National Library of Energy BETA

Sample records for fb faber fn

  1. Journal Diffusion Factors a measure of diffusion? Tove Faber Frandsen

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    1 Journal Diffusion Factors ­ a measure of diffusion? Tove Faber Frandsen Royal School of Library In this paper we show that the measure of diffusion introduced by Ian Rowlands called the Journal Diffusion Factor (JDF) is highly negatively correlated with the number of citations, leading highly cited journals

  2. Generic Properties of Actions of F_n 

    E-Print Network [OSTI]

    Hitchcock, James Mitchell

    2011-10-21

    embeds into the tracial ultraproduct of the hyperfinite II1 factor. We conclude by showing the finite approximation result may be transferred to a subspace of the space of all topological actions of Fn on the Cantor set. Within this class, we show the set...

  3. K Planning System: Progress Report ? Thomas Eiter 1 , Wolfgang Faber 1 ,

    E-Print Network [OSTI]

    Faber, Wolfgang

    The DLV K Planning System: Progress Report ? Thomas Eiter 1 , Wolfgang Faber 1 , Nicola Leone 2 of Calabria, 87030 Rende, Italy leone@unical.it 1 Introduction The knowledge based planning system DLV K implements answer set planning on top of the DLV system [1]. It is developed at TU Wien and supports

  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. 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

  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 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

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

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

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

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

  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 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

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

  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%) presentation (20%) #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%) Protokolle (70%) presentation (30%) journal (70%) #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni

  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 Biology" . #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 percent) and computational tasks (80 percent). #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni

  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 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

  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 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

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

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

  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: 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

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

  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 Modulprüfung (MP) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie, interference) #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, Kleingruppenpräsentation presentation script and presentation #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2.uni

  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 (30%) report (70%) presentation (30%) #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: Marine invertrebrates alternating with Marine Algae. #12;FB2 Biologie / Chemie www.uni-bremen.de www.fb2

  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: 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

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

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

  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 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

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

  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 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

  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 / 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

  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 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

  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 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

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

  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: 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

  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 2014/15 Modul) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie www

  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 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

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

  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 Modulprüfung (MP) / Assessment of module (MP) or submodule (TP) Klausur written exam #12;FB2 Biologie / Chemie

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

  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, 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

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

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

  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 PM 1

  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 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

  17. The FN400 indexes familiarity-based recognition of faces Tim Curran and Jane Hancock

    E-Print Network [OSTI]

    Curran, Tim

    The FN400 indexes familiarity-based recognition of faces Tim Curran and Jane Hancock Department processes contributing to recognition memory (e.g., Hintzman and Curran, 1994; Jacoby, 1991; Mandler, 1980 potentials (for reviews see, Curran et al., 2006b; Friedman and Johnson, 2000; Mecklinger, 2000; Wilding

  18. Applications of Statistics and Probability in Civil Engineering Faber, Khler & Nishijima (eds) 2011 Taylor & Francis Group, London, ISBN 978-0-415-66986-3

    E-Print Network [OSTI]

    to uncertainties in ground motion attenua- tion. As new strong ground motion data become available, and siteApplications of Statistics and Probability in Civil Engineering ­ Faber, Köhler & Nishijima (eds, but clearly this is part of a much wider problem. Seismologists and engineers can play a key role in public

  19. Answer Set Planning under Action Costs ? Thomas Eiter 1 , Wolfgang Faber 1 , Nicola Leone 2 , Gerald Pfeifer 1 , and Axel Polleres 1

    E-Print Network [OSTI]

    Faber, Wolfgang

    Answer Set Planning under Action Costs ? Thomas Eiter 1 , Wolfgang Faber 1 , Nicola Leone 2 the declarative planning language K by action costs and optimal plans that minimize overall action costs (cheapest plans). As shown, this novel language allows for expressing some nontrivial plan­ ning tasks

  20. RATIONAL HOMOLOGY OF AUT(Fn) Allen Hatcher* and Karen Vogtmann*

    E-Print Network [OSTI]

    Hatcher, Allen

    homology in dimensions less than seven of the group of automorphisms of a finitely generated free group of arbitrary rank. The only non-zero group in this range is H4(Aut(F4); Q), which is one-dimensional. §1. Introduction In [7] a space An was introduced on which the group Aut(Fn) of automorphisms of a free group

  1. $A^t_{FB}$ 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.

  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 2014/15 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

  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 2014/15 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

  4. 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

  5. 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.

  6. 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.

  7. *DEEP team: S.Faber,G.Illingworth,D.C.Koo,R.Guhathakurta,K.Denda,K.Gebhardt,A.C.Phillips,L.Simard,C.Willmer,M.Im(UCSC) and partners in UC Berkeley, U.Chicago, JHU, and Caltech evolution for E/S0s at z < 1, contrary to the theoretical models and some obser

    E-Print Network [OSTI]

    . For more information on DEEP, check our web site at http://www.ucolick.org/~deep/home.html 4. Conclusion*DEEP team: S.Faber,G.Illingworth,D.C.Koo,R.Guhathakurta,K.Denda,K.Gebhardt,A for a reduced set of DEEP data in the Groth strip. models based on CDM dominated universe predict that 50

  8. 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

  9. 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.

  10. 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.

  11. 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.

  12. 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.

  13. 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.

  14. 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.

  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. 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

  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 Shortest­Remaining­Processing­Time (SRPT have the least attained service (a.k.a age), they time­share the processor via PS. By biasing towards

  18. Ephippidae; Chaetodipterus faber TCWC 502.06 

    E-Print Network [OSTI]

    2013-07-03

    in Hood County Introduction ...................................................................................................................................1 Project Background... ......................................................................................................................1 Project Accomplishments .............................................................................................................2 Overall Summary...

  19. 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

  20. 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 ...

  1. 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.)].

  2. 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

  3. 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

  4. 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 ...

  5. 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.

  6. 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...

  7. 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.

  8. 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 ...

  9. 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.

  10. 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

  11. 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}.

  12. 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

  13. 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

  14. 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

  15. 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.

  16. 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%.

  17. 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

  18. 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.

  19. 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.

  20. 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.

  1. 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

  2. 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}.

  3. 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

  4. 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 ...

  5. 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 ...

  6. 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...

  7. 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...

  8. 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 ...

  9. 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 ...

  10. 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

  11. 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.

  12. 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.

  13. 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

  14. 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.

  15. 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

  16. 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

  17. 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.

  18. 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\

  19. 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.

  20. LN FN ADVISOR NAME Abbott Zachary Boucheron, Laura E.

    E-Print Network [OSTI]

    Johnson, Eric E.

    Ricardo Ramirez-Angulo, Jaime Corral Christopher Brahma, Sukumar Coughlin Brandon Tang, Wei Covarrubias T. Favela Jonathan Furth, Paul M. Fernandez Tracey Furth, Paul M. #12;Fishburn Adam Ranade

  1. 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

  2. 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}.

  3. 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

  4. 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%.

  5. 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.

  6. 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.

  7. 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.

  8. 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.

  9. 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...

  10. 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. ...

  11. 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.

  12. 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.

  13. 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.

  14. 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.

  15. 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.

  16. 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

  17. 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

  18. 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.

  19. 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.

  20. Current /sup 14/C measurements with the University of Washington FN tandem accelerator

    SciTech Connect (OSTI)

    Farwell, G.W.; Grootes, P.M.; Leach, D.D.; Schmidt, F.H.; Stuiver, M.

    1983-01-01

    The accelerator mass spectrometry (AMS) system shows a one-to-one relationship between sample /sup 14/C concentrations determined by AMS - and by ..beta..-counting. Measurements of unknown samples against a standard indicate that /sup 14/C concentration measurements to better than 2% can be made. For a 30-second data collection interval in a typical run of 100 intervals, the variability of the beam injected into the accelerator is ca 2%, that of the machine transmission is ca 4%, and counting statistics give 4.7% standard deviation for a sample of 80% of modern carbon.

  1. 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

  2. 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:

  3. 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

  4. 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

  5. Math 192r, Problem Set #1: Solutions 1. (a) Write and run a program to compute f(n) = n

    E-Print Network [OSTI]

    Propp, James

    . Every plus committee can be matched up with a minus committee, and vice versa, if one simply complements we are choosing a committee of size n from a group consisting of n men and n women, and where. Let's assume that the n men and n women are married in pairs, and that the couples are num- bered 1

  6. Important Basic Equations for Order of Magnitude Estimation Conservation Laws

    E-Print Network [OSTI]

    Nimmo, Francis

    area 4r2 or d2 Sphere: volume 4 3r3 or 1 6d3 Forces Newton's Second Law F = ma Force due to gravity Fg = mg = Gm1m2 r2 Drag force Fd = 1 2cDAv2 Frictional force Ff = cf FN Buoyant force Fb = fluidV g valid for non-relativistic systems) · Energy · Linear momentum · Angular momentum Quantities Force mass

  7. Haskins Laboratories Status Report on Speech Research 1993, SR-113, 107-130

    E-Print Network [OSTI]

    , Alice Faber, Louis Goldstein, Carol Gracco, Robin Greene, Kathy Harris, Pat Nye, Alfred Opoku, Elliot

  8. 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

  9. 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

  10. 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

  11. 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__

  12. Drawing Inferences about Others Based on Corporate Social Responsibility Associations

    E-Print Network [OSTI]

    Yoon, Yeosun; Gürhan-Canli, Zeynep; Bozok, Beyza

    2005-01-01

    Faber-Castle’s support of WEO is more congruent with Faber-Environmental Organization (WEO) and is now marketing a newpens, and markers with the WEO label. Jamie realizes that

  13. Review of Results from the FN-II Dense Plasma Focus Machine J.J.E. Herrera, F. Castillo, I. Gamboa, J. Rangel

    E-Print Network [OSTI]

    Boyer, Edmond

    the early days of plasma focus research that the origin of such neutrons is not necessarily thermonuclear

  14. Math 192r, Problem Set #1: Solutions 1. (a) Write and run a program to compute f(n) = P n

    E-Print Network [OSTI]

    Propp, James

    : n is odd. Every plus committee can be matched up with a minus committee, and vice versa, if one of signed counting, where we are choosing a committee of size n from a group consisting of n men and n women II: n is even, with n = 2m. Let's assume that the n men and n women are married in pairs

  15. Reliable Broadcast in a Wireless Grid Network with Probabilistic Failures

    E-Print Network [OSTI]

    Vaidya, Nitin

    . Then: lng = nln(1+ f(n) n ) = n f(n) n - 1 2 ( f(n) n )2 + 1 3 ( f(n) n )3 -.... [1] = n k=1 (-1)k-1 4 lng = nln(1+ f(n) n ) = n f(n) n - 1 2 ( f(n) n )2 + 1 3 ( f(n) n )3 -.... [1] = n k=1 (-1)k-1 1 k ( f(n) n )k = f(n)+ k=2 (-1)k-1 1 k ( f(n)k nk-1 ) lim n lng = lim n f(n)+ k=2 (-1)k-1 1 k ( f

  16. 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

  17. 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

  18. '('()%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

  19. 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

  20. 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...

  1. Modern Peoplehood: On Race, Racism, Nationalism, Ethnicity, and Identity

    E-Print Network [OSTI]

    Lie, John

    2011-01-01

    Faber. Miles, Robert. 1989. Racism. London: Routledge. ———.1993. Racism after “Race Relations”. London: Routledge.Asante, Molefi Kete. 1993. “Racism, Consciousness, and

  2. Answer

    E-Print Network [OSTI]

    2014-12-09

    Question 2 (10 points): Consider the sequence of functions fn : E1 ? E1 given by fn(x) = e?nx sin(nx). Prove that ? fn converges uniformly on [1, +?). Answer: ...

  3. -Oak Ridge National l. oy [EFECT%W flHSUia-9PI gi)N~PCOEjJIR!.,o tS N9IN FN_RWiD)LCTH pgR^ s -

    E-Print Network [OSTI]

    Oak Ridge National Laboratory

    , and cooler) of a I maximum velocity of fluid based on cross- Stirling engine properly. Two major design goals occurring in a real Stirling engine. Irmiance of the GPU-3 and 41.3 enginoe is dii- The effects of pressure 7 ABSItA(I' For ;:Ipo flow Pressure-drop correltl ons for Stirling-en-- I nondimensional variable

  4. mRNA Display selection of a novel activated leukocyte cell adhesion molecule (ALCAM) binding protein from a modified combinatorial protein library based on the tenth domain of human fibronection III (10FnIII)

    E-Print Network [OSTI]

    Park, Ann

    2015-01-01

    Activated Leukocyte Cell Adhesion Molecule (ALCAM)-Positiveof activated leukocyte-cell adhesion molecule (ALCAM), a CD6Activated leukocyte cell adhesion molecule (CD166/ALCAM):

  5. fn{EE49F893-CA64-40D2-9A32-E9DA8936271E}EIMS+Content&dbwisle@srn.sandia.gov.vsd

    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 WebQuantity ofkandz-cm11 Outreach Home RoomPreservationBio-Inspired SolarAboutXu Named| Princetondefault Sign InEnhanced OilProject Errors

  6. TD M41 Series Serie 3 Suites de fonctions

    E-Print Network [OSTI]

    Berglund, Nils

    1 + (x + n)2 ; 2. fn(x) = 1 - xn 1 + xn , x 0; 7. fn(x) = 1 nx2 + 1 ; 3. fn(x) = x n(1 + xn) ; 8. fn(x) = sin(nx) nx , x > 0; 4. fn(x) = nx 1 + n2x ; 9. fn(x) = (log x)2n - 2 (log x)2n + 2 , x > 0; 5. fn(x) = nx3 1 + nx2 ; 10. fn(x) = x2 e-x/n ; Exercice 2 D´eterminer pour lesquelles des suites de fonctions

  7. USC/ISI Technical Report ISI-TR-696 March 18, 2015 Implementation of the TCP Extended Data Offset Option

    E-Print Network [OSTI]

    Touch, Joe

    USC/ISI Technical Report ISI-TR-696 March 18, 2015 Implementation of the TCP Extended Data Offset Option Harry Trieu, Joe Touch, Ted Faber USC/ISI 4676 Admiralty Way, Suite 1001 Marina del Rey, CA 90292 310-822-1511 htrieu@usc.edu, touch@isi.edu, faber@isi.edu ABSTRACT TCP Extended Data Offset (EDO

  8. 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

  9. 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...

  10. 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...

  11. 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

  12. 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...

  13. 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\

  14. 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

  15. 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.

  16. MATH 472 STATISTICAL INFERENCE UNIVERSITY OF HAWAII AT MANOA

    E-Print Network [OSTI]

    Faber, Xander

    MATH 472 ­ STATISTICAL INFERENCE UNIVERSITY OF HAWAII AT MANOA SPRING 2013 Professor Info: Dr. Xander Faber 404 Physical Sciences Building xander@math.hawaii.edu www.math.hawaii.edu/xander/ Office

  17. MATH 140 PRECALCULUS UNIVERSITY OF HAWAII AT MANOA

    E-Print Network [OSTI]

    Faber, Xander

    MATH 140 ­ PRECALCULUS UNIVERSITY OF HAWAII AT MANOA FALL EXTENSION 2012 Professor Info: Dr. Xander Faber 404 Physical Sciences Building xander@math.hawaii.edu http://www.math.hawaii.edu/xander/ Office

  18. MATH 471 PROBABILITY UNIVERSITY OF HAWAII AT MANOA

    E-Print Network [OSTI]

    Faber, Xander

    MATH 471 ­ PROBABILITY UNIVERSITY OF HAWAII AT MANOA FALL 2012 Professor Info: Dr. Xander Faber 404 Physical Sciences Building xander@math.hawaii.edu www.math.hawaii.edu/xander/ Office Hours -- MW 10

  19. MATH 480O SENIOR SEMINAR UNIVERSITY OF HAWAII AT MANOA

    E-Print Network [OSTI]

    Faber, Xander

    MATH 480O ­ SENIOR SEMINAR UNIVERSITY OF HAWAII AT MANOA SPRING 2013 Professor Info: Dr. Xander Faber 404 Physical Sciences Building xander@math.hawaii.edu www.math.hawaii.edu/xander/ Office Hours

  20. MATH 111 MATH FOR ELEMENTARY TEACHERS I UNIVERSITY OF HAWAII AT MANOA

    E-Print Network [OSTI]

    Faber, Xander

    MATH 111 ­ MATH FOR ELEMENTARY TEACHERS I UNIVERSITY OF HAWAII AT MANOA FALL 2012 Professor Info: Dr. Xander Faber 404 Physical Sciences Building xander@math.hawaii.edu www.math.hawaii

  1. BIOCATALYSIS AND METABOLIC ENGINEERING CHEM /6760 Spring

    E-Print Network [OSTI]

    Sherrill, David

    in science and engineering. REQUIRED Biotransformations in Organic Chemistry, Kurt Faber TEXTS: Springer, 5th of pharmaceutical intermediates II 18 03/11 Biocatalysis in agriculture and in the food industry 19 03

  2. 2008 FERC Published ASCM_FRN_74_FR_47052-01_9-30-09_1741

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

    nor its legislative history explains the nature of this review. FN7 FN7 Methodology for Sales of Electric Power to Bonneville Power Administration, Order No. 400, FERC Stats. &...

  3. Departamento de Matematica, Universidad Tecnica Federico Santa Maria

    E-Print Network [OSTI]

    Markina, Irina

    necesito mostrar que {fn} tiene que convergerse uniformamente a 0. 2) Haga las construcciones: i) de una

  4. Multidimensional Divide-and-Conquer and Weighted Digital Sums

    E-Print Network [OSTI]

    Flajolet, Philippe

    - and-conquer problems originally developed in [4] (see [5] for a review of more recent innovations arises naturally in the analysis of binomial queues where Brown [6] gave upper and lower bounds n lg n-and-conquer recurrences of the form (2.6) fn = fn/2 + fn/2 + en with initial condition f1 = 0 and given "conquer" cost

  5. 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 ...

  6. 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 ...

  7. 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 = ...

  8. 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, ...

  9. 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...

  10. 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 ...

  11. 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 ...

  12. 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...

  13. 11601. For any prime p and positive integer n, let N(p, n) denote the dif-ference between the number of p's appearing as factors in the denominator

    E-Print Network [OSTI]

    Karaivanov, Borislav

    11601. For any prime p and positive integer n, let N(p, n) denote the dif- ference between the number of p's appearing as factors in the denominator of Fn and the number of those appearing in the numerator of Fn. Clearly, Fn is an integer if and only if N(p, n) 0 for all primes p. The idea of the proof

  14. Directed Generalized Measure of Association: A Data Driven Approach Towards Causal Inference

    E-Print Network [OSTI]

    Slatton, Clint

    ) and later Cartwright (1979) defined causality as: C causes E iff P(E|C ± F1 ± . . . ± Fn) > P(E| C ± F1 ± . . . ± Fn) where {F1 ±. . .±Fn, C} is a complete causal set for E. There are potential counterexamples Mehrnaz Kh. Hazrati* Jos´e C. Pr´incipe Department of Electrical and Computer Engineering University

  15. My lecture at the Conference on Algebraic Complexity in the memory of Jacques Morgenstern, INRIA Sophia Antipolis, France May 1995.

