National Library of Energy BETA

Sample records for q4 jul-sep q3

  1. Mathematics 1052 Exam 2, May 3rd, 2014 Q1 Q2 Q3 Q4 Q5 Q6 Total Bonus

    E-Print Network [OSTI]

    Kaygun, Atabey

    Mathematics 1052 Exam 2, May 3rd, 2014 Q1 Q2 Q3 Q4 Q5 Q6 Total Bonus 15pts 20pts 10pts 15pts 30pts) (9 points) n=1 1 n(n+2) #12;Mathematics 1052 Exam 2, May 3rd, 2014 2. Consider the region bounded above about the line y = 1. Page 2 of 5 #12;Mathematics 1052 Exam 2, May 3rd, 2014 3. (10 points) (a

  2. Q2 Q3 Q4 Q4 Q3 Q2 Q1 Q1 Q2 Q3 Q4 Q3 Q2 Q1 Q1 Q2 Q3 Q4 Q4 Q3 Q2 Q1

    E-Print Network [OSTI]

    .00/W Concentrating Solar Power (CSP and CPV) 6 MWac of concentrating solar capacity was installed installations totaled 723 MW in Q1 2013, up 33% over Q1 2012 Cumulative operating PV capacity in the U.S. now, installers, and manufacturers to collect granular data on the U.S. solar market. This data provides

  3. Observations from The EV Project in Q4 2013

    SciTech Connect (OSTI)

    John Smart

    2014-02-01

    This is a summary report for The EV Project 4th quarter 2013 reports. It describes electric vehicle driver driving and charging behavior observed in Q4. It is the same report as the previously approved/published Q3 2013 report, only the numbers have been updated. It is for public release and does not have limited distribution.

  4. Sep Nov Jan Mar May Jul Sep Nov Jan Mar May Jul Sep Nov Jan

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700 GJO-2003-411-TACe: SUBJIHX:ontine atSep Nov

  5. Microsoft Word - S07079_jul_sep_10.doc

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbinsMonumentThird6010 Task U.S. Department ofJuly

  6. Microsoft Word - S08308_FFA_ jul_sep_2011

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbinsMonumentThird6010 Task11 GroundwaterCommunityFernald1

  7. SPEAR 3 Quarterly Report Jul-Sep 2000

    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 RoomPreservation of Fe(II) byMultidayAlumni > The2/01/12 Page 1 ofSuper1 THIS PAGEthroughJuly

  8. IBM Systems Journal Q3 2002 Comparing Autonomic & Proactive Computing

    E-Print Network [OSTI]

    Somayaji, Anil

    IBM Systems Journal Q3 2002 Comparing Autonomic & Proactive Computing Roy Want , Trevor Pering between proactive computing and autonomic computing, considering the design of systems that are beyond principles we call proactive computing, enabling the transition from today's interactive systems to proactive

  9. Lone Star I (Q3) Wind Farm | 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 APPENDIXsource History ViewInformationWindsCompressedListguided wavesLone Star I (4Q07)Q3)

  10. FY 2014 Q3 Metric Summary | Department of Energy

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:FinancingPetroleum12, 2015Executive Order14, 20111,FY 2007 FeeFederal Realin TargetEnergy4 Q3

  11. Geometry of an elliptic-difference equation related to Q4

    E-Print Network [OSTI]

    James Atkinson; Phil Howes; Nalini Joshi; Nobutaka Nakazono

    2015-06-15

    In this paper, we investigate a nonlinear non-autonomous elliptic difference equation, which was constructed by Ramani, Carstea and Grammaticos by integrable deautonomization of a periodic reduction of the discrete Krichever-Novikov equation, or Q4. We show how to construct it as a birational mapping on a rational surface blown up at eight points in $\\mathbb P^1\\times \\mathbb P^1$, and find its affine Weyl symmetry, placing it in the geometric framework of the Painlev\\'e equations. The initial value space is ell-$A_0^{(1)}$ and its symmetry group is $W(F_4^{(1)})$. We show that the deautonomization is consistent with the lattice-geometry of Q4 by giving an alternative construction, which is a reduction from Q4 in the usual sense. A more symmetric reduction of the same kind provides another example of a second-order integrable elliptic difference equation.

  12. A Newsletter of the Lee Kuan Yew School of Public Policy 03ISSUE Jul/Sep

    E-Print Network [OSTI]

    Chin, Wei Ngan

    reserve Chairman Ben Bernanke's claim that we may be seeing some "green shoots" of recovery, most people Fights poverty and Illiteracy 24 Singapore president Nathan HostsTea for Students,Faculty Mpp Students

  13. Evaluation of EHD enhancement and thermoacoustic refrigeration for naval applications. Technical report, Jul-Sep 91

    SciTech Connect (OSTI)

    Memory, S.B.

