carried out on calcium-silicate-hydrates (C-S-H's), the major binding phase in concrete, of different compositions, we show that creep rates are well correlated to dissolution rates - an observation which supports the dissolution-precipitation mechanism as the origin of concrete creep. C-S-H compositions featuring high resistance to dissolution, and hence creep are identified - analysis of which, using topological constraint theory, indicates that these compositions present limited relaxation modes on account of their optimally connected (i.e., constrained) atomic networks.

  12. Nonprice incentives and energy conservation

    E-Print Network [OSTI]

    Asensio, OI; Delmas, MA; Delmas, MA

    2015-01-01

    Yes Yes Yes Yes Yes Yes Degree-hour bins Yes Yes Yes Yes YesOrganization Hourly Weather Controls Heating Degree HoursCooling Degree Hours Yes Yes Yes Yes Yes Time Dummies Day-

  13. School of Mechanical Engineering, Purdue UniversitySchool of Mechanical Engineering, Purdue UniversitySchool of Mechanical Engineering, Purdue University Energy Saving Control of Hydraulic SystemsEnergy Saving Control of Hydraulic Systems

    E-Print Network [OSTI]

    Yao, Bin

    School of Mechanical Engineering, Purdue UniversitySchool of Mechanical Engineering, Purdue UniversitySchool of Mechanical Engineering, Purdue University Energy Saving Control of Hydraulic Systems Principle Investigator: Bin Yao Research Assistant: Song Liu School of Mechanical Engineering Purdue

  14. School of Mechanical Engineering, Purdue UniversitySchool of Mechanical Engineering, Purdue UniversitySchool of Mechanical Engineering, Purdue University EnergyEnergy--Saving Control of Hydraulic SystemsSaving Control of Hydraulic Systems

    E-Print Network [OSTI]

    Yao, Bin

    School of Mechanical Engineering, Purdue UniversitySchool of Mechanical Engineering, Purdue UniversitySchool of Mechanical Engineering, Purdue University EnergyEnergy--Saving Control of Hydraulic Principle Investigator: Bin Yao Research Assistant: Song Liu School of Mechanical Engineering Purdue

  15. Lab 3a: Distribution functions Histogram

    E-Print Network [OSTI]

    Gustafsson, Torgny

    Lab 3a: Distribution functions Outline · Histogram · Basic concepts · Gaussian (normal) distribution ­Limiting distribution · Poisson distribution ­Counting measurements #12;Histogram and bin A histogram is a graphical representation of the distribution of data. It is a representation of tabulated

  16. Calculation of the Solar Load onto Occupants in a Room using Bidirectional Scattering Distribution Functions and a View Factor Approach

    E-Print Network [OSTI]

    Jedek, Christoph

    2012-01-01

    calculation of the solar load of one specific Bin, it willfor the amount of solar load on one polygon of the manikina given day time. The solar radiation on the one hand can be

  17. Analysis of three sets of SWIW tracer-test data using a two-population complex fracture model for matrix diffusion and sorption

    E-Print Network [OSTI]

    Doughty, C.

    2010-01-01

    as semi-infinite, and thus BTC behavior is comparable totracer breakthrough curve (BTC) are the peak arrival time tflow and transport. The BTC is obtained by binning particle

  18. Epithets, Divine

    E-Print Network [OSTI]

    Budde, Dagmar

    2011-01-01

    and praises addressed to Isis. Archiv für PapyrusforschungPress. Bricault, Laurent 1994 Isis myrionyme. In Hommages àFriedrich Joachim 2003 Ich bin Isis, die Herrin der beiden

  19. The Environment Team to Waste & Recycling

    E-Print Network [OSTI]

    Banaji,. Murad

    . Batteries · PLEASE DO NOT PUT BATTERIES IN THE LANDFILL BINS. · Please dispose of batteries in the battery. · Alternatively, as a last resort, send batteries in a strong internal envelope marked to 'The Battery Container

  20. How dangerous is farm work? Contrary to the popular image of fresh air

    E-Print Network [OSTI]

    Johnson, Eric E.

    surfaces of grain storage bins, silos, or hoppers. Never "walk the grain." Be aware that methane gas, carbon dioxide, ammonia, and hydrogen sulfide can form in unventilated grain silos and manure pits