    E-Print Network [OSTI]

    Kaltofen, Erich

    , . . .} is generated by a linear recursion #12;Theorem (Wiedemann 1986): For random u, v Fn , a linear generator high probability) c0Bj v + c1Bj+1 v + · · · + cdBj+d v = 0 (with high probability) c0Bj + c1Bj+1 Fn×n singular Output: w = 0 such that Bw = 0 Step W1: Pick random u, v Fn ; b Bv; for i 0 to 2n

  16. 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

  17. Highly Efficient Cardiac Differentiation of Human Embryonic Stem Cells for Cardiac Repair

    E-Print Network [OSTI]

    Sa, Silin

    2013-01-01

    gelatin. .70:30 FN:LN compared with gelatin increased the number of p-days. Plate 7-day-old EBs on gelatin- coated tissue culture

  18. Integrin and extracellular matrix interactions at the maternal conceptus interface in pigs 

    E-Print Network [OSTI]

    Garlow, Jane Elizabeth

    2002-01-01

    . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 59 3. 5 Detection of OPN protein in the porcine uterine and conceptus using immunofluorescence staining of frozen uterine or conceptus sections with the cocktail of rabbit anti-human OPN antibody (LF-123 + LF-124). 61 3. 6 Integrin receptor... is mutated to RAD, FN or to an irrelevant protein, BSA. . 4. 3 Effect of FN on phosphorylation of Akt in pTrl cells. . . . . 86 4. 4 Effect of FN on phosphorylation of ERK1 and ERK2 in pTrl cells. 87 4. 5 Effect of FN on phosphorylation of ERKI and ERKZ...

  19. On the singularities of the inverse to a meromorphic function of finite ...

    E-Print Network [OSTI]

    2015-08-26

    scendental meromorphic function in the complex plane. If f has ... that if f is a transcendental meromorphic function then f/fn with ... The following classification.

  20. The DEEP2 Galaxy Redshift Survey: Overview

    E-Print Network [OSTI]

    The DEEP2 Galaxy Redshift Survey: Overview David C. Koo & DEEP2 Team UCO/Lick Observatory. Univ. of California, Santa Cruz AAS Seattle Jan 2003 DEIMOSKECK #12;l What is DEEP2 ? l What are its Scientific Goals? l What is its Current Status? #12;The DEEP2 Collaboration Team Members: M. Davis (PI, UCB), S. Faber

  1. Journal self-citations -analysing the JIF mechanism

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    1 Journal self-citations - analysing the JIF mechanism Tove Faber Frandsen1 tff@db.dk Department investigates the mechanism of the Journal Impact Factor (JIF). Although created as a journal selection tool the indicator is probably the central quantitative indicator for measuring journal quality. The focus is journal

  2. Journal interaction A bibliometric analysis of economics journals

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    1 Journal interaction A bibliometric analysis of economics journals Tove Faber Frandsen1 Royal journals. The proposed method controls for the different characteristics of the journals as well Author manuscript, published in "Journal of Documentation 61, 3 (2005) 385-401" #12;2 economics

  3. Back to article page Steven Shapin

    E-Print Network [OSTI]

    Shapin, Steven

    and Politics by Graham Farmelo Faber, 554 pp, £25.00, October, ISBN 978 0 571 24978 7 Winston Churchill diverted to Britain's nuclear weapons programme. The Americans remained preoccupied in the Pacific, still's only nuclear power, and the gun-method Page 1 of 11Steven Shapin reviews `Churchill's Bomb' by Graham

  4. Abstract--Removing artifacts from biomedical signals, such as surface electromyography (sEMG), has become a major

    E-Print Network [OSTI]

    become a major research topic in biomedical signal processing. In electromyography signals, a source.taelman@ faber.kuleuven.be). S. Van Huffel is head of the biomedical signal processing group at the ElectricalAbstract-- Removing artifacts from biomedical signals, such as surface electromyography (sEMG), has

  5. Y AGRGATION INTERNE DE MATHMATIQUES Y Suites et sries de fonctions Samedi 16 Juin 2012.

    E-Print Network [OSTI]

    Lassere, Patrice

    dénies sur R par fn(x) = 2n 1 + x2n. (5) Y On pose pour n N : fn(x) = n + 1 sinn (x) cos(x). Montrer [-a, a] pour tout a > 0. Exercice 5. Soit f C 0 (R+) vériiant f(0) = 0 = lim+ f(x). On pose pour n N

  6. 6.001, Spring 2004---Recitation 4 1 MASSACHVSETTS INSTITVTE OF TECHNOLOGY

    E-Print Network [OSTI]

    Liskov, Barbara

    6.001, Spring 2004---Recitation 4 1 MASSACHVSETTS INSTITVTE OF TECHNOLOGY Department of Electrical Recitation 4 Orders of Growth Definitions Theta (#) notation: f(n) = #(g(n)) # k 1 · g(n) # f(n) # k 2 · g. For a sum, take the larger term. For a product, multiply the two terms. Orders of growth are concerned

  7. 6.001, Spring 2004--Recitation 4 1 MASSACHVSETTS INSTITVTE OF TECHNOLOGY

    E-Print Network [OSTI]

    Liskov, Barbara

    6.001, Spring 2004--Recitation 4 1 MASSACHVSETTS INSTITVTE OF TECHNOLOGY Department of Electrical Recitation 4 Orders of Growth Definitions Theta () notation: f(n) = (g(n)) k1 · g(n) f(n) k2 · g(n), for n, take the larger term. For a product, multiply the two terms. Orders of growth are concerned with how

  8. Some Teasers ffl Which is the ``best'' hyperplane that separates

    E-Print Network [OSTI]

    Roweis, Sam

    ` ) that are drawn i.i.d from P (x; y). ffl Empirical risk minimization (ERM) method: Pick ff ` which minimizes ` (we hope). ffl The method of ERM is not new: Least Squares is ERM for Regression loss fn. Maximum Likelihood is ERM for Density loss fn. Minimizing training error (e.g. in ANN) is ERM for Classification loss

  9. The Digital Signature Scheme MQQ-SIG Intellectual Property Statement and Technical Description

    E-Print Network [OSTI]

    International Association for Cryptologic Research (IACR)

    . Bijective multivariate quadratic mapping P (x) Input: A vector x = (f1, . . . , fn) of n linear Boolean, . . . , xn), i = 9, . . . , n 1. Represent a vector x = (f1, . . . , fn) of n linear Boolean functions of n and Electrical Engineering, The Norwegian University of Science and Technology (NTNU), O.S.Bragstads plass 2E, N

  10. Syllabus Analyse B2 door T. H. Koornwinder

    E-Print Network [OSTI]

    Wiegerinck, Jan

    , 1990. [5] W. Rudin, Principles of mathematical analysis, McGraw-Hill, Third ed., 1976. [6] W. Walter functierij (fn) n=1 convergeert puntsgewijs op X naar een limietfunctie f op X als voor elke x X geldt dat als er voor elke > 0 een natuurlijk getal N bestaat zo dat voor alle n N geldt dat |f(x) - fn

  11. Role of hypoxia and hypoxia induced factors in the development of breast cancer brain metastasis 

    E-Print Network [OSTI]

    Lungu, Gina Florentina

    2009-05-15

    /41 C-II, II, III, X Collagenase 2 MMP8 5/64 C-I, II, III Collagenase 3 MMP13 65/55 C-I, II, IV, X, XIV, FN, aggrecan, tenascin Stromelysin Stromelysin 1 MMP3 57/45,28 PG, FN, C-III, IV, VII, IX, Gelatin, LN Stromelysin 2 MMP10 56/47,24 C...-III, IV, V, gelatin, PG, FN Gelatinase Gelatinase A MMP2 72/67 Gelatin, C-IV, FN, PG, LN Gelatinase B MMP9 92/67 Gelatin, C-III, IV, V, elastin Matrylisin Matrylisin 1 MMP7 28/19 Gelatin, C-IV, FN, PG, LN Matrylisin 2 MMP26 29/19 Gelatin, C...

  12. 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

  13. 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

  14. 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

  15. 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

  16. Studies of a contact zone among three chromosome races of Geomys bursarius in Eastern Texas 

    E-Print Network [OSTI]

    Tucker, Priscilla Kate

    1980-01-01

    : Dr. David J. Schmidly A zone of contact among three chromosome races of ~Geom s bursarius designated. as races E(2N=74, FN=72), F(2N=70, FN=74), and. G(2N=70, FN=72), was located in Burleson County, Texas. Interactions between race E and rs. ces F-G... be unrecognized backcross and F2 individuals). No karyotypcially detectable beckcross or F individuals are known to occur except in the fetal state. Norphologically race E and. races F-G could. not be separated definitively, although two general groupings were...

  17. ORIGINAL PAPER P. R. Territo J. Altimiras

    E-Print Network [OSTI]

    Altimiras, Jordi

    - metamorphic climax). Surface area [8.5 mm2 at stages Nieuwkoop-Faber (NF) 33±34 to 70.2 mm2 at stages NF 50±51 (hemoglobin poisoning with carbon monoxide), whole animal surface area and volume were measured and bulk] and volume (1.8 mm3 at stages NF 33±34 to 35.7 mm3 at stages NF 50±51) measured from volu- metric analysis

  18. Accelerator mass spectrometry program at the University of Washington

    SciTech Connect (OSTI)

    Farwell, G.W.; Leach, D.D.; Grootes, P.M.; Schmidt, F.H.

    1984-04-10

    The University uses an FN-Tandem for /sup 14/C and /sup 10/Be measurements. Three main problems for accelerator-mass-spectrometry are normalization, stability, and sample preparation. The approach to these problems is discussed. (GHT)

  19. ACTICA 1. B ' USQUEDA HEUR'iSTICA

    E-Print Network [OSTI]

    Barreiro, Alvaro

    algunas variantes sencillas. El objeto del puzzle es mover las casillas sobre el espacio vac'io (o casilla­NODO(ESTADO­INICIAL[problema])) loop if nodos vacio then return fallo nodo / EXTRAE­FRENTE­COLA(nodos) if FN

  20. Controlling Methane Emissions in the Natural Gas Sector: A Review...

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

    to 93% methane by mass. NETL, 2012. Role of Alternative Energy Sources: Natural Gas Technology Assessment. See ICF, supra note 11 at 78, fn. 40. 39 This report is available...

  1. Performance Based Implementation of Seismic Protective Devices for Structures

    E-Print Network [OSTI]

    Xi, Wang

    2014-01-01

    Superstition Hills Los Gatos 1989 Loma Prieta Cape MendocinoTest Site (FP), 1987 Superstition Hills Los Gatos (FN), 1989Loma Prieta Los Gatos (FP), 1989 Loma Prieta Cape

  2. ANTONELLA DEL ROSSO C'era una volta Leonardo

    E-Print Network [OSTI]

    Garibaldi, Skip

    cosmici che ci colpiscono ad altissima energia? Qual è la natura profonda della gravità e il ruolo nei Sasso (Lngs) e all'Istituto Na- zionale di Fisica Nucleare (In- fn). Installati a 1400 metri sot- to la

  3. On the Convergence Rate of Multi-Block ADMM Shuzhong Zhang

    E-Print Network [OSTI]

    Ferguson, Thomas S.

    the following multi-block convex minimization problem: min f1(x1) + f2(x2) + · · · + fN (xN ) s.t. A1x1 + A2x2 (1.2) converges if all the functions f1, . . . , fN are further assumed to be strongly convex. Department of Systems Engineering and Engineering Management, The Chinese University of Hong Kong, Shatin

  4. Termination of Mutually Recursive Functions Andreas Abel

    E-Print Network [OSTI]

    Abel, Andreas

    ) Wellfounded part WF S: w 2 WF >:()6 9f : N ! S. f(0) = w ^ 8n 2 N. f(n) > f(n + 1: half' = RN (~xB . 0) (~xN ~fB!N . RB (f true) (1 + (f false))) half = ~nN . half' n 1 = 0 half n+2 = (half n)+1 But: syntax permits non-total functions

  5. CS 376 Programming with Abstract Data Types Solutions to Coursework 1

    E-Print Network [OSTI]

    Berger, Ulrich

    ! booleg The BOOLE-algebra Boole is given by Boole boole = B, T Boole = #t, F Boole = #f , not Boole (p) = :p, and Boole (p; q) = p ^ q, or Boole (p; q) = p _ q, for all p; q 2 B. The BOOLE-algebra Pow := fn 2 N j n 2 X and n 2 Y g X [ Y := fn 2 N j n 2 X or n 2 Y g (b) BOOLE := (S; where S := fbooleg

  6. 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 ...

  7. 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

  8. 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

  9. The TLR4 agonist fibronectin extra domain A is cryptic, exposed by elastase-2; use in a fibrin matrix cancer vaccine

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

    Julier, Ziad; Martino, Mikaël M.; de Titta, Alexandre; Jeanbart, Laura; Hubbell, Jeffrey A.

    2015-02-24

    Fibronectin (FN) is an extracellular matrix (ECM) protein including numerous fibronectin type III (FNIII) repeats with different functions. The alternatively spliced FN variant containing the extra domain A (FNIII EDA), located between FNIII 11 and FNIII 12, is expressed in sites of injury, chronic inflammation, and solid tumors. Although its function is not well understood, FNIII EDA is known to agonize Toll-like receptor 4 (TLR4). Here, by producing various FN fragments containing FNIII EDA, we found that FNIII EDA's immunological activity depends upon its local intramolecular context within the FN chain. N-terminal extension of the isolated FNIII EDA with itsmore »neighboring FNIII repeats (FNIII 9-10-11) enhanced its activity in agonizing TLR4, while C-terminal extension with the native FNIII 12-13-14 heparin-binding domain abrogated it. We reveal that an elastase 2 cleavage site is present between FNIII EDA and FNIII 12. Activity of the C-terminally extended FNIII EDA could be restored after cleavage of the FNIII 12-13-14 domain by elastase 2. FN being naturally bound to the ECM, we immobilized FNIII EDA-containing FN fragments within a fibrin matrix model along with antigenic peptides. Such matrices were shown to stimulate cytotoxic CD8+ T cell responses in two murine cancer models.« less

  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. 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

  16. 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...

  17. 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...

  18. 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...

  19. 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

  20. The variability of fly ash and its effects on selected properties of fresh Portland cement/fly ash mortars 

    E-Print Network [OSTI]

    McKerall, William Carlton

    1980-01-01

    for air content testing for 15 cubic feet of mortar per cubic yard of concrete 44 13 Summary of samples failing to meet ASTM C-618 uniformity specifications for specific gravity and fineness Average and relative rankings of flow, set, and air... of Energy (2). C Faber and Styron (9). Figure 2. Photomicrograph of' f'l y ash from sub-bituminous coal exposed to moisture ior seven days. 14 ~Sit'i ti ASTM recommends speci f1cat1ons for both class F and class C fly ashes (8). Tables 3 and 4 list...

  1. A Review of Annual Review of Astronomy and Astrophysics, Volume 52, 2014

    E-Print Network [OSTI]

    Rao, A R

    2015-01-01

    A review of the Annual Review of Astronomy and Astrophysics Volume 52, 2014 (Ed. S.M. Faber, Ewine van Dishoeck, and John Kormendy) is given, with a perspective of understanding the current trends in Astronomy and Astrophysics. The impact of high volume data, high connectivity, and fast computations is clearly seen in the various research areas discussed in this volume. This has provided unprecedented development in the understanding of various astrophysical phenomena. At the same time, some negative trends like commodification of science, ignoring dissenting views are also evident.

  2. From Globalisation to Liquidation: The Deutsch-Asiatische Bank and the First World War in China

    E-Print Network [OSTI]

    Moazzin, G.

    2015-07-30

    of the liquidation regulations that excluded enemy debtors from the liquidation. The Times article called on the Allied governments to “enforce the liquidation of the Deutsch- Asiatische Bank,” which it called the “keystone of the German commercial system in China... Faber asked Foreign Secretary Balfour “why the Deutsch- Asiatische Bank, which is the keystone of the German commercial system in China, has not been put into liquidation; and when it is likely to be so put?” Balfour’s reply was that the Allied...

  3. Exact polynomial system solving for robust geometric computation 

    E-Print Network [OSTI]

    Ouchi, Koji

    2007-04-25

    (f1,...,fn) to be the non- zero coefficient of the lowest degree term in TGCP (s,u) regarded as a polynomial in variable s. Theorem 2.1. Rojas ([81] Main Theorem 2.4) TPert (u) is well-defined, i.e., for a given square system of polynomials f1,...,fn... for the degree of DOCTOR OF PHILOSOPHY Approved by: Co-Chairs of Committee, Donald Friesen John Keyser Committee Members, Jianer Chen J. Maurice Rojas Head of Department, Valerie E. Taylor December 2006 Major Subject: Computer Science iii ABSTRACT Exact...

  4. Genic differentiation among chromosomally characterized mainland Peromyscus from the Pacific Northwest 

    E-Print Network [OSTI]

    Ensink, Jan

    1987-01-01

    subdivided into H (high FN) and L (low FN) populations since these were localities at which P. oreas and P. m. austerus were sympatric Proteins assayed, buffer systems, running conditions, and tissue types used, and the presumptive gene loci scored... and P. maniculatus. In order to provide P d p p l l l d -~p Pl*, * l populations of P. maniculatus subspecies from east of the oreas- austerus range were also included in this analysis. MATERIALS AND METHODS 41 f94 p*' f~pd709 1 f P, m. austerus...

  5. The historical accentuation of masculine nouns in ?akavian and Štokavian Dalmatian dialects in light of Deanovi?’s Lingvisti?ki atlas Mediterana

    E-Print Network [OSTI]

    Schallert, Joseph

    2014-11-01

    ) and Ranko Marinkovic?, a writer and native of Vis (Deanovc? 1966: 10). Previous citation: Langston (2006: 261, fn. 26) refers to D 1966, but does not cite examples. Some of Deanovic?’s data for Komiža are also cited by Hraste and Šimunovic? (1979...) and Ranko Marinkovic?, a writer and native of Vis (Deanovc? 1966: 10). Previous citation: Langston (2006: 261, fn. 26) refers to D 1966, but does not cite examples. Some of Deanovic?’s data for Komiža are also cited by Hraste and Šimunovic? (1979...

  6. 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.

  7. 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

  8. 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

  9. 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

  10. 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).

  11. 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...

  12. 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-

  13. 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 ?

  14. Resource personnel available and a plan for their use 

    E-Print Network [OSTI]

    Booth, Chester Eli

    1960-01-01

    caupile e liat of capable ~ aho cme cCLD Ieg Co eeaiat vacational ~toto dapcctccsnna fn pan@ding in- fecumtfon to adult seal pcs' Caner ~. avoca none hse Sean aaecaessaLad co as Iy' Sr 01if Aalaanqn, 8aoagm of Chs ~1tccaei Qepacaseat& @neaten...