    1991-12-01

    An evaluation has been made of two different techniques which could prove valuable for Naval refrigeration needs in the future. The first is electrohydrodynamic (EHD) enhancement of pool boiling and condensation heat transfer; this has been shown to provide significant enhancements for both modes of heat transfer under certain conditions and could provide increases in efficiency of present vapor-compression systems. EHD techniques are quite advanced and prototype condenser and evaporator bundles are currently being tested. The second technique is an alternative refrigeration technology called thermoacoustic refrigeration; alternative technologies have become increasingly attractive over recent years due to environmental concerns over CFCs. Thermoacoustic refrigeration uses acoustic power to pump heat from a low temperature source to a high temperature sink. It is still in the early stages of development and can presently accommodate only small thermal loads. However, its general principles of operation have been proven and its resent capacity and efficiency limitations are not seen as a problem in the long term. Electrohydrodynamic Enhancement, Boiling and Condensation, Thermoacoustic Refrigeration.

  14. Microsoft Word - SPEAR3 Jul-Sep 02 Qtrly Rpt.doc

    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 Room NewsInformationJessework uses concrete7 Assessment ofLana Cox (803) TO:1 of5 RPI28433- 1 -

  15. Dish Stirling High Performance Thermal Storage FY14Q4 Quad Chart

    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:Speeding accessby aLED Street Lighting Host Site: City ofNovelQ3: Charles

  16. Dish Stirling High Performance Thermal Storage FY15Q3 Quad Chart

    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:Speeding accessby aLED Street Lighting Host Site: City ofNovelQ3:Q3: Charles

  17. Far-ultraviolet observations of comet C/2001 Q4 (NEAT) with FIMS/SPEAR

    SciTech Connect (OSTI)

    Lim, Y.-M.; Min, K.-W. [Korea Advanced Institute of Science and Technology (KAIST), 291 Daehak-ro, Yuseong-gu, Daejeon 305-701 (Korea, Republic of); Feldman, P. D. [Department of Physics and Astronomy, Johns Hopkins University, 3400 North Charles Street, Baltimore, MD 21218 (United States); Han, W. [Korea Astronomy and Space Science Institute (KASI), 776 Daedeokdae-ro, Yuseong-gu, Daejeon 305-348 (Korea, Republic of); Edelstein, J., E-mail: ymlim@kaist.ac.kr [Space Sciences Laboratory, University of California, Berkeley, 7 Gauss Way, Berkeley, CA 94720 (United States)

    2014-02-01

    We present the results of far-ultraviolet observations of comet C/2001 Q4 (NEAT) that were made with the Far-Ultraviolet Imaging Spectrograph on board the Korean satellite STSAT-1. The observations were conducted in two campaigns during its perihelion approach between 2004 May 8 and 15. Based on the scanning mode observations in the wavelength band of 1400-1700 Å, we have constructed an image of the comet with an angular size of 5°×5°, which corresponds to the central coma region. Several important fluorescence emission lines were detected including S I multiplets at 1429 and 1479 Å, C I multiplets at 1561 and 1657 Å, and the CO A{sup 1}?-X{sup 1}?{sup +} Fourth Positive system; we have estimated the production rates of the corresponding species from the fluxes of these emission lines. The estimated production rate of CO was Q {sub CO} = (2.65 ± 0.63) × 10{sup 28} s{sup –1}, which is 6.2%-7.4% of the water production rate and is consistent with earlier predictions. The average carbon production rate was estimated to be Q{sub C} = ?1.59 × 10{sup 28} s{sup –1}, which is ?60% of the CO production rate. However, the observed carbon profile was steeper than that predicted using the two-component Haser model in the inner coma region, while it was consistent with the model in the outer region. The average sulfur production rate was Q{sub S} = (4.03±1.03) × 10{sup 27} s{sup –1}, which corresponds to ?1% of the water production rate.

  18. Dish Stirling High Performance Thermal Storage FY14Q3 Quad Chart

    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:Speeding accessby aLED Street Lighting Host Site: City ofNovelQ3: Charles E.

  19. Chiral O(Q^4) two-body operators for s-wave pion photoproduction on the NN system

    E-Print Network [OSTI]

    A. Gardestig

    2006-04-16

    The two-body currents for s-wave pion photoproduction on the NN system are derived to O(Q^4) in chiral perturbation theory. For the interesting case of 3S1 1S0 transitions, we show that an axial isovector two-nucleon contact term connects the short-distance physics of pion photoproduction to pion production and several important electroweak reactions. We also find that the standard chiral Lagrangian gives a gamma pi pi N N vertex that have not been explicitly mentioned in previous literature. The corresponding Feynman rule is presented here and some processes where it should be important are briefly discussed.