  1. Tomography of lensing cross power spectra

    E-Print Network [OSTI]

    Masahiro Takada; Martin White

    2004-09-14

    By obtaining photometric redshift information, tomography allows us to cross-correlate galaxy ellipticities in different source redshift bins. The cross-correlation is non-vanishing because the different bins share much of the foreground mass distribution from which, over Gpc scales, the lensing signal is built. If the redshift bins are thick enough however, the cross-correlations are insensitive to contamination from the intrinsic alignments of galaxies since these fall off rapidly on scales larger than a few tens of Mpc. We forecast how lensing tomography using only the cross-power spectra can constrain cosmological parameters compared to tomography including the auto-spectra. It is shown that the parameter errors are degraded by only O(10%) for 5 or more source redshift bins. Thus, the cross-power spectrum tomography can be a simple, model-independent means of reducing the intrinsic alignment contamination while retaining most of the constraints on cosmology.

  2. Probing the molecular basis for the functional interactions between the histone acetyltransferase Gcn5 and protein phosphatase 2A

    E-Print Network [OSTI]

    Tomlinson, Shannon Lee

    2012-01-01

    the response of gcn5? to heat stress in combination with H2Bin sensitivity to heat stress and DNA damage [reviewed in (dosage in response to heat stress, it followed that this

  3. Listing of awardee names: Active awards

    SciTech Connect (OSTI)

    Not Available

    1994-07-01

    This catalog/directory presents DOE`s procurement and assistance data system, arranged according to awardee name, bin, completion date, description of work, division, vendor ID, city, state, congressional district, contract value, obligations to date, P/S.

  4. Cleaning procedure beakers # of times cleaning acid has been used (discard after 5x)

    E-Print Network [OSTI]

    Mcdonough, William F.

    the jars, store them in Ziploc bag or plastic bin Cleaning procedure centrifuge tubes # of times cleaning droplets 5 a large number are cleaned in advance, store them in a Ziploc bag with an appropriate label #12;#12;

  5. Syntheses and Characterizations of One-Dimensional Coordination Polymers Generated from Cadmium Nitrate and Bipyridine Ligands

    E-Print Network [OSTI]

    zur Loye, Hans-Conrad

    Syntheses and Characterizations of One-Dimensional Coordination Polymers Generated from Cadmium Nitrate and Bipyridine Ligands Yu-Bin Dong, Ralph C. Layland, Mark D. Smith, Neil G. Pschirer, Uwe H. F

  6. Bounded Coordinate System Indexing for Real-time Video Clip Search

    E-Print Network [OSTI]

    Zhou, Xiaofang

    -dimensional transformation method called Bi-Distance Transformation (BDT) is introduced to utilize a pair of optimal, Peking University, China; email: bin.cui@pku.edu.cn. Permission to make digital/hard copy of all or part

  7. Vehicle Technologies Office Merit Review 2014: ATP-LD; Cummins...

    Broader source: Energy.gov (indexed) [DOE]

    Review and Peer Evaluation Meeting about ATP-LD; Cummins next generation tier 2 bin 2 diesel engine. ace061ruth2014o.pdf More Documents & Publications ATP-LD; Cummins Next...

  8. Applied Materials Develops an Advanced Epitaxial Growth System to Bring Down LED Costs

    Broader source: Energy.gov [DOE]

    With the help of DOE funding, Applied Materials has developed an advanced epitaxial growth system for gallium nitride (GaN) LED devices that decreases operating costs, increases internal quantum efficiency, and improves binning yields.

  9. Urea SCR and DPF System for Diesel Sport Utility Vehicle Meeting...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    SCR and DPF System for Diesel Sport Utility Vehicle Meeting Tier II Bin 5 DOE and Ford Motor Company Advanced CIDI Emission Control System Development Program (DE-FC26-01NT41103)...

  10. TECHNICAL BASIS DOCUMENT FOR NATURAL EVENT HAZARDS

    SciTech Connect (OSTI)

    KRIPPS, L.J.