  15. THE FOURIER ENTROPY-INFLUENCE CONJECTURE HOLDS FOR A LOGDENSITY 1 CLASS OF CRYPTOGRAPHIC

    E-Print Network [OSTI]

    International Association for Cryptologic Research (IACR)

    THE FOURIER ENTROPY-INFLUENCE CONJECTURE HOLDS FOR A LOG­DENSITY 1 CLASS OF CRYPTOGRAPHIC BOOLEAN FUNCTIONS SUGATA GANGOPADHYAY AND PANTELIMON STANICA Abstract. We consider the Fourier Entropy . The algebraic degree of f is deg(f) = max aFn 2 {wt(a) : µa = 0}. The Fourier transform or the Fourier

  16. Answers for Homework Handout for unit 4 Work and Energy

    E-Print Network [OSTI]

    Mansell, Edward "Ted"

    the net work is zero: Wapp = mg(y) = 330 J. 4. The spring constant comes from Fapp = k(x); k = (200 N)/(0 ), and FN does zero work because it is perpendicular to the displacement (cos 90 = 0). Work-energy tells us doing work are the applied force and gravity, and the net work is zero (constant velocity).] 10

  17. Response of the Femur to Exercise During Recovery Between Two Bouts of Hindlimb Unloading in Adult Male Rats 

    E-Print Network [OSTI]

    Gonzalez, Estela

    2012-10-19

    of BMC increased following exercise recovery above AC at the FN and DFM. Ambulatory recovery values revealed incomplete recovery in total and cortical BMC at the DFM and full recovery in other parameters. DFM and FD vBMD data indicated there were further...

  18. ACTICA 1. B ' INTELIGENCIA ARTIFICIAL

    E-Print Network [OSTI]

    Barreiro, Alvaro

    estrategias de b'usqueda. El objeto del puzzle es mover las casillas sobre el espacio vac'io (o casilla en­NODO(ESTADO­INICIAL[problema])) loop if nodos vacio then return fallo nodo / EXTRAE­FRENTE­COLA(nodos) if FN

  19. Annals of Nuclear Energy, Vol. 7, pp. 535 to 539 Pergamon Press Ltd. 1980. Printed in Great Britain

    E-Print Network [OSTI]

    Siewert, Charles E.

    ON MULTI-MEDIA CALCULATIONS IN THE THEORY OF NEUTRON DIFFUSION J. R. MAIORINO* and C. E. SIEWERT NuclearAnnals of Nuclear Energy, Vol. 7, pp. 535 to 539 Pergamon Press Ltd. 1980. Printed in Great Britain) Abstract--The FN method is used to solve the critical problem for a three-region reactor and to compute

  20. CS 2223 B term WPI Nov 6 -10 minute look back at (asymptotic) code analysis

    E-Print Network [OSTI]

    Dougherty, Daniel J.

    CS 2223 B term WPI Nov 6 Today: ! - 10 minute look back at (asymptotic) code analysis ! - then on to Quicksort 1 #12;a quick look back at analyzing code (by popular demand) Here is a recipe for arriving the worst: the cost here is O(*max* f(n), g(n)). ! 2 #12;a quick look back at analyzing code (by popular

  1. Central Limit Theorem for the Size of the Range of a Renewal Process

    E-Print Network [OSTI]

    Hitczenko, Pawel

    Central Limit Theorem for the Size of the Range of a Renewal Process Pawe l Hitczenko 1;2 ;3 Robin Subject classi#12;cation: 60K05, 60J10, 60F05 Running headline: CLT for the range of a renewal process 1 gn := fn Æ #1; #1; #1; Æ f 1 has been studied in various contexts. It models the coalescence

  2. Modeling of time dependence of hole current and prediction of QBD and tBD for thin gate MOS devices based upon

    E-Print Network [OSTI]

    Schroder, Dieter K.

    near the hole charge trapped interface during F±N tunneling of electrons. The ®eld at the localized yield, ®rst order trapping kinetics and dierent tunneling conditions for determining the time variation for evaluating the time dependence of injected electron and generated substrate hole current under constant

  3. Effects of electrical stress on mid-gap interface trap density and capture cross sections in n-MOSFETs characterized

    E-Print Network [OSTI]

    Lee, Jong Duk

    stress. The decrease of mid-gap trap cross sections following the F­N tunneling injection is found. OurEffects of electrical stress on mid-gap interface trap density and capture cross sections in n-dong, Kwanak-gu, Seoul 151-742, South Korea b Department of Electronics Engineering, Sejong University, 98

  4. TDDB AT LOW VOLTAGES: AN ELECTROCHEMICAL PERSPECTIVE

    E-Print Network [OSTI]

    Bazant, Martin Z.

    tail of the lifetime distribution2 ). Typical electron injection mechansms include Schottky emission and Fowler- Nordheim (FN) tunneling and transport in conduction band (CB) of dielectric is Poole-Frenkel (PF) in presence of traps. Carrier heating in CB and thermalization can lead to formation of additional traps

  5. Journal of the Korean Physical Society, Vol. 44, No. 1, January 2004, pp. 4649 Effects of Electrical Stress on the Mid-Gap Interface

    E-Print Network [OSTI]

    Lee, Jong Duk

    -N) electrical stress. A decrease in the mid-gap trap cross-sections following F-N tunneling injection is found of Electrical Stress on the Mid-Gap Interface Trap Density and the Capture Cross Sections Characterized University, Seoul 151-742 Woo Suk Hyun and Sang Sik Park Department of Electronics Engineering, Sejong

  6. 258 IEEE TRANSACTIONS ON NANOTECHNOLOGY, VOL. 2, NO. 4, DECEMBER 2003 Fabrication and Program/Erase Characteristics of

    E-Print Network [OSTI]

    Lee, Jong Duk

    --Band-to-band (BTB), channel hot electron (CHE) injection, F­N tunneling, hole injection, nonvolatile memory, sil-nm SONOS devices, channel hot electron injection program mechanism is inefficient and 2-b operation based on localized carrier trapping in the nitride film is difficult. The erase speed is improved

  7. Measurement of spin diffusion length in sputtered Ni films using a special exchange-biased spin valve geometry

    E-Print Network [OSTI]

    Birge, Norman

    valve geometry Charles E. Moreaua Department of Physics, Albion College, Albion, Michigan 49224 Ion C exchange-biased spin valve geometry that inserts a Ni "spoiler" layer into a Py/Cu/Py spin valve. Fits In the context of ferromagnetic/nonmagnetic F/N multilayers or spin valves, the size of the giant

  8. Large x physics: recent results and future plans Roy J. Holt

    E-Print Network [OSTI]

    Heller, Barbara

    2 Fp 2 x1 = 1 + 4(dv/uv) 4 + (dv/uv) . (1) Thus a measurement of the neutron and proton structure, the planned measurements of the Fn 2 /Fp 2 and d/u ratios as well as present status; Secondly, measurements of the longitudinal spin asymmetries for #12;the proton and neutron, while the third, the planned measurements

  9. Finite Fields and Their Applications 23 (2013) 80102 Contents lists available at SciVerse ScienceDirect

    E-Print Network [OSTI]

    Ghorpade, Sudhir

    2013-01-01

    Bombay, Powai, Mumbai 400076, India b Department of Mathematics, Indian Institute of Science Education(n,Fq)) such that cM C for all c C. Finally, Aut(C) consists of compositions M of (linear maps corresponding to) monomial matrices M GL(n,Fq) and field au- tomorphisms of Fq (giving maps of Fn q into itself by acting

  10. ANALISI MATEMATICA I MODULO CORSO DI LAUREA IN INFORMATICA

    E-Print Network [OSTI]

    Boccuto, Antonio

    ANALISI MATEMATICA I MODULO CORSO DI LAUREA IN INFORMATICA I prova scritta di settembre 2012 f(n) 2 n · n n + 1 . #12;ANALISI MATEMATICA I E II MODULO CORSO DI LAUREA IN INFORMATICA I prova IN INFORMATICA I prova scritta di settembre 2012 ESERCIZIO - (8 punti) Sia q il numero delle lettere del vostro

  11. Evidence for a Supershear Transient during the 2002 Denali Fault Earthquake

    E-Print Network [OSTI]

    Carlson, Jean

    Evidence for a Supershear Transient during the 2002 Denali Fault Earthquake Eric M. Dunham subshear slip pulse on the fault. Introduction On November 3, 2002, a Mw 7.9 earthquake shook central than FN. This is not typical of large strike-slip earthquakes, as discussed by Archuleta and Hartzell

  12. NORPAC Hydrographic Data Report of the Scripps Institution of Oceanography, University of California, and the South Pacific Fishery Investigations, U. S. Fish and Wildlife Service, for the NORPAC cruise of August-September 1955.

    E-Print Network [OSTI]

    Scripps Institution of Oceanography

    1956-01-01

    s t i t u t i o n of Oceanography; manuscript) ThermostericSCRIPPS INSTITUTION OF OCEANOGRAPHY La J o l l a , C a l i fn s t i t u t i o n of Oceanography, University of C a l i f

  13. Optimal Hlderian functional central limit theorems for uniform empirical and quantile

    E-Print Network [OSTI]

    Suquet, Charles

    Fn between its consecutive jumps). Denote by Gpg n the polygonal uniform sample quantile function) - t , pg n (t) := n Gpg n (t) - t , t [0, 1]. It is well known that pg n and pg n converge in law to B

  14. Optical dating of St. Lawrence Iroquoian ceramics from the Mailhot-Curran site, southern Quebec

    E-Print Network [OSTI]

    Optical dating of St. Lawrence Iroquoian ceramics from the Mailhot-Curran site, southern Quebec L) was applied on pottery sherds from the Mailhot-Curran archaeological site (BgFn-2), a Late Woodland period previous dating methods used for Mailhot-Curran (radiocarbon and seriation of the archaeological remains

  15. 734 IEEE TRANSACTIONS ON COMPUTER-AIDED DESIGN OF INTEGRATED CIRCUITS AND SYSTEMS, VOL. 25, NO. 4, APRIL 2006 Short Papers

    E-Print Network [OSTI]

    Hu, Jiang

    that the proposed techniques can lead to an average of 76% antenna-violation reduction and 99% via of oxide, act like antennas that collect charges when exposed directly to the plasma [1]. If the charged conductors are connected only to a gate oxide, a Fowler­Nordheim (F­N) tunneling current will discharge

  16. Elsevier.com -Natural Hazards: Monitoring and Assessment Using Rem... http://www.elsevier.com/wps/find/bookdescription.cws_home/30785/des... 1 of 1 5/10/2006 4:44 AM

    E-Print Network [OSTI]

    Singh, Ramesh P.

    -electromagnetic effects (M. Parrot). Application of remote sensing data in earthquake monitoring (D. Massonnet. Iglsederet al.). Satellite remote sensing data on industrial hazards (J.R. Givri). Application of vegetation index and brightness temperature for drought detection (F.N. Kogan). Monitoring of oil spills using

  17. AI.IALYSIS OF RINGING RECOVERIES OF RUFF INVOLVING SOUTHERN AFRICA

    E-Print Network [OSTI]

    de Villiers, Marienne

    and India to Siberia, east of the Ural Mountains (6o"n). RESULTS ( a) Recoveries. Of the 17 long in Uatarii and Uganda, one in lran, one in Russia and eight in Siberia. fn addition, two foreign-ringed Ruffs NUMBER OF RECOVERIES !iHERE MORE THAN ONE. 76 #12;The birds recovered in Russia and Iran \\dere both

  18. Sandia is a multiprogram laboratory operated by Sandia Corporation, a Lockheed Martin Company, for the United States Department of Energy's National Nuclear Security Administration

    E-Print Network [OSTI]

    Siefert, Chris

    , for the United States Department of Energy's National Nuclear Security Administration under contract DE-AC04-94AL objects. ­ Application provides simple functions to answer queries. ­ Small extra costs in memory_Set_Fn) COMPUTE Move data (Zoltan_Migrate) Clean up (Zoltan_Destroy) APPLICATION Zoltan_LB_Partition: · Call query

  19. Extraction of emission area from FowlerNordheim plots Richard G. Forbes,a)

    E-Print Network [OSTI]

    Deane, Jonathan

    Extraction of emission area from Fowler­Nordheim plots Richard G. Forbes,a) Jonathan H. B. Deane June 2004 The process of deriving emission-area estimates from Fowler­Nordheim FN plots is investigated, using emission-area extraction functions and an iterative procedure suggested earlier R. G. Forbes, J

  20. &Science Service Featws Released upon receipt

    E-Print Network [OSTI]

    available for Only 28 stations. One of these stations is at Washington, D.C. where, on a Ch&= less day fn midsummer, the receipt of radiation amounts to nearly 30 million horse- power hours per square mile horse-power hours. ttThis,lf says Dr. H. H. KimbaJ.1, Ifappears t o be an enormous mount

  1. Computer Engineering Department, "Lucian Blaga" University of Sibiu, Romania http://csac.ulbsibiu.ro/

    E-Print Network [OSTI]

    Vintan, Lucian N.

    : Min/Max y = f(x) = (f1(x), f2(x) ... fn(x)) x = (x1, x2, ..., xm) X - decision vector (no. of coresComputer Engineering Department, "Lucian Blaga" University of Sibiu, Romania http" University of Sibiu (LBUS), Romania Academy of Technical Sciences of Romania #12;22 Computer Engineering

  2. If the behavior of otariids at sea is similar to that exhibited by the entangled sea lion, then drowning

    E-Print Network [OSTI]

    in a larger net. Additionally, because the net was so tightly wrap- ped around the sea lion's neck, necrosis swimming could continue to tighten the net. Although several authors (Scordino and Fisher fn. 1) have, easily iden- tified by the eight dark saddle-like bl

  3. Products and symmetrised powers of irreducible representations of SO \\Lambda

    E-Print Network [OSTI]

    Toumazet, Frédéric

    Products and symmetrised powers of irreducible representations of SO \\Lambda (2n) R C Kingyx F'n, Poland 31 March 1998 Abstract. The calculation of branching rules, tensor products and plethysms products is derived and a complete analysis of the terms in both Hm \\Theta Hm 0 and H \\Theta H is given

  4. *Corresponding author. Fax: #7-3832-33-1080. E-mail address: bykov@thermo.isp.nsc.ru (A.A. Bykov).

    E-Print Network [OSTI]

    Gusev, Guennady

    *, G.M. Gusev , J.R. Leite , N.T. Moshegov , A.K. Bakarov , A.I. Toropov , D.K. Maude , J.C. Portal Novosibirsk, Russia Instituto de Fn&sica da Universidade de SaJ o Paulo, SP, Brazil GHMF, MPI-FKF/CNRS, BP 166

  5. Controlling acid rain

    E-Print Network [OSTI]

    Fay, James A.

    1983-01-01

    High concentrations of sulfuric and nitric acid in raTn fn the northeastern USA are caused by the large scale combustion of fossil fuels within this region. Average precipitation acidity is pH 4.2, but spatial and temporal ...

  6. Khesbn no. 149 - Spring 2007 - Journal

    E-Print Network [OSTI]

    Admin, LAYCC

    2007-01-01

    ryrrf,.t rybrse:XbXu X - 0"l'l nx r1$1l? - Dl'Dl5t6r1 "lltrro'. 'tuuxs yu'rgllpr) nx i:*pi*ulrii:rru>rp lyDll fN .ly:Eyl ? '? ff lltly vtrnrrn nx uDNVJrb orD D'tt Fryn ybr /? t{

  7. Grades of Discrimination: Indiscernibility, Symmetry, and Relativity

    E-Print Network [OSTI]

    Button, Tim

    2015-01-01

    prove that these are genuine definitions, i.e. that c(M,N ) and i(M,N ) are func- tions. I begin with c(M,N ): Lemma 4.5 If pi ? I(M,N ), then pic is a relativeness correspondence, and hence pic ? C(M,N ). Proof Fix n pic fN (e). Hence pic is a...

  8. r:. (/ '7 .' Rgferenee me flo. . /[ 7~ / e /

    E-Print Network [OSTI]

    (GJE IEXJP'JElRHWEN"n §"fFnJl Dq Berkeley, Califo r nia Air-Drying of Robusta Eucalyptus Lumber ABSTRACT: A study of air-drying 4/ 4 Eucalyptus robusta lumber in Hilo, Hawaii showed that during typical summer: SKOLMEN Eucalyptus robusta, a t r e e native to Australia, is an important timber species in Haw a i i

  9. First-row hydrides: Dissociation and ground state energies using quantum Monte Carlo

    E-Print Network [OSTI]

    Anderson, James B.

    First-row hydrides: Dissociation and ground state energies using quantum Monte Carlo Arne Lu, Pennsylvania 16802 Received 20 May 1996; accepted 24 July 1996 Accurate ground state energies comparable FN-DQMC method. The residual energy, the nodal error due to the error in the nodal structure

  10. Gear coupling effects on rotordynamics 

    E-Print Network [OSTI]

    Clark, Robert Warren

    1988-01-01

    The forces on the rotor gear shown in Figure 5, will be equal but opposite those on the spacer. Therefore the forces on a tooth of the rotor located at 8, in spacer reference frame are: sp ace r FN rotor Ey Z. torque Y. Y, f Fig. 5. Forces on one...

  11. Published: March 09, 2011 r 2011 American Chemical Society 4680 dx.doi.org/10.1021/ja110505r |J. Am. Chem. Soc. 2011, 133, 46804683

    E-Print Network [OSTI]

    Goddard III, William A.

    Tkatchouk, William A. Goddard, III, and Paula L. Diaconescu*, Department of Chemistry & Biochemistry to novel transformations. While studyingthe reactivity behavior of group 3 metal alkyl11-15 and uranium unknown as a product of C-H activation in the chemistry of d0 fn metals,27 was observed. In the course

  12. Towards Robust Peer Counting Alberto Montresor

    E-Print Network [OSTI]

    Montresor, Alberto

    peer count in absence of churn. The protocol can handle extreme levels of churn, and automatically churn resilience [2]. Others let each node assume f(n) identities to balance load [3], [4. First, it is eventually accurate, i.e. the estimate converges to the number of nodes in absence of churn

  13. CALCULATION OF SCALED NUCLEATION RATES FOR WATER USING MONTE CARLO GENERATED CLUSTER FREE ENERGY DIFFERENCES

    E-Print Network [OSTI]

    Hale, Barbara N.

    CALCULATION OF SCALED NUCLEATION RATES FOR WATER USING MONTE CARLO GENERATED CLUSTER FREE ENERGYMattio All Rights Reserved #12;iii ABSTRACT Helmholtz free energy differences, -dFn , are calculated inconsistent with the experimental properties of water. Summation of the scaled TIP4P free energy differences

  14. Serologic titers in the bovine with relation to the demonstration of anaplasma organisms under the light microscope and the infectivity of the animals' blood 

    E-Print Network [OSTI]

    Huff, John Wesley

    1962-01-01

    & $f. c hmplsenasie Qbso~~ad fn Speeds?. J. ac, e. ", yet, BA. Assu, , 92, +935)& 529 582. RQ. stkles?c, M, g Qbsecvetione on hneplmeumie in &hho. 3, assz'. yet, ~& assn. , 99, f1932) c. pXP. "N. gl. Stiles, 6, 9, : Ths Spread of knsplcnmesis...

  15. Hydrodynamical Simulations of Molecular Dynamics in Supersonic Turbulent Flow

    E-Print Network [OSTI]

    ) = R (T ; n; f) D (T ; n; f) ; (1d) where n is the hydrogen nuclei density, e is the internal energy analyse PDFs of density for the volume, mass, molec- ular mass and the energy distribution over the range density and f is the molecular hydrogen abundance (i.e. n(H 2 ) = fn). We consider the gas as a mixture

  16. Soliton solutions of the Kadomtsev-Petviashvili II equation Gino Biondinia

    E-Print Network [OSTI]

    Biondini, Gino

    of Mathematics, State University of New York, Buffalo, New York 14260-2900 S. Chakravartyb Department including water waves and plasmas, astrophysics, cosmology, optics, magnetics, anisotropic two, ... , fN are a set of linearly independent solutions of the linear system f y = 2 f x2, f t = 3 f x3 . 1

  17. 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.

  18. 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 ...

  19. 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 ...

  20. 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 ...

  1. 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 ...

  2. 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 ...

  3. 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

  4. 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...

  5. 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

  6. 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 ...

  7. 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 ...

  8. 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

  9. 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 ...

  10. 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

  11. 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

  12. 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...

  13. 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

  14. 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

  15. CGCG 480-022: A distant lonesome merger?

    E-Print Network [OSTI]

    Carretero, C; Gonzalez-Garcia, C; Beckman, J E; Quilis, V

    2006-01-01

    We present a complete analysis, which includes morphology, kinematics, stellar populations and N-body simulations of CGCG 480-022, the most distant (cz=14317 km/s) isolated galaxy studied so far in such detail. The results all support the hypothesis that this galaxy has suffered a major merger event with a companion of ~0.1 times its mass. Morphology reveals the presence of a circumnuclear ring and possibly further ring debris. The radial velocity curve looks symmetrical, whilst the velocity dispersion increases with radius reaching values that do not correspond to a virialized system. Moreover, this galaxy deviates significantly from the Fundamental Plane and the Faber-Jackson relation. The stellar population analysis show that the ring is younger and more metal-rich, which suggest that it has undergone a fairly recent burst of star formation. Both morphological and dynamical results are in broad agreeement with our N-body simulations.

  16. CGCG 480-022: A distant lonesome merger?

    E-Print Network [OSTI]

    C. Carretero; A. Vazdekis; C. Gonzalez-Garcia; J. E. Beckman; V. Quilis; ;

    2006-08-01

    We present a complete analysis, which includes morphology, kinematics, stellar populations and N-body simulations of CGCG 480-022, the most distant (cz=14317 km/s) isolated galaxy studied so far in such detail. The results all support the hypothesis that this galaxy has suffered a major merger event with a companion of ~0.1 times its mass. Morphology reveals the presence of a circumnuclear ring and possibly further ring debris. The radial velocity curve looks symmetrical, whilst the velocity dispersion increases with radius reaching values that do not correspond to a virialized system. Moreover, this galaxy deviates significantly from the Fundamental Plane and the Faber-Jackson relation. The stellar population analysis show that the ring is younger and more metal-rich, which suggest that it has undergone a fairly recent burst of star formation. Both morphological and dynamical results are in broad agreeement with our N-body simulations.

  17. Structures of Adnectin/Protein Complexes Reveal an Expanded Binding Footprint

    SciTech Connect (OSTI)

    Ramamurthy, Vidhyashankar; Krystek, Jr., Stanley R.; Bush, Alexander; Wei, Anzhi; Emanuel, Stuart L.; Gupta, Ruchira Das; Janjua, Ahsen; Cheng, Lin; Murdock, Melissa; Abramczyk, Bozena; Cohen, Daniel; Lin, Zheng; Morin, Paul; Davis, Jonathan H.; Dabritz, Michael; McLaughlin, Douglas C.; Russo, Katie A.; Chao, Ginger; Wright, Martin C.; Jenny, Victoria A.; Engle, Linda J.; Furfine, Eric; Sheriff, Steven

    2014-10-02

    Adnectins are targeted biologics derived from the tenth type III domain of human fibronectin ({sup 10}Fn3), a member of the immunoglobulin superfamily. Target-specific binders are selected from libraries generated by diversifying the three {sup 10}Fn3 loops that are analogous to the complementarity determining regions of antibodies. The crystal structures of two Adnectins were determined, each in complex with its therapeutic target, EGFR or IL-23. Both Adnectins bind different epitopes than those bound by known monoclonal antibodies. Molecular modeling suggests that some of these epitopes might not be accessible to antibodies because of the size and concave shape of the antibody combining site. In addition to interactions from the Adnectin diversified loops, residues from the N terminus and/or the {beta} strands interact with the target proteins in both complexes. Alanine-scanning mutagenesis confirmed the calculated binding energies of these {beta} strand interactions, indicating that these nonloop residues can expand the available binding footprint.

  18. Genetic Evidence for the Phylogenetic Relationship between Na-Dene and Yeniseian Speakers

    E-Print Network [OSTI]

    Rubicz, Rohina; Melvin, Kristin L.; Crawford, Michael H.

    2002-12-01

    *O, MN*M, RH*R1, RH*R2, GM*AG, GM*AXG, KM*]) from three blood group systems and immunoglobulins. The first principal component accounts for 55.8% of the total variation and separates the Na-Dene (AP, DG, HA, and NV) from the Siberian populations (AE, CC..., EK, FN, KT, and 748 / RUBICZ ET AL. 0.3 NG FN '-. 0.2 - C..' 0 0.1 DG a) c HA *L) 0.0 -. ,---- ,---,,,,,---- ,,,,---- ,-- ,,,-,,,,,---,,,,,,,----............ AE NV CC -0.1 -EK * AP A~KT -0.2 -0.1 0.0 0.1 0.2 0.3 0.4 Eigenvector 1 - 55.8% Figure 2...

  19. Centro de Investigacion y de Estudios Avanzados del IPN Departamento de Matematicas

    E-Print Network [OSTI]

    una matriz P tal que PAP-1 es una matriz diagonal. 2. C´alculo 2.1 Probar que la serie n k=1 1 k 1 #12;no converge. 2.2 Sea h una funci´on continua y g una funci´on diferenciable en R . Calcu- lar la que f no es diferenciable en (0, 0) 3. Problemas opcionales 3.1 Si f(x) = x3 - x, probar que f(n) es

  20. Equations for predicting the layer stiffness moduli in pavement systems containing lime-flyash stabilized materials 

    E-Print Network [OSTI]

    Alam, Shah Manzoor

    1984-01-01

    Site 3 located on FN '1604 in Bexar Count This test site consisted of six test sections constructed of a 10- inch flexible base over a 6-inch lime-flyash stabilized subbase. The sections were surfaced with a two- course bituminous surface treatment...EOUATIONS FOR PREDICTING THE LAYER STIFFNESS ' MODULI IN PAVEMENT SYSTEMS CONTAINING LIME-FLYASH STABILIZED MATERIALS A Thesis by SHAH MANZOOR ALAM Submitted to the Graduate College of Texas AN University in partial fulfillment...

  1. Effects of some chemical substances on germination, root development, and growth of the stem cuttings of sugar cane 

    E-Print Network [OSTI]

    Khan, Mohammad Abdullah

    1953-01-01

    ? O ?H o c d W O O I fn -H e O O I CV r l O (d T3 S 0}8 ?H ?H ?P ?H a) TJ a O?H 6 X> a 6o oo CV 1-3 \\ T3 a a ? f-i PL,? . J3 o $ ao ?H aVCtO -P -P...

  2. Embodied rationality

    E-Print Network [OSTI]

    Spellman, Barbara A.; Schnall, Simone

    2009-01-01

    muscles. On some trials participants pulled up the corners of the mouth, in others they pulled the eyebrows down and together. Although they did not realize that they were actually producing smiles or frowns, participants reported feelings consistent... expressions of various emotions report feeling the corresponding emotions. [FN57] In a typ- ical experiment, *139 participants were told that facial muscle activity was being measured by electrodes while they were contorting their faces to contract various...

  3. Buddha in Art: From Symbol to Image

    E-Print Network [OSTI]

    Ganguli, Kalyankumar

    1986-01-01

    Upanishadic"princ.;;iples. Though growing out of Vedic thin kings, the Upanishads had emphasised on the pursuit of wisdom and a right course of action and behaviour but did not promote any idea conducive to image worship. In this perspective it may... by offering of flowers, garlands and incense and also by circumambulating the same. After the Mahaparinirvana, eight stupas containing the sacred relics of Buddha were reported to have been built by king Ajatasatru at different places as stated fn...

  4. Bulletin of Tibetology: Volume 22 Number 3 : Full issue

    E-Print Network [OSTI]

    Namgyal Institute of Tibetology

    1986-11-23

    and rebirth, and had virtually nullified the efficacy of sacrifice. The way of fulfilment as laId down by Gautama after attaining Buddhahood, is found to bear intimate awareness of those Upanishadic"princ.;;iples. Though growing out of Vedic thin kings... and also by circumambulating the same. After the Mahaparinirvana, eight stupas containing the sacred relics of Buddha were reported to have been built by king Ajatasatru at different places as stated fn the Mahaparinibbana Suttanta; Later Asoka...

  5. International trade in grains and cotton: a market share-Markov chain analysis 

    E-Print Network [OSTI]

    Seelig, Leonard Robert

    1980-01-01

    o p ment May 1980 ABSTRACT International Trade in Grains and Cotton: A Market Share - Markov Chain Analysis May 1980 Leonard Robert Seeli g, B . Com . , University of the Wi twatersand, South Africa Chairman of Advisory Committee: Dr. Michael... the relative trade positions of each country fn the market, market shares give some indication of the potential market power of individual trading nations. Markov Chain Analysis was used to project the probability distribution of the export of selected...

  6. Nepali Aawaz Volume 1, Issue 7, 23 December 2005 - 3 January 2006

    E-Print Network [OSTI]

    Shrestha, Kashish Das

    {qmddf clwjQmf lbg]z lqkf7Ln] dfgj clwsf/ s'g} jfb xf]Og, ;j} gful/ssf] st{Jo / clwsf/ xf] eGg'xb} ;Eo ;dfh / ;d'Ggt /fi6« agfpg /fli6«o d"No / dfGotfsf ljsNkx? vf]lhg'kg]{ s'/f atfpg' eof] . pxfFn] hgtfsf] cfjfh /f]s]/ aGb'sn] zflGt sfod x'g g...

  7. Determination of the static polarizability of the 8s2 S1/2 state of atomic cesium

    E-Print Network [OSTI]

    Safronova, Marianna

    Determination of the static polarizability of the 8s2 S1/2 state of atomic cesium Mevan Gunawardena of the static polarizability of the 8s2 S1/2 state of atomic cesium, carried out jointly through experimental number s : 32.10.Dk, 32.60. i, 32.10.Fn I. INTRODUCTION Atomic cesium has played a central role in a wide

  8. Physics 112 Mathematical Notes Winter 2000 1. Power Series Expansion of the Fermi-Dirac Integral

    E-Print Network [OSTI]

    California at Santa Cruz, University of

    Physics 112 Mathematical Notes Winter 2000 1. Power Series Expansion of the Fermi-Dirac Integral The Fermi-Dirac integral is defined as: fn(z) 1 (n) 0 xn-1 dx z-1ex + 1 , where x /kT and z eµ/kT . We (ze-x )m = z (n) m=0 (-1)m zm 0 e-(m+1)x xn-1 dx . Using the well known integral: 0 e-Ax xn-1 dx

  9. A determination of the acceptability of the liquid media sampler as an alternative to the standard midget impinger 

    E-Print Network [OSTI]

    Ruser, Bernard Henry

    1983-01-01

    Micrograms of Ammonia in Standard 26 INTRODUCTION Over the past several decades many changes have come about fn air sampling techniques and equipment. These changes are due primarily to advancement in technology. This advancement has been perpetuated... comparison of the mean collection efficiencies of the LMS and the standard midget impinger over their respective recommended flow rate ranges. ' The two (2,1T) questions addressed relative to collection efficiency were: 1) does the LNS show significant...

  10. Understanding the Structural Basis for Functional Differences in Staphylococcal MSCRAMMS SDRE1 and BBP/SDRE2 and Their Role in Species Tropism 

    E-Print Network [OSTI]

    Francis, Mathew Prashanth

    2015-04-29

    DAP-R: Daptomycin Resistant DNA: Deoxyribonucleic Acid ECM: Extracellular Matrix ELISA: Enzyme-Linked Immunosorbent Assay Fg: Fibrinogen fH : Factor H vii Fn: Fibronectin FnbpA: Fibronectin-binding Protein A FnbpB: Fibronectin... Figure 4-10. Cow Fibrinogen Peptide Inhibition. ................................................. 77 Figure 4-11. Animal Fibrinogen Peptide Inhibition. ............................................. 78 Figure 5-1. Apo-SdrE2-N2N3 and SdrE2-N2N3-Fg Peptide...

  11. Released upon receipt but intended f o r use

    E-Print Network [OSTI]

    them are several patterns. that measure the energy radiated by sun and slry t w e t h e r are various ways of measuring the t o t a l amount of energy in the ambeams and E t i l l other6 of measuring the distribution Of energy through the d.if- ferent parts of the solar spectrum. fn heat units called "calories

  12. 1) Probar que en el anlisis promedio del algoritmo de ordenamiento por insercin, la probabilidad de que en la iteracin i, el elemento en la posicin i le corresponda la posicin k (k entre 1 e i) es 1/i.

    E-Print Network [OSTI]

    Meza, Oscar J.

    Tarea 1 1) Probar que en el análisis promedio del algoritmo de ordenamiento por inserción, la.O(g) si f no se anula para n n0 4) Análisis del caso promedio del algoritmo de ordenamiento por selección si f(n) = O(nk ) entonces f es b-uniforme? 8) El tiempo de corrida en peor caso de un algoritmo

  13. Bull. Polish Acad. Sci. Math. 37 (1989), 351353 ON SOME FUNCTIONALS ON BERGMAN SPACES

    E-Print Network [OSTI]

    Chojnacki, Wojtek

    1989-01-01

    , then the functionals f f(k)(w) (w , k N {0}) on the Bergman space of are nonzero and linearly independent. Let square integrable functions on . Suppose that L2 H() = {0}. For each w and each n N {0}, let (n) w denote the linear continuous functional on L2 H() defined by (n) w (f) = f(n) (w) f L2 H() . M. Skwarczy

  14. Generalized bounds for reconstruction of words

    E-Print Network [OSTI]

    Sziklai, Péter

    word w Fn t . Definition 1 Let sk(w) = {u Fk t : u w}, the multiset of all of the n k subwords of w problem: for a given word w of length n, what is the smallest k, such that we can reconstruct w from of these problems. It is relatively easy to prove (see [2] for instance), that s n-1(w) is enough for the reconstruc

  15. Com S 631: Lower bounds and Separation Results Lecture 1 Scribe: Pavan Aduri

    E-Print Network [OSTI]

    Aduri, Pavan

    the following machine N. (1) Input w, |w| = n. (2) If w is not of the form x, 0i , then reject. (3) Run U(x, w(| x, 0i |). Let | y, 0i | = n. Consider the behavior of N on w = y, 0i . In Step 3, it runs U(y, w) steps. Since Cyf(n) log f(n) n), the U completes the simulation. If My accepts w, then N rejects w

  16. On irrationality and transcendency of infinite sums of rational numbers

    E-Print Network [OSTI]

    Tijdeman, Robert

    On irrationality and transcendency of infinite sums of rational numbers R. Tijdeman Abstract the irrationality and transcendency of sums n=1 nf(n) where Q, f(x) Q(x) such that f(n) is defined for all(n) where P(x), Q(x) Z[x]. We give conditions under which such a sum is irrational and under which

  17. AN EFFICIENT SECOND ORDER IN TIME SCHEME FOR APPROXIMATING LONG TIME STATISTICAL PROPERTIES OF

    E-Print Network [OSTI]

    AN EFFICIENT SECOND ORDER IN TIME SCHEME FOR APPROXIMATING LONG TIME STATISTICAL PROPERTIES of the following efficient second order in time scheme for the 2D Navier-Stokes equation in a periodic box: 3n+1 - 4n + n-1 2k + (2n - n-1 ) · (2n - n-1 ) - n+1 = fn+1 , -n = n . The scheme is a combination of a 2

  18. A study of oil displacement by carbonated water 

    E-Print Network [OSTI]

    Partovi-Najafabadi, Roohollah

    1968-01-01

    A STUDY OF OIL DISPLACEMENT BY CARBONATED WATER A Thesis by Roohollah Partovi-N. Submitted to the Graduate College of the Texas A&M University in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE January 1988... Major Subject: Petroleum Fn ineerin A STUDY OF OIL DISPLACEMENT BY CARBONATED WATER A Thesis by Roohollah Partovi-N. Approved as to style and content by: ( irman of mmittee) M mber) (Head of partment) (Member) January 1968 CP9292...

  19. Search for WZ resonances in the fully leptonic channel using pp collisions at ?s = 8 TeV with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for resonant WZ production in the ???[superscript ?]?[superscript ?] (?,?[superscript ?] =e,?) decay channel using 20.3 fb[superscript ?1] of ?s = 8 TeV collision data collected by the ATLAS experiment at LHC is ...

  20. Simultaneous measurements of the t[bar over t], W[superscript +]W[superscript -], and Z/ ?[superscript *] ? ?? production cross-sections in pp collisions at ?s = 7 TeV with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    Simultaneous measurements of the t[bar over t], W[superscript +]W[superscript ?], and Z/?[superscript ?] ? ?? production cross-sections using an integrated luminosity of 4.6??fb[superscript ?1] of pp collisions at ?s = ...

  1. Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for the Standard Model Higgs boson in proton–proton collisions with the ATLAS detector at the LHC is presented. The datasets used correspond to integrated luminosities of approximately 4.8 fb[superscript ?1] ...

  2. Volatilizable Biogenic Organic Compounds (VBOCs) with two dimensional Gas Chromatography-Time of Flight Mass Spectrometry (GC × GC-TOFMS): sampling methods, VBOC complexity, and chromatographic retention data

    E-Print Network [OSTI]

    2012-01-01

    4 isoprene toluene- d 8 OxMT FB BFB ST MT t 1 (s) ? primarycedrene camphor linalool BFB t 1 (s) ? primary retentiontoluene-d8, bromofluorobenzene (BFB), and 1,2-DCB-d4 (1,2-

  3. 1 Introduction CPU speed has doubled roughly every 18 months, while

    E-Print Network [OSTI]

    Jacob, Bruce

    [9]. Each type of DRAM i.e., SDRAM, DDR SDRAM etc., has different behaviors and architectures, including SDRAM, DDR, DDR2, DRDRAM and FB-DIMM,with the capability to easily vary their parameters. It also

  4. IECM OverviewIECM Overview Edward S. Rubin

    E-Print Network [OSTI]

    · Mechanical treatment Boiler/Turbine Types · Subcritical · Supercritical · Ultra-supercritical Furnace Firing-Stretford Unit Gas Turbine - GE 7FA - GE 7FB Heat Recovery Steam Generator Steam Turbine Boiler Feedwater System

  5. Observation of New Charmless Decays of Bottom Hadrons

    E-Print Network [OSTI]

    Xie, Si

    We search for new charmless decays of neutral b hadrons to pairs of charged hadrons, using 1??fb[superscript -1] of data collected by the CDF II detector at the Fermilab Tevatron. We report the first observation of the ...

  6. Search for the Standard Model Higgs Boson Produced in Association with Top Quarks Using the Full CDF Data Set

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    A search is presented for the standard model Higgs boson produced in association with top quarks using the full Run II proton-antiproton collision data set, corresponding to 9.45??fb[superscript -1], collected by the ...