    2006-07-31

    This technical basis document was developed to support the documented safety analysis (DSA) and describes the risk binning process and the technical basis for assigning risk bins for natural event hazard (NEH)-initiated accidents. The purpose of the risk binning process is to determine the need for safety-significant structures, systems, and components (SSC) and technical safety requirement (TSR)-level controls for a given representative accident or represented hazardous conditions based on an evaluation of the frequency and consequence. Note that the risk binning process is not applied to facility workers, because all facility worker hazardous conditions are considered for safety-significant SSCs and/or TSR-level controls.

  11. LNT or Urea SCR Technology: Which is the right technology for...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    More Documents & Publications The BMW Approach to Tier2 Bin5 Laboratory and Vehicle Demonstration of a "2nd-Generation" LNT+in-situ SCR Diesel NOx Emission Control Concept...

  12. Photoluminescence spectral study of single CdSe/ZnS Colloidal Nanocrystals in Poly(methyl methacrylate) and Quantum Dots molecules

    E-Print Network [OSTI]

    Shen, Yaoming

    2008-01-01

    in self- assembled inp quantum dots in gainp. Phys. Rev. B,in self-assembled inp quantum dots. Phys. Rev. Lett. , 86(also been observed in InP quantum dots in a Ga x In 1?x P

  13. Comparison of Conventional Diesel and Reactivity Controlled Compression Ignition (RCCI) Combustion in a Light-Duty Engine

    Broader source: Energy.gov [DOE]

    CFD modeling was used to compare conventional diesel and dual-fuel Reactivity Controlled Compression Ignition combustion at US Tier 2 Bin 5 NOx levels, while accounting for Diesel Exhaust Fluid needed to meet NOx constraints with aftertreatment.

  14. The neuronal encoding of information in the brain Edmund T. Rolls a,

    E-Print Network [OSTI]

    Rolls, Edmund T.

    . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 452 2.4.1. Smoothing or binning neuronal response data . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 452 2.4.2. The effects of limited sampling. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 452 2.4.3. Correction procedures for limited sampling

  15. Z-scan measurement for the nonlinear absorption of Bi2.55La0.45TiNbO9 thin films Hengzhi Chen a

    E-Print Network [OSTI]

    Cao, Wenwu

    a , Bin Yang a, , Mingfu Zhang b , Feiyan Wang c , Kokwai Cheah c , Wenwu Cao a,d a Center for Condensed were acquired through this procedure. The films were deposited on double-sided polished fused silica

  16. New Developments in Storage and Handling of Biomass 

    E-Print Network [OSTI]

    Bundalli, N.

    1986-01-01

    An extensive research project to derive guidelines for the design of a reliable bin-feeder system for biomass materials has been completed. The new system uses a converging mass flow hopper with a much smaller outlet ...

  17. Targeted Discovery of Glycoside Hydrolases from a Switchgrass-Adapted Compost Community

    E-Print Network [OSTI]

    Reddy, Amitha

    2012-01-01

    2004) Microbial Ecology of Compost. In: Lens P, Hamelers B,composting in a monitored compost bin. J Appl Microbiol 94:a Switchgrass-Adapted Compost Community Martin Allgaier ,

  18. Targeted discovery of glycoside hydrolases from a switchgrass-adapted compost community

    E-Print Network [OSTI]

    Allgaier, M.

    2010-01-01

    S2 Correspondence analysis of the compost bioreactor Author2004) Microbial Ecology of Compost. In: Lens P, Hamelers B,composting in a monitored compost bin. J Appl Microbiol 94:

  19. GEOTHERMAL EXPLORATION ASSESSMENT AND INTERPRETATION, KLAMATH BASIN, OREGON-SWAN LAKE AND KLAMATH HILLS AREA

    E-Print Network [OSTI]

    Stark, M.

    2011-01-01

    New York, New York, p. 290. Group Seven Incorporated, 1972,Falls and Honey Lake: Group Seven Incorporated, Golden,125-135. The O r e Bin, Group Seven, 1972, Electrical r e s

  20. Department of Energy listing of awardee names active awards as of January 6, 1994

    SciTech Connect (OSTI)

    Not Available

    1994-02-01

    The awards are listed according to awardee name, bin, completion date, description of work, division, vendor ID, city, state, congressional district, contract value, obligations to date, and P/S.