  7. Search for neutral Higgs bosons in events with multiple bottom quarks at the Tevatron

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    The combination of searches performed by the CDF and D0 collaborations at the Fermilab Tevatron Collider for neutral Higgs bosons produced in association with b quarks is reported. The data, corresponding to 2.6??fb[superscript ...

  8. Search for B[subscript s][superscript 0]??[superscript +]?[superscript -] and B[superscript 0]??[superscript +]?[superscript -] Decays with CDF II

    E-Print Network [OSTI]

    Bauer, Gerry P.

    A search has been performed for B[subscript s][superscript 0]??[superscript +]?[superscript -] and B[superscript 0]??[superscript +]?[superscript -] decays using 7??fb[superscript -1] of integrated luminosity collected by ...

  9. Measurements of the Top-Quark Mass and the tt? Cross Section in the Hadronic ?+jets Decay Channel at ?s=1.96??TeV

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We present the first direct measurement of the top-quark mass using tt? events decaying in the hadronic ?+jets decay channel. Using data corresponding to an integrated luminosity of 2.2??fb[superscript -1] collected by the ...

  10. Search for New Dielectron Resonances and Randall-Sundrum Gravitons at the Collider Detector at Fermilab

    E-Print Network [OSTI]

    Bauer, Gerry P.

    A search for new dielectron-mass resonances using data recorded by the CDF II detector and corresponding to an integrated luminosity of 5.7??fb[superscript -1] is presented. No significant excess over the expected standard ...

  11. Search for the rare radiative decay W??? in pp? collisions at ?s=1.96??TeV

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We present a search for the rare radiative decay W[superscript ±]??[superscript ±]? using data corresponding to an integrated luminosity of 4.3??fb[superscript -1] of proton-antiproton collisions at a center-of-mass energy ...

  12. Search for the Standard Model Higgs Boson Decaying to a bb? Pair in Events with Two Oppositely Charged Leptons Using the Full CDF Data Set

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We present a search for the standard model Higgs boson produced in association with a Z boson in data collected with the CDF II detector at the Tevatron, corresponding to an integrated luminosity of 9.45??fb[superscript ...

  13. Search for a Higgs boson in the diphoton final state using the full CDF data set from pp? collisions at ?s = 1.96 TeV

    E-Print Network [OSTI]

    CDF Collaboration

    A search for a narrow Higgs boson resonance in the diphoton mass spectrum is presented based on data corresponding to 10 fb[superscript ?1] of integrated luminosity collected by the CDF experiment from proton–antiproton ...

  14. 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

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    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[superscript ...

  15. Search for the Higgs boson in the all-hadronic final state using the CDF II detector

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We report on a search for the production of the Higgs boson decaying to two bottom quarks accompanied by two additional quarks. The data sample used corresponds to an integrated luminosity of approximately 4??fb[superscript ...

  16. dosplus.mac

    E-Print Network [OSTI]

    H describes row, L describes column. dcio: mov c,e; Possible output char. inr e jrz dcio5; 0ffh, do input inr e jrz dcio4; 0feh, get status lda flags ani fb.comp; ...

  17. Searches for new physics using the t[bar over t] invariant mass distribution in pp collisions at ?s = 8??TeV

    E-Print Network [OSTI]

    Apyan, Aram

    Searches for anomalous top quark-antiquark production are presented, based on pp collisions at s? = 8??TeV. The data, corresponding to an integrated luminosity of 19.7??fb[superscript ?1], were collected with the CMS ...

  18. Search for Dark Matter and Large Extra Dimensions in pp Collisions Yielding a Photon and Missing Transverse Energy

    E-Print Network [OSTI]

    Bauer, Gerry P.

    Results are presented from a search for new physics in the final state containing a photon (?) and missing transverse energy (E?T). The data correspond to an integrated luminosity of 5.0??fb-1 collected in pp collisions ...

  19. Interpretation of searches for supersymmetry with simplified models

    E-Print Network [OSTI]

    Apyan, Aram

    The results of searches for supersymmetry by the CMS experiment are interpreted in the framework of simplified models. The results are based on data corresponding to an integrated luminosity of 4.73 to 4.98??fb[superscript ...

  20. Top quark physics expectations at the LHC

    E-Print Network [OSTI]

    Gaponenko, Andrei; ATLAS Collaboration; CMS Collaboration

    2008-01-01

    Physics Analysis Summary TOP 08 005. ATLAS Collaboration,Note 2006/013. E. W. Varnes, Top Physics plenary talk, thismass in the ATLAS cuts based top mass analysis with 1fb ?1

  1. Observation of Spin Correlation in tt? Events from pp Collisions at ?s=7??TeV Using the ATLAS Detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A measurement of spin correlation in tt? production is reported using data collected with the ATLAS detector at the LHC, corresponding to an integrated luminosity of 2.1??fb[superscript -1]. Candidate events are selected ...

  2. Search for TeV-scale gravity signatures in final states with leptons and jets with the ATLAS detector at ?s = 7 TeV

    E-Print Network [OSTI]

    Taylor, Frank E.

    The production of events with multiple high transverse momentum particles including charged leptons and jets is measured, using 1.04 fb[superscript ?1] of proton–proton collision data recorded by the ATLAS detector during ...

  3. Search for Gluinos in Events with Two Same-Sign Leptons, Jets, and Missing Transverse Momentum with the ATLAS Detector in pp Collisions at ?s=7??TeV

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search is presented for gluinos decaying via the supersymmetric partner of the top quark using events with two same-sign leptons, jets, and missing transverse momentum. The analysis is performed with 2.05??fb-1 of ...

  4. Search for anomalous production of prompt like-sign muon pairs and constraints on physics beyond the standard model with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    An inclusive search for anomalous production of two prompt, isolated muons with the same electric charge is presented. The search is performed in a data sample corresponding to 1.6??fb[superscript -1] of integrated luminosity ...

  5. Search for WH production with a light Higgs boson decaying to prompt electron-jets in proton–proton collisions at ?s=7 TeV with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search is performed for WH production with a light Higgs boson decaying to hidden-sector particles resulting in clusters of collimated electrons, known as electron-jets. The search is performed with 2.04 fb[superscript ...

  6. Characterizing the regulatory mechanisms in fusarium verticillioides secondary metabolism using functional genomics approaches 

    E-Print Network [OSTI]

    Choi, Yoon E

    2009-05-15

    the complex secondary metabolism regulations in F. verticillioides. First, using the reverse genetics approach, I characterized a putative protein phosphatase gene, CPP1 as a negative regulator of FB1 biosynthesis. CPP1 gene deletion also affected multiple...

  7. Search for Supersymmetry in Events with Four or More Leptons in ?s = 8 TeV pp Collisions with the ATLAS Detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    Results from a search for supersymmetry in events with four or more leptons including electrons, muons and taus are presented. The analysis uses a data sample corresponding to 20.3??fb[superscript ?1] of proton-proton ...

  8. VIA HAND DELIVERY Mr. John A. Anderson Office of Fossil Energy

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

    No. IH 2f::B- LNG Application for Long-Term Authorization to Expmt Liquefied Natural Gas Dear Mr. Anderson: American LNG Marketing LLC ("American LNG") seeks long-term,...

  9. The effects of moisture and particle size of feedlot biomass on co-firing burner performance 

    E-Print Network [OSTI]

    Chen, Chen-Jung

    2001-01-01

    based fuels. For coal fired power plants located around feedlots where cattle are raised, the renewable biomass is the cattle manure, called feedlot biomass (FB). Thus coal could be mixed with feedlot biomass and then fired in existing boiler burners...

  10. Acceptable Knowledge Summary Report for Mixed TRU Waste Streams: SR-W026-221F-HET-A through D

    SciTech Connect (OSTI)

    Lunsford, G.F.

    2001-10-02

    This document, along with referenced supporting documents provides a defensible and auditable record of acceptable knowledge for the heterogeneous debris mixed transuranic waste streams generated in the FB-Line after January 25, 1990 and before March 20, 1997.

  11. Discovering colorons at the early stage LHC

    SciTech Connect (OSTI)

    Dicus, Duane A. [Center for Particles and Fields and Texas Cosmology Center, University of Texas, Austin, Texas 78712 (United States); Kao, Chung; Sayre, Joshua [Homer L. Dodge Department of Physics and Astronomy and Oklahoma Center for High Energy Physics, University of Oklahoma, Norman, Oklahoma 73019 (United States); Nandi, S. [Department of Physics and Oklahoma Center for High Energy Physics, Oklahoma State University, Stillwater, Oklahoma 74078 (United States)

    2011-05-01

    Prospects are investigated for the discovery of massive hypergluons using data from the early runs of the Large Hadron Collider. A center of mass energy of 7 TeV and an integrated luminosity of 1 fb{sup -1} or 5 fb{sup -1} are assumed. A phenomenological Lagrangian is adopted to evaluate the cross section of a pair of colored vector bosons (colorons, {rho}-tilde) decaying into four colored scalar resonances (hyperpions, {pi}-tilde), which then decay into eight gluons. The dominant eight-jet background from the production of 8g, 7g1q, 6g2q, and 5g3q is included. We find an abundance of signal events and that realistic cuts reduce the background enough to establish a 5{sigma} signal for the coloron mass of up to 733 GeV with 1 fb{sup -1} or 833 GeV with 5 fb{sup -1}.

  12. First observation and amplitude analysis of the B[superscript -] ? D[superscript +]K[superscript -]?[superscript -] decay

    E-Print Network [OSTI]

    Aaij, R.

    The B[superscript -] ? D[superscript +]K[superscript -]?[superscript -] decay is observed in a data sample corresponding to 3.0??fb^{-1} of pp collision data recorded by the LHCb experiment during 2011 and 2012. Its branching ...

  13. Amplitude analysis of B[superscript 0] ? [bar over D][superscript 0]K[superscript +]?[superscript -] decays

    E-Print Network [OSTI]

    Aaij, R.

    The Dalitz plot distribution of B[superscript 0] ? [bar over D][superscript 0]K[superscript +]?[superscript -] decays is studied using a data sample corresponding to 3.0??fb[superscript -1] of pp collision data recorded ...

  14. Observation of the B[0 over s] ? n[superscript ']n[superscript '] Decay

    E-Print Network [OSTI]

    Aaij, R.

    The first observation of the B[s over 0] ? ?[superscript ?]?[superscript ?] decay is reported. The study is based on a sample of proton-proton collisions corresponding to 3.0??fb[superscript -1] of integrated luminosity ...

  15. Human Exposure to Foodborne Toxins in Ghana: Intervention Strategy for Reduction of Aflatoxin and Fumonisin Bioavailability 

    E-Print Network [OSTI]

    Mitchell, Nicole Jean

    2013-08-30

    ......................................................................................18 1.1.8 Human exposure in Africa .............................................................................21 1.1.9 AFB1 metabolism ...........................................................................................25... of exposure .................................................................................48 1.2.7 Regulation ......................................................................................................49 1.3 AFB1/FB1 co...

  16. 894 Volume 55, Number 7, 2001 APPLIED SPECTROSCOPY0003-7028 / 01 / 5507-0894$2.00 / 0 q 2001 Society for Applied Spectroscopy

    E-Print Network [OSTI]

    Hastings, Gary

    that has been stripped of the iron sulfur clusters FA and FB; RC, reaction center; RT, room temperature; S. INTRODUCTION The primary solar capture and conversion processes in oxygen-evolving organisms (OEOs) occur

  17. Measurement of the differential and double-differential Drell-Yan cross sections in proton-proton collisions at ?s = 7 TeV

    E-Print Network [OSTI]

    Apyan, Aram

    Measurements of the differential and double-differential Drell-Yan cross sections are presented using an integrated luminosity of 4.5 (4.8) fb[superscript ?1] in the dimuon (dielectron) channel of proton-proton collision ...

  18. EIS-0219: F-Canyon Plutonium Solutions

    Broader source: Energy.gov [DOE]

    This EIS evaluates the potential environmental impacts of processing the plutonium solutions to metal form using the F-Canyon and FB-Line facilities at the Savannah River Site.

  19. Study of top quark production and decays involving a tau lepton at CDF and limits on a charged Higgs boson contribution

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We present an analysis of top-antitop quark production and decay into a tau lepton, tau neutrino, and bottom quark using data from 9??fb[superscript ?1] of integrated luminosity at the Collider Detector at Fermilab. Dilepton ...

  20. Studies of jet mass in dijet and W/Z + jet events

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Benelli, Gabriele; Kenny, R. P. III; Murray, Michael J.; Noonan, Danny; Sanders, Stephen J.; Stringer, Robert W.; Tinti, Gemma; Wood, Jeffrey Scott; Chatrchyan, S.; Khachatryan, V.; Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Aguilo, E.; Bergauer, T.

    2013-05-17

    Invariant mass spectra for jets reconstructed using the anti-k T and CambridgeAachen algorithms are studied for different jet “grooming” techniques in data corresponding to an integrated luminosity of 5 fb(?1), recorded with the CMS detector...

  1. Application of the Software as a Service Model to the Control of Complex Building Systems

    E-Print Network [OSTI]

    Stadler, Michael

    2012-01-01

    battery, FB: Zinc Bromine flow battery, FC: fuel cell withGeneric heat storage Zinc-bromine flow battery energyZinc-bromine flow battery power Photovoltaics Solar thermal

  2. Flat band potential measurements of naked and viologen-modified n-WS[sub 2] electrodes in aqueous iodide and triiodide solutions

    SciTech Connect (OSTI)

    Huang, J.; Wrighton, M.S. )

    1994-09-15

    The flat band potentials, E[sub FB], of naked n-WS[sub 2] electrodes and cationic viologen polymer-modified n-WS[sub 2] electrodes have been determined in KI and KI[sub 3] solutions by differential capacitance measurements. The E[sub FB] values for naked n-WS[sub 2] electrodes are shifted negatively in electrolyte media containing I[sup [minus

  3. CDF/PUB/TOP/PUBLIC/10793 Measurement of Single Top Quark Production

    E-Print Network [OSTI]

    Quigg, Chris

    CDF/PUB/TOP/PUBLIC/10793 Measurement of Single Top Quark Production in 7.5 fb-1 of CDF Data Using a measurement of single top quark production in lepton plus jets final state using 7.5 fb-1 of p¯p collision. We measure a cross section of 3.04+0.57 -0.53pb (stat+syst) and set a lower limit |Vtb| > 0

  4. CDF/PUB/TOP/PUBLIC/10793 Measurement of Single Top Quark Production

    E-Print Network [OSTI]

    Quigg, Chris

    CDF/PUB/TOP/PUBLIC/10793 Measurement of Single Top Quark Production in 7.5 fb-1 of CDF Data Using a measurement of single top quark production in lepton plus jets final state using 7.5 fb-1 of p¯p collision. We measure a cross section of 3.04+0.57 -0.53pb (stat. + syst.) and set a lower limit |Vtb| > 0

  5. Measurements of fiducial cross-sections for $t\\bar{t}$ production with one or two additional $b$-jets in $pp$ collisions at $\\sqrt{s}$=8 TeV using the ATLAS detector

    E-Print Network [OSTI]

    ,; ATLAS Collaboration

    2015-01-01

    Fiducial cross-sections for $t\\bar{t}$ production with one or two additional $b$-jets are reported, using an integrated luminosity of 20.3 fb$^{-1}$ of proton--proton collisions at a centre-of-mass energy of 8 TeV at the Large Hadron Collider, collected with the ATLAS detector. The cross-section times branching ratio for $t\\bar{t}$ events with at least one additional $b$-jet is measured to be 950 $\\pm$ 70 (stat.) $^{+240}_{-190}$ (syst.) fb in the lepton-plus-jets channel and 50 $\\pm$ 10 (stat.) $^{+15}_{-10}$ (syst.) fb in the $e \\mu$ channel. The cross-section times branching ratio for events with at least two additional $b$-jets is measured to be 19.3 $\\pm$ 3.5 (stat.) $\\pm$ 5.7 (syst.) fb in the dilepton channel ($e \\mu$,\\,$\\mu\\mu$, and \\,$ee$) using a method based on tight selection criteria, and 13.5 $\\pm$ 3.3 (stat.) $\\pm$ 3.6 (syst.) fb using a looser selection that allows the background normalisation to be extracted from data. The latter method also measures a value of 1.30 $\\pm$ 0.33 (stat.) $\\pm$...

  6. Flat band variation of n-cadmium chalcogenides in aqueous cyanide

    SciTech Connect (OSTI)

    Licht, S.; Peramunage, D. [Clark Univ., Worcester, MA (United States)] [Clark Univ., Worcester, MA (United States)

    1996-05-23

    Flatband potential, V{sub fb}, measurements of n-CdSe in alkaline ferrocyanide electrolytes substantiate trends observed for photoelectrochemical open circuit voltage, V{sub oc}, with dissolved cyanide. Similar trends comprising a negative shift of V{sub fb} and an increase in V{sub oc} with increasing concentration of cyanide are also observed for an n-CdTe alkaline ferrocyanide photoelectrochemical cell, PEC. Modification of an alkaline ferro/ferricyanide electrolyte with KCN, in an n-CdSe or n-CdTe PEC, stabilizes the photocurrent, and increases the V{sub oc} by several hundred milivolts. In an approach to the high cyanide concentration limit, V{sub fb} for both n-CdSe and n-CdTe in alkaline ferrocyanide appraches a single limiting value of -1.2 V vs ferro/ferricyanide. 32 refs., 6 figs., 2 tabs.

  7. Top Quark Properties at the TeVatron

    E-Print Network [OSTI]

    Yvonne Peters for the CDF; D0 Collaborations

    2011-03-29

    Discovered in 1995 by CDF and D0 at the Fermilab Tevatron collider, the top quark remains interesting to test the Standard Model. Having collected more than 7 fb$^{-1}$ of integrated luminosity with both experiments until today, several top quark properties have been measured with increasing precision, while other properties have been investigated for the first time. In this article recent measurements of top quark properties from CDF and D0 are presented, using between 1 fb$^{-1}$ and 4.8 fb$^{-1}$ of data. In particular, the measurement of the top quark mass, the top quark width, the top antitop mass difference, a check of the electric charge of the top quark, measurements of the top antitop quark spin correlation and W helicity as well as a search for charged Higgs bosons are discussed.

  8. Search for anomalous production of prompt like-sign lepton pairs at $ \\sqrt{s}=7\\;\\mathrm{TeV} $ with the ATLAS detector

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

    Aad, G.

    2012-12-03

    An inclusive search for anomalous production of two prompt, isolated leptons with the same electric charge is presented. The search is performed in a data sample corresponding to 4.7 fb-1 of integrated luminosity collected in 2011 at ?s = 7 TeV with the ATLAS detector at the LHC. Pairs of leptons (e± e±, e± ?±, and ?± ?±) with large transverse momentum are selected, and the dilepton invariant mass distribution is examined for any deviation from the Standard Model expectation. No excess is found, and upper limits on the production cross section of like-sign lepton pairs from physics processes beyondmore »the Standard Model are placed as a function of the dilepton invariant mass within a fiducial region close to the experimental selection criteria. The 95% confidence level upper limits on the cross section of anomalous e± e±, e± ?±, or ?± ?± production range between 1.7 fb and 64 fb depending on the dilepton mass and flavour combination.« less

  9. Measurements of the total cross sections for Higgs boson production combining the $H \\to \\gamma \\gamma$ and $H \\to ZZ^* \\to 4\\ell$ decay channels at 7, 8 and 13 TeV center-of-mass energies with the ATLAS detector

    E-Print Network [OSTI]

    The ATLAS collaboration

    2015-01-01

    Measurements of total cross sections are presented for Higgs boson production in proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider. The data correspond to 4.5 fb$^{-1}$ collected at the center-of-mass energy of 7 TeV, 20.3 fb$^{-1}$ at 8 TeV, and most recently 3.2 fb$^{-1}$ at 13 TeV. Cross sections are obtained from measured $H \\to \\gamma\\gamma$ and $H \\to ZZ^{*} \\to 4\\ell$ event yields, which are combined accounting for detector effects, fiducial acceptances and branching fractions. The total Higgs boson production cross sections are measured to be $34^{+11}_{-10}$ pb, $33.3^{+5.8}_{-5.5}$ pb, and $24^{+21}_{-18}$ pb for center-of-mass energies of 7, 8 and 13 TeV, respectively. These measurements are compared to state-of-the-art Standard Model theoretical predictions.

  10. Technological advances in the University of Washington accelerator mass spectrometry system

    SciTech Connect (OSTI)

    Farwell, G.W.; Grootes, P.M.; Leach, D.D.; Schmidt, F.H.

    1983-01-01

    During the past year we have continued to work toward greater stability and flexibility in nearly all elements of our accelerator mass spectrometry (AMS) system, which is based upon an FN tandem Van de Graaff accelerator, and have carried out measurements of /sup 14/C//sup 12/C and /sup 10/Be//sup 9/Be isotopic abundance ratios in natural samples. The principal recent developments and improvements in the accelerator system and in our sample preparation techniques for carbon beryllium are discussed, and the results of a study of /sup 10/Be cross-contamination of beryllium samples in the sputter ion source are presented.

  11. Accelerator mass spectrometry facility at the University of Washington: current status, and an application to the /sup 14/C profile of a tree ring

    SciTech Connect (OSTI)

    Farwell, G.W.; Grootes, P.M.; Leach, D.D.; Schmidt, F.H.

    1984-01-01

    The University of Washington Model FN Tandem accelerator (1) is used for Accelerator Mass Spectrometry (AMS) of /sup 10/Be and /sup 14/C. This paper describes our basic system, our methods for rare-isotope normalization, final ion detection, and sample preparation, and the general problem of adapting an existing accelerator to meet the stringent stability requirements of precision AMS measurements while retaining human and technical compatibility with other users and uses of the accelerator. Recent preliminary data obtained on /sup 14/C in thin sequential sections of a single Sitka spruce tree ring (1963) are presented.

  12. Compleximetric determination of sulfate with ethylenediaminetetraacetic acid 

    E-Print Network [OSTI]

    Spurlock, William W

    1961-01-01

    tftrstfoay causing fn esse cones the persfeteaoe of original colors well beyoad the point oy stofohfoaotry, sad 1a other oeoes es fndeffnite color reactions The lftersture sites various buffer solutioas an4 sony 1a4fes toro tor the tftratfoa of aetsl foas... would produce fascoureey ia detersfastfoa of other aetal foes ff sagaesiua foa be ?sed ia preperfag s buffer solutiosa This observstioa suggests the pos ?fbilfty of usfag tho neutral saLt oE aegaesfua, slreo4y roasted with QCk~ (Ngi&iygk) ae...

  13. O. Forster: Die Riemannsche Zetafunktion 3. Euler-Mascheronische Konstante

    E-Print Network [OSTI]

    Forster, Otto

    6x a n f(n) mit a n = 1 und f(x) = 1=x an und erhalten X n6x 1 n = bxc x + Z x 1 btc t 2 dt = 1 x bxc x + Z x 1 dt t Z x 1 t btc t 2 dt = log x + #16; 1 Z 1 1 t btc t 2 dt #17; x bxc x + Z 1 x t btc t 2 dt = log x + +O #16; 1 x #17; mit = 1 Z 1 1 t btc t 2 dt: 3.2. Satz. Mit der Euler

  14. The Power of Space: The Acropolis, the Theatre of Dionysos, and Tragedy in the 5th Century BCE

    E-Print Network [OSTI]

    Bondari, Katrina

    2011-05-19

    ssssc?s?wct??c? HE POWRFWSAC:FLIW,D::N:IWAC:WSNDEYEGRLWLARGGWLRALWP5EU:WAC:WNRAOIWRALWDBRFLW PDARLARNPGGOWGRAWPAWFRoCAWAEWpBGGOW RLYGPOWRALWyOLA:DOWPF WyPoFRpRN:FN:WriGPA:WTghWSFOEF:W tPG2RFoWACDEBoCWAC:WSNDEYEGRLWNEyYG:0W BDRFoWAC:W POWNPFWp...::GWAC:WLAD:FoACWPF W YEt:DWEpWAC:WPFNR:FAWLENR:AOWACPAWNEFLADBNA: WLBNCWoGEDREBLWyEFBy:FALhW1EE2RFo FEDACWpDEyWAC:WYD:NRYRN:WEpWAC:WSNDEYEGRLWEF:WCPLWPWUR:tWEpWAC:WPFNR:FAWKEyPFWpEDByW PF W,D::2Wpolip IWPLWt:GGWPLWAC:WAEBDRLAOWD:LAPBDPFALIWNPp:LIWPF WLEBU...

  15. An experiment to detect gravity at sub-mm scale with high-Q mechanical oscillators

    E-Print Network [OSTI]

    L. Haiberger; M. Weingran; H. Wenz; S. Schiller

    2005-10-20

    Silicon double paddle oscillators are well suited for the detection of weak forces because of their high Q factor (about 10^5 at room temperature). We describe an experiment aimed at the detection of gravitational forces between masses at sub-mm distance using such an oscillator. Gravitational excitation is produced by a rotating aluminium disk with platinum segments. The force sensitivity of this apparatus is about 10 fN at room temperature for 1000 s averaging time at room temperature. The current limitations to detection of the gravitational force are mentioned.

  16. Recursion relations for the matrix elements of the two-dimensional harmonic oscillator 

    E-Print Network [OSTI]

    Ferester, Avner Herman

    1970-01-01

    and degree k are given expl1citly (&+~~. '(- ~) (&+R)/ (k-n)/fn+Z)/ n/ $/ J/ p/ L (y= ~~ . + . +~~is. n-0 Two generating functions for the LJ (2) are (10) ~p~ ?, Q t) -Q / (@ 4=o . F, (~ f-, . ~) The ~gQ satisfy the recursion formula ~ i, ~~y= (z... and the Lorentzian (c+z) will also be derived. The recursion relations will be obtained from the generating functions for 0he matrix elements. THE TWO-DIMERSIOVAL RARMO'. JIC OSCILLATOR AVD ITS WAVE- FUWCTIONS A particle of mass m, at the end of . a spr1ng fixed...

  17. ERROR IN LINEAR INTERPOLATION Let P1(x) denote the linear polynomial interpolating

    E-Print Network [OSTI]

    Atkinson, Kendall

    (x) - P1(x) = (x - x0) (x - x1) 2 f00(cx) for some cx between the minimum and maximum of x0, x1, and x cx x1 #12;(x - x0) (x1 - x) 0, x0 cx x1 and therefore (x - x0) (x1 - x) " log10 e 2x2 1 # log10]. Then f(x)-Pn(x) = (x - x0) (x - x1) · · · (x - xn) (n + 1)! f(n+1) (cx) with cx some point between

  18. Academic Achievement of K-12 Students With Emotional and Behavioral Disorders

    E-Print Network [OSTI]

    Nelson, J. Ron; Benner, Gregory J.; Lane, Kathleen Lynne; Smith, Benjamin W.

    2004-01-01

    to be relatively representative in terms of severity of problem behaviors of the pop- 6 2 Fall 2004 at i I I I so "T oo CN ^ O SO ^ M oo 1/N rs rn • ^ 00 fN bo ys ) - l/N 00 oO ;^ so 3 bo ys ; 2 gir ls) ON ON CN SO CN oo •^ o r-- so oo (12 bo ys ; 2 gi rls...Grew, K. S., & Mather, N, (2001). Woodcock-Johnson HI Tests of Achievement. Itasca, IL: Riverside, ABOUT THE AUTHORS J. RON NELSON (CEC #060), Co-Directot and Associate Professor, Center for At-Risk Children's Services, University of Nebraska, Lincoln...

  19. Pewter and pewterers from Port Royal, Jamaica: flatware before 1692 

    E-Print Network [OSTI]

    Gotelipe-Miller, Shirley

    1990-01-01

    Figure 2: The INA/TAMU Archaeological Excavations at Port Royal Figure 3: Detail of ar i e a la Mod by William Hogarth Figure 4: Der Kandelgiesser (The Pewterer) by P. Abraham Figure 5: Scrap Pewter Recovered from INA/TAMU Excavations Figure 6: Array... Land Holdings in Port Royal Table 3: Childermas Family Tree Table fn Benning Land Holdings in Port Royal Table 5: Benning Family Tree Table 6: Benning Family Timeline Table 7: Comparison of Probate Inventories Table 8: Comparison of Prices derived...

  20. Symmetrical Multilevel Diversity Coding and Subset Entropy Inequalities 

    E-Print Network [OSTI]

    Jiang, Jinjing

    2013-05-29

    )L c?(U)H(XU |Sn1 , . . . , Snm)+ n m? ?=1 f?(?)H(S?)? n m? ?=1 f?(?)?(n)? (2.40) for any m = 1, . . . , L. In particular, let m = L, and note that for ? = 1 the optimal 16 solution to the linear program (2.19) is unique and is given by c... perfectly reconstruct the sources S1, . . . , S|U | no matter what the realization of U is. 7 Formally, an (n, (M1, . . . ,ML)) code is defined by a collection of L encoding functions: el : L? ?=1 Sn? ? {1, . . . ,Ml}, ?l = 1, . . . , L (2.1) and 2L...

  1. Factored Language Models and Generalized Parallel Backoff Jeff A. Bilmes Katrin Kirchhoff

    E-Print Network [OSTI]

    Washington at Seattle, University of

    model, a word is viewed as a vec- tor of k factors, so that wt {f1 t , f2 t , . . . , fK t }. Fac- tors. An FLM is a model over factors, i.e., p(f1:K t |f1:K t-1:t-n), that can be factored as a product of probabilities of the form p(f|f1, f2, . . . , fN ). Our task is twofold: 1) find an appropriate set of factors

  2. On the Global Linear Convergence of the ADMM with Multi-Block Variables

    E-Print Network [OSTI]

    Ferguson, Thomas S.

    be formulated as min ~f1(x1) + ~f2(x2) + · · · + ~fN (xN ) s.t. A1x1 + A2x2 + · · · + AN xN = b, xi Xi, i = 1 of Minnesota, Minneapolis, MN 55455, USA. 1 #12;indicator function, i.e., (1.1) can be rewritten as min f1(x1 an Department of Systems Engineering and Engineering Management, The Chinese University of Hong Kong, Shatin

  3. Modeliranje suma v astronomskih podatkih

    E-Print Network [OSTI]

    ?umer, Slobodan

    sirina spektralne crte model opazovanje #12;2 = NX i=1 (fi m i )2 2 i #12;p(fi|, i) = 1 p 2 2 i exp (fi Cebisova osme stopnje] / #12;2 ln L = C 1 2 NX i=1 (fi m i )2 2 i + s2 1 2 NX i=1 ln( 2 i + s2 ) ln L = C 1 2 NX i=1 (fi m i )2 2 i #12;3 [f1 m(x1), . . . fN m(xN )] 2 6 6 6 6 6 4 1 2 1 0 · · · 0 0 1 2 2

  4. Semiempirical range and stopping power values for heavy ions 

    E-Print Network [OSTI]

    Schilling, Ralph Franklin, III

    1968-01-01

    and Graphs . . . 21 USE OF THE TABLES AND GRAPHS. . . . . . . 2$ VALIDITY OF SZii1IEviPIRICAL RESULTS. . . . 26 RZFZRZNCES. APPENDIX . . ~ ~ ~ ~, ~ ~ ~ 28 29 LIST OF FIGURES Stopping power curves for 1ons of various atomic numbers 1n Al. The energy... Uj U1 ~ ~ ~ y m I (D r r co ~ ~ ~ a NOND t(1 Q ~ ~ ~ ~ rn a I 4 lf', CJ a Nu ++O (T N 4' 0 In ~ 4 Ill ~ ~ ~ ~ ~ N QNONQ 0 0 nj Q' ~ ~ \\ ((1 Q Q ~ 4 W Gj Q ~l (T ocoa ~ rn a' 4 C' ~ N N N ((I C tn ~ ~ ~ N rh fn nJ 0 Nt 0 0 0 rn...

  5. A survey of Meloidogyne spp. parasitizing peaches in Texas and their effects on four peach rootstocks 

    E-Print Network [OSTI]

    Johnson, Jerral D

    1964-01-01

    compared with reproduction or 42 p nt of' ttl M. ~fnfta ~fc it p p 1 tf ns, nd 31 percent f th N, ~fnco nit cr1. ta populati (Tables 3, 5 and. 7). The wide variation that existed between populations of M. ~fn nfta ~fc nit (Bable 2B) nd N. ~no nits a... ntt nd n. dn ntta var. st . Ft nt nts. Reptr. Supp. 8K-8 McBeth, C. W. , A. L. Taylor, and A. L. Smith. 1941. Note on staining nematodes in root tissue. Proc. Helminth. Soc. Wash. 8: 26. 32. 33 ' 34. 35. McClintock, J. A. 1922. Resistant plants...

  6. Identification of powered parafoil-vehicle dynamics from modelling and flight test data 

    E-Print Network [OSTI]

    Hur, Gi-Bong

    2006-08-16

    S consisting of N particles P1,...,PN, suppose that n -m gen- eralized speeds have been introduced, and let vPir denote the rth partial velocity of Pi. Then, if Ri is the resultant of all contact and body forces acting on Pi, then the n -m quantities F1,...,Fn-m...IDENTIFICATION OF POWERED PARAFOIL-VEHICLE DYNAMICS FROM MODELLING AND FLIGHT TEST DATA A Dissertation by GI-BONG HUR Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree...

  7. Probing of a human proteome microarray with a recombinant pathogen protein reveals a novel mechanism by which hookworms suppress B cell receptor signaling

    E-Print Network [OSTI]

    Tribolet, Leon; Cantacessi, Cinzia; Pickering, Darren; Navarro, Severine; Doolan, Denise; Trieu, Angela; Fei, Huang; Chao, Yang; Hofmann, Andreas; Gasser, Robin; Giacomin, Paul; Loukas, Alex

    2014-08-19

    , Sigma). 154 155 Flow cytometry and cell sorting 156 Cells were stained with fluorophore-conjugated antibodies against CD19 (HIB19), CD20 (2H7), 157 CD3 (OKT3), CD4 (OKT4), CD14 (61D3) CD69 (FN50), HLA-DR (LN3), CD80 (2D10.4), CD86 158 (IT2.2) (all... . Controlling the false discovery rate in 462 behavior genetics research. Behav Brain Res 2001; 125:279-84. 463 30. Boyle EI, Weng S, Gollub J, et al. GO::TermFinder--open source software for accessing Gene 464 Ontology information and finding significantly...

  8. BPA-2011-00619-FOIA Request

    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 WebQuantity ofkandz-cm11 OutreachProductswsicloudwsiclouddenDVA N C E D B L O O DBiomassBudgetAugust 19, 2009E+^ ,0, 2011 In1-Fn J"rt

  9. BPA-2011-00621-FOIA Correspondence

    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 WebQuantity ofkandz-cm11 OutreachProductswsicloudwsiclouddenDVA N C E D B L O O DBiomassBudgetAugust 19, 2009E+^ ,0, 2011 In1-Fn

  10. 15N

    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 WebQuantity ofkandz-cm11 Outreach Home RoomPreservationBio-InspiredAtmosphericdevicesPPO RetireesLecturersO β+-DecayBeFCPTC HourlyFN

  11. 17N

    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 WebQuantity ofkandz-cm11 Outreach Home RoomPreservationBio-InspiredAtmosphericdevicesPPO RetireesLecturersOThermal NeutronC β--DecayFN

  12. 17N

    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 WebQuantity ofkandz-cm11 Outreach Home RoomPreservationBio-InspiredAtmosphericdevicesPPO RetireesLecturersOThermal NeutronC β--DecayFN

  13. 17N(3).PDF

    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 WebQuantity ofkandz-cm11 Outreach Home RoomPreservationBio-InspiredAtmosphericdevicesPPO RetireesLecturersOThermal NeutronC β--DecayFN

  14. 17N.PDF

    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 WebQuantity ofkandz-cm11 Outreach Home RoomPreservationBio-InspiredAtmosphericdevicesPPO RetireesLecturersOThermal NeutronC β--DecayFN

  15. TUNL Nuclear Data Project, HTML Project

    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-effectWorking With LivermoreSustainableDEPARTMENT OFEnergy-8, 2004N 10NA =A =FN 13N

  16. TUNL Nuclear Data Project, HTML Project

    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-effectWorking With LivermoreSustainableDEPARTMENT OFEnergy-8, 2004N 10NA =A =FN

  17. Summary of ILD performance at SPS1a'

    E-Print Network [OSTI]

    Mikael Berggren; Nicola d'Ascenzo; Peter Schade; Olga Stempel

    2009-02-14

    The performance of the ILD detector at the ILC for the analysis of $\\mu$ and $\\tau$ channels at the SUSY benchmark-point SPS1a' has been studied with full detector simulation. It is concluded that if 500 fb$^{-1}$ is delivered to the experiment, $\\Delta(\\MXN{1}) = 920 \\MeVcc$, $\\Delta(\\msmul) = 100 \\MeVcc$, $\\Delta(\\MXN{2}) = 1.38 ~\\GeVcc$, and $\\Delta(\\sigma(\\eeto \\smul \\smul))$ = 1.35 fb can be achieved from the $\\mu$ channels alone. The preliminary results from the $\\stau$ channels, indicates that $\\Delta(P_{\\tau}) = 13 $ % is also achievable.

  18. Prospects on the search for invisible Higgs decays in the ZH channel at the LHC and HL-LHC: A Snowmass White Paper

    E-Print Network [OSTI]

    Hideki Okawa; Josh Kunkle; Elliot Lipeles

    2014-12-16

    We show prospects on a search for invisible decays of a Higgs boson at the Large Hadron Collider (LHC) and High Luminosity LHC (HL-LHC). This search is performed on a Higgs boson produced in association with a Z boson. We expect that the branching ratio of 17-22% (6-14%) could be excluded at 95% confidence level with 300 fb^{-1} (3000 fb^{-1}) of data at sqrt(s)=14 TeV. The range indicates different assumptions on the control of systematic uncertainties. Interpretations with Higgs-portal dark matter models are also considered.

  19. Measurement of the Forward-Backward Charge Asymmetry and Extraction of sin(2) ?[eff over W] in pp-bar?Z/?*+X?e(+)e(?)+X Events Produced at s?=1.96??TeV

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Hensel, Carsten; Clutter, Justace Randall; Moulik, Tania; Wilson, Graham Wallace; Abazov, V. M.; Abbott, B.; Abolins, M.; Acharya, B. S.; Adams, M.

    2008-11-06

    ?effW at the Z-pole is 0:23149 ? 0:00013 [2]. Two sin2?effW measurements are more than 2 standard deviations from the world average value: that from the charge asym- metry for b quark production (A0;bFB) from the LEP and SLD collaborations [3...] and that from neutrino and antineutrino cross sections from the NuTeV collaboration [4]. The A0;bFB measurement is sensitive to the couplings of b quarks to the Z boson, and the NuTeV measurement is sensitive to the couplings of u and d quarks to the Z boson...

  20. Search for the Higgs boson in the $\\mathrm{b\\bar{b}}$ decay channel using the CMS detector

    E-Print Network [OSTI]

    Caterina Vernieri for the CMS Collaboration

    2014-11-17

    A search for the standard model Higgs boson in the \\bbbar decay channel has been carried out with the CMS detector at the LHC collider. The searched production modes are the associated VH production, the VBF production and the production in association with top quark pairs (ttH). The analyses are based on pp collision data collected at centre-of-mass energies of 7 and 8 TeV, corresponding to integrated luminosities of 5 fb$^{-1}$ and 20 fb$^{-1}$, respectively. The strategy and results of the searches are reported.

  1. Photon + jets at D0

    E-Print Network [OSTI]

    Lars Sonnenschein

    2009-06-15

    Photon plus jet production has been studied by the D0 experiment in Run II of the Fermilab Tevatron Collider at a centre of mass energy of sqrt{s}=1.96 TeV. Measurements of the inclusive photon, inclusive photon plus jet, photon plus heavy flavour jet cross sections and double parton interactions in photon plus three jet events are presented. They are based on integrated luminosities between 0.4 fb$^-1 and 1.0 fb^-1. The results are compared to perturbative QCD calculations in various approximations.

  2. Measurement of the tt¯ production cross section in pp collisions at ?s=7 TeV in dilepton final states containing a ?

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

    Chatrchyan, S.; Khachatryan, V.; Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Bergauer, T.; Dragicevic, M.; Erö, J.; Fabjan, C.; Friedl, M.; et al

    2012-06-19

    The top quark pair production cross section is measured in dilepton events with one electron or muon, and one hadronically decaying ? lepton from the decay tt¯?(l?l)(?h??)bb¯, (l=e,?). The data sample corresponds to an integrated luminosity of 2.0 fb?¹ for the electron channel and 2.2 fb?¹ for the muon channel, collected by the CMS detector at the LHC. This is the first measurement of the tt¯ cross section explicitly including ? leptons in proton-proton collisions at ?s=7 TeV. The measured value ?tt¯=143±14(stat)±22(syst)±3(lumi) pb is consistent with the standard model predictions.

  3. Validation of a 4D-PET Maximum Intensity Projection for Delineation of an Internal Target Volume

    SciTech Connect (OSTI)

    Callahan, Jason; Kron, Tomas; Peter MacCallum Department of Oncology, The University of Melbourne, Melbourne ; Schneider-Kolsky, Michal; Dunn, Leon; Thompson, Mick; Siva, Shankar; Aarons, Yolanda; Peter MacCallum Department of Oncology, The University of Melbourne, Melbourne ; Binns, David; Hicks, Rodney J.; Peter MacCallum Department of Oncology, The University of Melbourne, Melbourne

    2013-07-15

    Purpose: The delineation of internal target volumes (ITVs) in radiation therapy of lung tumors is currently performed by use of either free-breathing (FB) {sup 18}F-fluorodeoxyglucose-positron emission tomography-computed tomography (FDG-PET/CT) or 4-dimensional (4D)-CT maximum intensity projection (MIP). In this report we validate the use of 4D-PET-MIP for the delineation of target volumes in both a phantom and in patients. Methods and Materials: A phantom with 3 hollow spheres was prepared surrounded by air then water. The spheres and water background were filled with a mixture of {sup 18}F and radiographic contrast medium. A 4D-PET/CT scan was performed of the phantom while moving in 4 different breathing patterns using a programmable motion device. Nine patients with an FDG-avid lung tumor who underwent FB and 4D-PET/CT and >5 mm of tumor motion were included for analysis. The 3 spheres and patient lesions were contoured by 2 contouring methods (40% of maximum and PET edge) on the FB-PET, FB-CT, 4D-PET, 4D-PET-MIP, and 4D-CT-MIP. The concordance between the different contoured volumes was calculated using a Dice coefficient (DC). The difference in lung tumor volumes between FB-PET and 4D-PET volumes was also measured. Results: The average DC in the phantom using 40% and PET edge, respectively, was lowest for FB-PET/CT (DCAir = 0.72/0.67, DCBackground 0.63/0.62) and highest for 4D-PET/CT-MIP (DCAir = 0.84/0.83, DCBackground = 0.78/0.73). The average DC in the 9 patients using 40% and PET edge, respectively, was also lowest for FB-PET/CT (DC = 0.45/0.44) and highest for 4D-PET/CT-MIP (DC = 0.72/0.73). In the 9 lesions, the target volumes of the FB-PET using 40% and PET edge, respectively, were on average 40% and 45% smaller than the 4D-PET-MIP. Conclusion: A 4D-PET-MIP produces volumes with the highest concordance with 4D-CT-MIP across multiple breathing patterns and lesion sizes in both a phantom and among patients. Freebreathing PET/CT consistently underestimates ITV when compared with 4D PET/CT for a lesion affected by respiration.

  4. Measurements of the masses, lifetimes and mixings of B hadrons at the Tevatron

    SciTech Connect (OSTI)

    Malde, S; /Oxford U.

    2009-09-01

    The Tevatron, with p{bar p} collisions at {radical}s = 1.96 TeV, can produce all flavors of B hadrons and allows for unprecedented studies in the B physics sector. The CDF and D0 collaborations have more than 5 fb{sup -1} of data recorded. I present here a selection of recent results on the masses, lifetimes and mixings of B hadrons using between 1.0 and 2.8 fb{sup -1} of data.

  5. Measuring the dark matter equation of state

    E-Print Network [OSTI]

    Ana Laura Serra; Mariano Javier de León Domínguez Romero

    2011-05-30

    The nature of the dominant component of galaxies and clusters remains unknown. While the astrophysics community supports the cold dark matter (CDM) paradigm as a clue factor in the current cosmological model, no direct CDM detections have been performed. Faber and Visser 2006 have suggested a simple method for measuring the dark matter equation of state that combines kinematic and gravitational lensing data to test the widely adopted assumption of pressureless dark matter. Following this formalism, we have measured the dark matter equation of state for first time using improved techniques. We have found that the value of the equation of state parameter is consistent with pressureless dark matter within the errors. Nevertheless, the measured value is lower than expected because typically the masses determined with lensing are larger than those obtained through kinematic methods. We have tested our techniques using simulations and we have also analyzed possible sources of error that could invalidate or mimic our results. In the light of this result, we can now suggest that the understanding of the nature of dark matter requires a complete general relativistic analysis.

  6. Isospin violating dark matter in Stückelberg portal scenarios

    E-Print Network [OSTI]

    Victor Martin-Lozano; Miguel Peiro; Pablo Soler

    2015-03-05

    Hidden sector scenarios in which dark matter (DM) interacts with the Standard Model matter fields through the exchange of massive Z' bosons are well motivated by certain string theory constructions. In this work, we thoroughly study the phenomenological aspects of such scenarios and find that they present a clear and testable consequence for direct DM searches. We show that such string motivated St\\"uckelberg portals naturally lead to isospin violating interactions of DM particles with nuclei. We find that the relations between the DM coupling to neutrons and protons for both, spin-independent (fn/fp) and spin-dependent (an/ap) interactions, are very flexible depending on the charges of the quarks under the extra U(1) gauge groups. We show that within this construction these ratios are generically different from plus and minus 1 (i.e. different couplings to protons and neutrons) leading to a potentially measurable distinction from other popular portals. Finally, we incorporate bounds from searches for dijet and dilepton resonances at the LHC as well as LUX bounds on the elastic scattering of DM off nucleons to determine the experimentally allowed values of fn/fp and an/ap.

  7. Effect of Fast Neutron Irradiation on the Properties of a Superconducting (Bi-2223+0.8% 238U)/Ag-Tape

    E-Print Network [OSTI]

    Goncharov, I N; Voloshin, I F; Kalinov, A V; Fisher, L M

    2001-01-01

    The critical current density (J_c) of a high temperature superconductor doped with uranium can be significantly increased due to neutron irradiation which results in the production of fission fragment tracks. The disadvantages of such a method in case of enriched U introducing into the Bi-2223/Ag-tape are analysed in this paper. The main of them is a high level of long-lived radioactivity after thermal neutron irradiation. The alternative method, in which unenriched uranium introduced into HTS is irradiated with fast neutrons of a>1.4 MeV energy has been checked experimentally. There was a very small fraction of slow neutrons in the reactor beam. At liquid nitrogen temperatures, increasing J_c was found to be observed only at B>0.5 T and for low enough fluences F_n (as compared with the calculated optimum one). For higher F_n, the values of J_c degraded at any B though the radioactivity level is much lower than in the method, where thermal neutrons are used.

  8. Search for Dark Matter in Events with a Z Boson and Missing Transverse Momentum in pp Collisions at ?s = 8 TeV with the ATLAS Detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search is presented for production of dark-matter particles recoiling against a leptonically decaying Z boson in 20.3??fb[superscript ?1] of pp collisions at ?s = 8??TeV with the ATLAS detector at the Large Hadron Collider. ...

  9. Search for new phenomena in the dijet mass distribution using pp collision data at ?s = 8 TeV with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    Dijet events produced in LHC proton-proton collisions at a center-of-mass energy ?s = 8??TeV are studied with the ATLAS detector using the full 2012 data set, with an integrated luminosity of 20.3??fb[superscript ?1]. Dijet ...

  10. Flavor tagged time-dependent angular analysis of the B[0 over s] ? J/?? decay and extraction of ??[subscript s] and the weak phase ?[subscript s] in ATLAS

    E-Print Network [OSTI]

    Taylor, Frank E.

    A measurement of the B[0 over s] ? J/?? decay parameters, updated to include flavor tagging is reported using 4.9??fb[superscript ?1] of integrated luminosity collected by the ATLAS detector from ?s = 7??TeV pp collisions ...

  11. Measurement of the WW cross section in ?s = 7 TeV pp collisions with the ATLAS detector and limits on anomalous gauge couplings

    E-Print Network [OSTI]

    Taylor, Frank E.

    This Letter reports a measurement of the WW production cross section in?s = 7 TeV pp collisions using data corresponding to an integrated luminosity of 1.02 fb[superscript ?1] collected with the ATLAS detector. Using ...

  12. Search for direct slepton and gaugino production in final states with two leptons and missing transverse momentum with the ATLAS detector in pp collisions at ?s = 7 TeV

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for the electroweak pair production of charged sleptons and weak gauginos decaying into final states with two leptons is performed using 4.7 fb[superscript ?1] of proton–proton collision data at ?s = 7 TeV recorded ...

  13. Evidence for Electroweak Production of W[superscript ±]W[superscript ±]jj in pp Collisions at ?s = 8 TeV with the ATLAS Detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    This Letter presents the first study of W[superscript ±]W[superscript ±]jj, same-electric-charge diboson production in association with two jets, using 20.3??fb[superscript ?1] of proton-proton collision data at ?s = 8??TeV ...

  14. Search for the decay B[superscript +]-->K[subscript s] [superscript 0] K[subscript s] [superscript 0] pi[superscript +

    E-Print Network [OSTI]

    Zhao, M.

    We search for charmless decays of charged B mesons to the three-body final state B[superscript +]-->K[subscript s] [superscript 0] K[subscript s] [superscript 0] pi[superscript +]. Using a data sample of 423.7??fb[superscript ...

  15. Measurement of D(0)-D? (0) Mixing from a Time-Dependent Amplitude Analysis of D(0) -->K(+)pi(-)pi(0) Decays

    E-Print Network [OSTI]

    Cowan, Ray Franklin

    We present evidence of D[superscript 0]-D?[superscript 0] mixing using a time-dependent amplitude analysis of the decay D0?K[superscript +]?[superscript -]?[superscript 0] in a data sample of 384??fb[superscript -1] ...

  16. Search for Higgs Boson Pair Production in the ??b[bar over b] Final State Using pp Collision Data at ?s = 8 TeV from the ATLAS Detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    Searches are performed for resonant and nonresonant Higgs boson pair production in the ??b[bar over b] final state using 20??fb[superscript ?1] of proton-proton collisions at a center-of-mass energy of 8 TeV recorded with ...

  17. Measurement of Semileptonic B Decays into Orbitally Excited Charmed Mesons

    E-Print Network [OSTI]

    Zhao, M.

    We present a study of B decays into semileptonic final states containing charged and neutral D1(2420) and D2*(2460). The analysis is based on a data sample of 208??fb-1 collected at the ?(4S) resonance with the BABAR ...

  18. Measurement of the t-channel single top-quark production cross section in pp collisions at ?s = 7 TeV with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    We report a measurement of the cross section of single top-quark production in the t -channel using 1.04 fb[superscript ?1] of pp collision data at ?s = 7 TeV recorded with the ATLAS detector at the LHC. Selected events ...

  19. Search for Lepton Flavor Violating Decays tau--->l-Ks0 with the BABAR Experiment

    E-Print Network [OSTI]

    Fisher, Peter H.

    A search for the lepton flavor violating decays tau--->l-KS0 (l=e or mu) has been performed using a data sample corresponding to an integrated luminosity of 469??fb[superscript -1], collected with the BABAR detector at the ...

  20. Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in pp collisions at ?s = 8 TeV

    E-Print Network [OSTI]

    Taylor, Frank E.

    The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3 fb[superscript ?1] of data ...

  1. Measurement of the W[superscript ±]Z production cross section and limits on anomalous triple gauge couplings in proton–proton collisions at ?s = 7 TeV with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    This Letter presents a measurement of W[superscript ±]Z production in 1.02 fb[superscript ?1] of pp collision data at ?s = 7 TeV collected by the ATLAS experiment in 2011. Doubly leptonic decay events are selected with ...

  2. Search for Flavor-Changing Neutral Current and Lepton-Flavor Violating Decays of D[superscript 0]-->l+l-

    E-Print Network [OSTI]

    Cowan, Ray Franklin

    We report on a search for the flavor-changing neutral current decays D0?e+e- and D0??+?-, and the lepton-flavor violating decay D0?e±??. The measurement is based on 122??fb-1 of data collected by the BABAR detector at the ...

  3. Search for light top squark pair production in final states with leptons and b-jets with the ATLAS detector in ?s = 7 TeV proton–proton collisions

    E-Print Network [OSTI]

    Taylor, Frank E.

    The results of a search for pair production of light top squarks are presented, using 4.7 fb[superscript ?1] ?s = 7 TeV proton–proton collisions collected with the ATLAS detector at the Large Hadron Collider. This search ...

  4. Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in ?s = 7 TeV pp collisions with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for the direct production of charginos and neutralinos in final states with three electrons or muons and missing transverse momentum is presented. The analysis is based on 4.7 fb[superscript -1] of ?s = 7 TeV ...

  5. [MRO] Search for resonant diboson production in the WW/WZ???jj decay channels with the ATLAS detector at ?s=7??TeV

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for resonant diboson production using a data sample corresponding to 4.7??fb[superscript -1] of integrated luminosity collected by the ATLAS experiment at the Large Hadron Collider in pp collisions at ?s=7??TeV ...

  6. Study of the e?e???????? process using initial state radiation with BABAR

    E-Print Network [OSTI]

    Cowan, Ray Franklin

    The process e?e????????? has been studied at a center-of-mass energy near the ?(4S) resonance using a 89.3??fb?¹ data sample collected with the BABAR detector at the PEP-II collider. From the measured 3? mass spectrum we ...

  7. Measurement of W? and Z? production cross sections in pp collisions at ?s = 7 TeV and limits on anomalous triple gauge couplings with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    This Letter presents measurements of l[superscript ±]?? and l[superscript +l[superscript ?]? (l=e,?) production in 1.02 fb[superscript ?1] of pp collision data recorded at ?s = 7 TeV with the ATLAS detector at the LHC in ...

  8. Search for new particles decaying to ZZ using final states with leptons and jets with the ATLAS detector in ?s = 7 TeV proton–proton collisions

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search is presented for a narrow resonance decaying to a pair of Z bosons using data corresponding to 1.02 fb[superscript ?1] of integrated luminosity collected by the ATLAS experiment from pp collisions at ?s = 7 TeV. ...

  9. Search for events with large missing transverse momentum, jets, and at least two tau leptons in 7 TeV proton–proton collision data with the ATLAS detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    A search for events with large missing transverse momentum, jets, and at least two tau leptons has been performed using 2 fb[superscript ?1] of proton–proton collision data at ?s = 7 TeV recorded with the ATLAS detector ...

  10. Robustness of TransEuropean Gas Networks: The Hot Backbone Rui Carvalho, 1, # Lubos Buzna, 2, 3, + Flavio Bono, 4, # Eugenio Gutierrez, 4 Wolfram Just, 1 and David Arrowsmith 1

    E-Print Network [OSTI]

    Just, Wolfram

    instead of oil for transporta­ tion [2], and gas­fired power plants are responsible for the production topological data with information on inter­country flows, we estimate the global load of the network and its, 89.75.Fb I. INTRODUCTION The world is going through a period when research in energy is overarching

  11. Search for massive supersymmetric particles decaying to many jets using the ATLAS detector in pp collisions at ?s = 8 TeV

    E-Print Network [OSTI]

    Taylor, Frank E.

    Results of a search for decays of massive particles to fully hadronic final states are presented. This search uses 20.3??fb[superscript ?1] of data collected by the ATLAS detector in ?s = 8??TeV proton-proton collisions ...

  12. Improving the Ocean Initialization of Coupled HurricaneOcean Models Using Feature-Based Data Assimilation

    E-Print Network [OSTI]

    Rhode Island, University of

    oceanic features in the Gulf of Mexico, including the Loop Current (LC), Loop Current eddies [i.e., warm-assimilated" case, the LC, a single WCR, and a single CCR are assimilated into NAVOCEANO's Global Digitized to the depth of the 26°C isotherm. Assuming the AXBT profiles are truth, the TCHP rms error for the F-B SHA

  13. CDF note 9642 Search for the Standard Model Higgs boson in the ET plus jets sample

    E-Print Network [OSTI]

    Fermilab

    CDF note 9642 Search for the Standard Model Higgs boson in the ET plus jets sample The CDF Collaboration URL http://www-cdf.fnal.gov (Dated: August 17, 2009) We search for the Higgs boson produced; the Higgs boson decays into a bb pair. This analysis is an update of the previous one to 3.6 fb-1 of CDF

  14. Measurement of B(D+->(K)over-bar(*0)l(+)nu(l))

    E-Print Network [OSTI]

    Ammar, Raymond G.; Besson, David Zeke; Zhao, X.

    2002-11-01

    Using 13.53 fb(-1) of CLEO data, we have measured the ratios of the branching fractions R-e(+),R-mu(+) and the combined branching fraction ratio R-l(+), defined by R-l(+)=[B(D+-->(K) over bar (*0)l(+)nu(l))]/[B(D+-->K(-) ...

  15. Observation of B -> K-S(0)pi(+)pi(-) and evidence for B -> K-*+/-pi(-/+)

    E-Print Network [OSTI]

    Ammar, Raymond G.; Besson, David Zeke; Zhao, X.

    2002-12-01

    We report on a search for charmless hadronic B decays to the three-body final states K(S)(0)h(+)pi(-), K(+)h(-)pi(0), K(S)(0)h(+)pi(0) (h(+/-) denotes a charged pion or kaon), and their charge conjugates, using 13.5 fb(-1) ...

  16. Rate measurement of D0 -> K+pi-pi 0 and constraints on D-0 D(0)over-bar mixing

    E-Print Network [OSTI]

    Ammar, Raymond G.; Bean, Alice; Besson, David Zeke; Zhao, X.

    2001-08-01

    We present an observation and time-integrated rate measurement of the decay D-0-->K(+)pi (-)pi (0) produced in 9 fb(-1) of e(+)e(-) collisions near the Y(4S) resonance. The signal is inconsistent with an upward fluctuation ...

  17. Inclusive Search for Standard Model Higgs Boson Production in the WW Decay Channel Using the CDF II Detector

    E-Print Network [OSTI]

    Xie, Si

    We present a search for standard model (SM) Higgs boson production using pp? collision data at ?s=1.96??TeV, collected with the CDF II detector and corresponding to an integrated luminosity of 4.8??fb[superscript -1]. We ...

  18. Search for the Associated Production of the Standard-Model Higgs Boson in the All-Hadronic Channel

    E-Print Network [OSTI]

    Makhoul, K.

    We report on a search for the standard-model Higgs boson in pp? collisions at ?s=1.96??TeV using an integrated luminosity of 2.0??fb[superscript -1]. We look for production of the Higgs boson decaying to a pair of bottom ...

  19. Combined Tevatron upper limit on gg --> H --> W[superscript +]W[superscript -] and constraints on the Higgs boson mass in fourth-generation fermion models

    E-Print Network [OSTI]

    Paus, Christoph M. E.

    We combine results from searches by the CDF and D0 collaborations for a standard model Higgs boson (H) in the process gg-->H-->W+W- in pp? collisions at the Fermilab Tevatron Collider at [sqrt]s=1.96??TeV. With 4.8??fb-1 ...

  20. Combination of searches for the Higgs boson using the full CDF data set

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We present a combination of searches for the standard model Higgs boson using the full CDF run II data set, which corresponds to an integrated luminosity of 9.45–10.0??fb[superscript ?1] collected from s? = 1.96??TeV p[¯ ...

  1. Measurement of the properties of a Higgs boson in the four-lepton final state

    E-Print Network [OSTI]

    Apyan, Aram

    The properties of a Higgs boson candidate are measured in the H ? ZZ ? 4? decay channel, with ? = e, ?, using data from pp collisions corresponding to an integrated luminosity of 5.1??fb[superscript ?1] at the center-of-mass ...

  2. BROWNIAN DYNAMICS SIMULATIONS OF POLYMERS AND SOFT MATTER

    E-Print Network [OSTI]

    Doyle, Patrick S.

    (free-draining), the drag force is taken as Stokes drag on a sphere Fd i = - dri dt - u (ri) (2) where of a drag force Fd i from the particle moving through the viscous solvent, a Brownian force FB i due force. The technique takes advantage of the fact that there is a large separation in time scales between

  3. Laser-produced plasma-wall interaction O. RENNER,1

    E-Print Network [OSTI]

    Liska, Richard

    Laser-produced plasma-wall interaction O. RENNER,1 R. LISKA,2 AND F.B. ROSMEJ3,4 1 Institute, France (RECEIVED 30 August 2009; ACCEPTED 21 September 2009) Abstract Jets of laser­generated plasma surfaces (walls). The pilot experiments carried out on the iodine laser system (5­200 J, 0.44 mm, 0

  4. The Effect of Equilibrating Mounted Dental Stone Casts in Maximum Intercuspation on the Occlusal Harmony of an Indirect Restoration 

    E-Print Network [OSTI]

    Benson, Peter Andrew

    2013-12-13

    , 1982. 13(2): p. 187-93. 9. Celenza, F.V., The centric position: replacement and character. J Prosthet Dent, 1973. 30(4 Pt 2): p. 591-8. 30 10. Hollinger, F.B., et al., Reduction in risk of hepatitis transmission by heat- treatment of a human...

  5. Search for a Higgs-like boson decaying to two photons in proton antiproton collisions at center of mass energy of 1.96 TeV

    E-Print Network [OSTI]

    Chen, Guo

    2013-05-31

    We present a search for the Standard Model (SM) Higgs boson decaying to two photons using the 9.6 fb-1 of proton antiproton collisions at center of mass energy of 1.96 TeV collected by the D0 detector at the Tevatron from ...

  6. Measurement of Collins asymmetries in inclusive production of charged pion pairs in e[superscript +]e[superscript ?] annihilation at BABAR

    E-Print Network [OSTI]

    Lees, J.?P.

    We present measurements of Collins asymmetries in the inclusive process e[superscript +]e[superscript ?] ? ??X, where ? stands for charged pions, at a center-of-mass energy of 10.6 GeV. We use a data sample of 468??fb[superscript ...

  7. Measurement of the Branching Fractions of the Radiative Leptonic ? Decays ? ? e??[bar over ?] and ? ? ???[bar over ?] at BABAR

    E-Print Network [OSTI]

    Lees, J.?P.

    We perform a measurement of the ? ? l??[bar over ?] (l = e,?) branching fractions for a minimum photon energy of 10 MeV in the ? rest frame, using 431??fb[superscript -1] of e[superscript +]e[superscript -] collisions ...

  8. Measurements of Direct CP Asymmetries in B ? X[subscript s]? Decays Using Sum of Exclusive Decays

    E-Print Network [OSTI]

    Lees, J.?P.

    We measure the direct CP violation asymmetry, A[subscript CP], in B ? X[subscript s]? and the isospin difference of the asymmetry, ?A[subscript CP], using 429??fb[superscript -1] of data collected at ?(4S) resonance with ...

  9. Time-Frequency Analysis as Probabilistic Inference

    E-Print Network [OSTI]

    Turner, Richard E.

    2014-11-06

    ) and (19) yields: (21) 6176 IEEE TRANSACTIONS ON SIGNAL PROCESSING, VOL. 62, NO. 23, DECEMBER 1, 2014 Fig. 1. Relationships between classical and probabilistic time-frequency anal- ysis. A complex filter bank (cFB, ) is formed from a set of filters...

  10. Low-frequency square-wave electronic ballast with resonant ignition using digital mode and power

    E-Print Network [OSTI]

    Low-frequency square-wave electronic ballast with resonant ignition using digital mode and power both the functions of a resonant circuit for lamp ignition and a current controlled low frequency of the FB converter according to the lamp requirements. I. INTRODUCTION The primary motivation for using low

  11. On the Predictability of Large Transfer TCP Throughput Georgia Tech

    E-Print Network [OSTI]

    Dovrolis, Constantinos

    'D¤¢¥BWYS48¤j¢¥¤§1(B@!#¨FB ¥g13GHI!#BCG¦13A1(Q@¢A1$BC'D¤`¢E1(%%)F¨F§13¥¨!$BWcf1(g¦s1$TP!#"©E¨#¢©ª!('£¥¤ l

  12. Functional Characterization of the Arabidopsis b-Ketoacyl-Coenzyme A Reductase Candidates of the

    E-Print Network [OSTI]

    Kunst, Ljerka

    Chemistry, Rothamsted Research, Harpenden, Herts AL5 2JQ, United Kingdom (F.B., R.P.H., J.A.N.); University of British Columbia, Vancouver, British Columbia, Canada V6T 1Z4 (X.W., F.L., H.Z., L.K.); and Donald (VLCFAs; .18 carbon) are precursors of sphingolipids, triacylglycerols, cuticular waxes, and suberin

  13. How large is the contribution of cosmic web to $?_?$ ? A preliminary study on a novel inhomogenous model

    E-Print Network [OSTI]

    Stefano Viaggiu; Marco Montuori

    2013-07-04

    The distribution of matter in the universe shows a complex pattern, formed by cluster of galaxies, voids and filaments denoted as cosmic web. Different approaches have been proposed to model such structure in the framework of the general relativity. Recently, one of us has proposed a generalization ($\\Lambda$FB model) of the Fractal Bubble model, proposed by Wiltshire, which accounts for such large scale structure. The $\\Lambda$FB model is an evolution of FB model and includes in a consistent way a description of inhomogeneous matter distribution and a $\\Lambda$ term. Here we analyze the $\\Lambda$FB model focusing on the relation between cosmological parameters. The main result is the consistency of $\\Lambda$CDM model values for $\\Omega_{\\Lambda0}$ ($\\approx 0.7$) and $\\Omega_{k0}$ ($|\\Omega_{k0}|<\\approx 0.01$) with a large fraction of voids. This allows to quantify to which extent the inhomogeneous structure could account for $\\Lambda$ constant consistently with standard values of the other cosmological parameters.

  14. Assorted weak matrix elements involving the bottom quark

    E-Print Network [OSTI]

    C. Bernard; T. Blum; T. DeGrand; C. E. DeTar; Steven Gottlieb; U. M. Heller; J. E. Hetrick; C. McNeile; K. Rummukainen; R. L. Sugar; D. Toussaint; M. Wingate

    1996-08-15

    As part of a larger project to estimate the fB decay constant, we are recalculating fB_static using a variational smearing method in an effort to improve accuracy. Preliminary results for the static B_B parameter and HQET two point functions are also presented.

  15. Search for Magnetic Monopoles in ?s=7??TeV pp Collisions with the ATLAS Detector

    E-Print Network [OSTI]

    Taylor, Frank E.

    This Letter presents a search for magnetic monopoles with the ATLAS detector at the CERN Large Hadron Collider using an integrated luminosity of 2.0??fb[superscript -1] of pp collisions recorded at a center-of-mass energy ...

  16. Measurements of the properties of the Higgs boson using the ATLAS Detector

    E-Print Network [OSTI]

    Filipuzzi, Marco; The ATLAS collaboration

    2015-01-01

    A review of the Higgs coupling and spin/CP properties measurements with up to 25 fb-1 of 7 TeV and 8 TeV pp collision data collected by the ATLAS detector in 2011 and 2012 will be presented.

  17. Combination of couplings of the Higgs boson by the ATLAS experiment with Run 1 data

    E-Print Network [OSTI]

    Lu, Nan; The ATLAS collaboration

    2015-01-01

    A review of the Run 1 combination of the mass. coupling, and spin CP properties measurements of the Higgs boson using the ATLAS detector and up to 25 fb-1 of 7 TeV and 8 TeV pp collision data collected in 2011 and 2012 will be presented.

  18. LCPHSM2001055 Determination of the Higgs boson spin

    E-Print Network [OSTI]

    LC­PHSM­2001­055 Determination of the Higgs boson spin with a Linear e + e \\Gamma Collider M of a light Higgs boson is studied at threshold and compared to the expectation of several spin as­ sumptions luminosity of 20 fb \\Gamma1 allow confirmation of the scalar nature of the Higgs Boson. INTRODUCTION

  19. arXiv:hepex/0505096 Measurement of the Higgs Boson Mass

    E-Print Network [OSTI]

    ################ arXiv:hep­ex/0505096 v1 30 May 2005 Measurement of the Higgs Boson Mass for the measurement of the Higgs boson mass. An integrated luminosity of 500 fb 1 is assumed. For Higgs boson masses of 120, 150 and 180 GeV the uncertainty on the Higgs boson mass measurement is estimated to be 40, 65

  20. Search for New Physics with a Dijet Plus Missing ET Signature in pp? Collisions at ?s=1.96??TeV

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We present results of a signature-based search for new physics using a dijet plus missing transverse energy (E[subscript T]T) data sample collected in 2??fb[superscript -1] of pp? collisions at ?s=1.96??TeV with the CDF ...

  1. Measurement of Z gamma production in pp[over-bar] collisions at [sqrt]s=1.96 TeV

    E-Print Network [OSTI]

    Paus, Christoph M. E.

    The production rate and kinematics of photons produced in association with Z bosons are studied using 2??fb-1 of pp[over-bar] collision data collected at the Collider Detector at Fermilab. The cross section for pp[over-bar] ...

  2. Search for a Fermiophobic Higgs Boson Decaying into Diphotons in pp-bar Collisions at sqrt[s]=1.96 TeV

    E-Print Network [OSTI]

    Xie, Si

    A search for a narrow diphoton mass resonance is presented based on data from 3.0??fb[superscript -1] of integrated luminosity from pp? collisions at ?s=1.96??TeV collected by the CDF experiment. No evidence of a resonance ...

  3. Search for Dark Matter in Events with One Jet and Missing Transverse Energy in pp? Collisions at ?s=1.96??TeV

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We present the results of a search for dark matter production in the monojet signature. We analyze a sample of Tevatron pp? collisions at ?s=1.96??TeV corresponding to an integrated luminosity of 6.7??fb[superscript -1] ...

  4. Combination of CDF and D0 measurements of the W boson helicity in top quark decays

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We report the combination of recent measurements of the helicity of the W boson from top quark decay by the CDF and D0 collaborations, based on data samples corresponding to integrated luminosities of 2.7–5.4??fb[superscript ...

  5. Measurement of the Cross Section for Prompt Isolated Diphoton Production in pp[over-bar] Collisions at [sqrt]s=1.96??TeV

    E-Print Network [OSTI]

    Bauer, Gerry P.

    This Letter reports a measurement of the cross section of prompt isolated photon pair production in pp[over-bar] collisions at a total energy [sqrt]s=1.96??TeV using data of 5.36??fb-1 integrated luminosity collected with ...

  6. Search for a Standard Model Higgs Boson in WH-->lvbb-bar in pp-bar Collisions at sqrt[s]=1.96 TeV

    E-Print Network [OSTI]

    Xie, Si

    We present a search for a standard model Higgs boson produced in association with a W boson using 2.7??fb[superscript -1] of integrated luminosity of pp? collision data taken at ?s=1.96??TeV. Limits on the Higgs boson ...

  7. Combination of tevatron searches for the standard model Higgs Boson for observing antiferromagnetism and superfluidity

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We combine searches by the CDF and D0 Collaborations for a Higgs boson decaying to W[superscript +]W[superscript -]. The data correspond to an integrated total luminosity of 4.8 (CDF) and 5.4 (D0) fb[superscript -1] of pp? ...

  8. Direct Measurement of the W Production Charge Asymmetry in p(p)over-bar Collisions at root s = 1.96 TeV

    E-Print Network [OSTI]

    Paus, Christoph M. E.

    We present the first direct measurement of the W production charge asymmetry as a function of the W boson rapidity yW in p(p)over-bar collisions at ?s=1.96??TeV. We use a sample of W?e? events in data from 1??fb[superscript ...

  9. Top-Quark Mass Measurement Using Events with Missing Transverse Energy and Jets at CDF

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We present a measurement of the top-quark mass using a sample of tt? events in 5.7??fb[superscript -1] of integrated luminosity from pp? collisions at the Fermilab Tevatron with ?s=1.96??TeV and collected by the CDF II ...

  10. Search for High-Mass e+e- Resonances in pp-bar Collisions at sqrt[s]=1.96 TeV

    E-Print Network [OSTI]

    Makhoul, K.

    A search for high-mass resonances in the e[superscript +]e[superscript -] final state is presented based on 2.5??fb[superscript -1] of ?s=1.96??TeV pp? collision data from the CDF II detector at the Fermilab Tevatron. The ...

  11. Measurement of the Single Top Quark Production Cross Section and |V[subscript tb]| in Events with One Charged Lepton, Large Missing Transverse Energy, and Jets at CDF

    E-Print Network [OSTI]

    Aaltonen, T.

    We report a measurement of single top quark production in proton-antiproton collisions at a center-of-mass energy of ?s = 1.96??TeV using a data set corresponding to 7.5??fb[superscript -1] of integrated luminosity collected ...

  12. Measurement of the Ratio sigmatt[over-bar] /sigmaZ/gamma*-->ll and Precise Extraction of the tt[over-bar] Cross Section

    E-Print Network [OSTI]

    Paus, Christoph M. E.

    We report a measurement of the ratio of the tt[over-bar] to Z/gamma* production cross sections in [sqrt]s=1.96??TeV pp[over-bar] collisions using data corresponding to an integrated luminosity of up to 4.6??fb[superscript ...

  13. Observation of Electroweak Single Top-Quark Production

    E-Print Network [OSTI]

    Xie, Si

    We report the observation of single top-quark production using 3.2??fb[superscript -1] of pp? collision data with ?s=1.96??TeV collected by the Collider Detector at Fermilab. The significance of the observed data is 5.0 ...

  14. First Observation of Vector Boson Pairs in a Hadronic Final State at the Tevatron Collider

    E-Print Network [OSTI]

    Paus, Christoph M. E.

    We present the first observation in hadronic collisions of the electroweak production of vector boson pairs (VV, V=W, Z) where one boson decays to a dijet final state. The data correspond to 3.5??fb[superscript -1] of ...

  15. Search for Production of Heavy Particles Decaying to Top Quarks and Invisible Particles in pp[over-bar] Collisions at [sqrt]s=1.96??TeV

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We present a search for a new particle T? decaying to top quark via T?-->t+X, where X is an invisible particle. In a data sample with 4.8??fb[superscript -1] of integrated luminosity collected by the CDF II detector at ...

  16. Search for Top-Quark Production via Flavor-Changing Neutral Currents in W+1 Jet Events at CDF

    E-Print Network [OSTI]

    Xie, Si

    We report on a search for the non-standard-model process u(c)+g?t using pp? collision data collected by the Collider Detector at Fermilab II detector corresponding to 2.2??fb[superscript -1]. The candidate events are ...

  17. Search for a Dark Matter Candidate Produced in Association with a Single Top Quark in pp? Collisions at ?s=1.96??TeV

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We report a new search for dark matter in a data sample of an integrated luminosity of 7.7??fb[superscript -1] of Tevatron pp? collisions at ?s=1.96??TeV, collected by the CDF II detector. We search for production of a ...

  18. Exclusion of an Exotic Top Quark with-4/3 Electric Charge Using Soft Lepton Tagging

    E-Print Network [OSTI]

    Paus, Christoph M. E.

    We present a measurement of the electric charge of the top quark using pp[over-bar] collisions corresponding to an integrated luminosity of 2.7??fb[superscript -1] at the CDF II detector. We reconstruct tt[over-bar] events ...

  19. Search for New T? Particles in Final States with Large Jet Multiplicities and Missing Transverse Energy in pp? Collisions at ?s=1.96??TeV

    E-Print Network [OSTI]

    Bauer, Gerry P.

    We present a search for a new particle T? decaying to a top quark via T??t+X, where X goes undetected. We use a data sample corresponding to 5.7??fb[superscript -1] of integrated luminosity of pp? collisions with ?s=1.96??TeV, ...

  20. Search for Gluino-Mediated Bottom Squark Production in pp? Collisions at ?s=1.96??TeV

    E-Print Network [OSTI]

    Gomez-Ceballos, Guillelmo

    We report on a search for the supersymmetric partner of the bottom quark produced from gluino decays in data from 2.5??fb[superscript -1] of integrated luminosity collected by the Collider Detector at Fermilab at ?s=1.96??TeV. ...