  20. 2012_Q4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergyTher i n c i p a l De p u t y A s s i sEnergy It is the intent of the

  1. 2013_Q4.indd

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergyTher i n c i p a l De p u t y A s s i sEnergyEnergy The intent

  2. FORMALDEHYDE IN COMETS C/1995 O1 (HALE-BOPP), C/2002 T7 (LINEAR), AND C/2001 Q4 (NEAT): INVESTIGATING THE COMETARY ORIGIN OF H2CO

    E-Print Network [OSTI]

    FORMALDEHYDE IN COMETS C/1995 O1 (HALE-BOPP), C/2002 T7 (LINEAR), AND C/2001 Q4 (NEAT of formaldehyde (H2CO) have been conducted toward comets C/1995 O1 (Hale-Bopp), C/2001 Q4 (NEAT), and C/2002 T72CO other than the comet nucleus. The extended source of formaldehyde is probably grains composed

  3. 2014_Q3.indd

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergyTher i n c i p a l De p u t y A s s iof1 of 8 2 of 8 3 ofRuleWe We We el lc lc lc

  4. U.S. Residential Photovoltaic (PV) System Prices, Q4 2013 Benchmarks: Cash Purchase, Fair Market Value, and Prepaid Lease Transaction Prices

    SciTech Connect (OSTI)

    Davidson, C.; James, T. L.; Margolis, R.; Fu, R.; Feldman, D.

    2014-10-01

    The price of photovoltaic (PV) systems in the United States (i.e., the cost to the system owner) has dropped precipitously in recent years, led by substantial reductions in global PV module prices. This report provides a Q4 2013 update for residential PV systems, based on an objective methodology that closely approximates the book value of a PV system. Several cases are benchmarked to represent common variation in business models, labor rates, and module choice. We estimate a weighted-average cash purchase price of $3.29/W for modeled standard-efficiency, polycrystalline-silicon residential PV systems installed in the United States. This is a 46% decline from the 2013-dollar-adjusted price reported in the Q4 2010 benchmark report. In addition, this report frames the cash purchase price in the context of key price metrics relevant to the continually evolving landscape of third-party-owned PV systems by benchmarking the minimum sustainable lease price and the fair market value of residential PV systems.

  5. The Gell-Mann-Okubo and Colemann-Glashow relations for octet and decuplet baryons in the $SU_q(3)$ quantum algebra

    E-Print Network [OSTI]

    A. Carcamo

    2006-08-10

    The q-deformed Clebsch-Gordan coefficients corresponding to the $\\lrpy{3}\\times\\lrpy{21}$ reduction of the $SU_q(3)$ quantum algebra are computed. From these results and using the quantum Clebsch-Gordan coefficients for the $\\lrpy{21}\\times\\lrpy{21}$ reduction found by Zhong Qi Ma, the q-deformed Gell-Mann-Okubo mass relations for octet and decuplet baryons are determined by generalizing the procedure used for the SU(3) algebra. We also determine the Coleman-Glashow relations for octet and decuplet baryons in the $SU_q(3)$ algebra. Finally, by using the experimental particle masses of the octet and decuplet baryons, two values of the $q$-parameter are found and adjusted for the predicted masses expressions (one for the Gell-Mann-Okubo mass relations and the other for the Coleman-Glashow relations) and a possible physical interpretation is given.

  6. A new family of $N$ dimensional superintegrable double singular oscillators and quadratic algebra $Q(3)\\oplus so(n) \\oplus so(N-n)$

    E-Print Network [OSTI]

    Md Fazlul Hoque; Ian Marquette; Yao-Zhong Zhang

    2015-04-20

    We introduce a new family of $N$-dimensional quantum superintegrable model consisting of double singular oscillators of type $(n,N-n)$. The special cases $(2,2)$ and $(4,4)$ were previously identified as the duals of 3- and 5-dimensional deformed Kepler-Coulomb systems with $u(1)$ and $su(2)$ monopoles respectively. The models are multiseparable and their wave functions are obtained in $(n,N-n)$ double-hyperspherical coordinates. We obtain the integrals of motion and construct the finitely generated polynomial algebra that is the direct sum of a quadratic algebra $Q(3)$ involving three generators, $so(n)$, $so(N-n)$ (i.e. $Q(3)\\oplus so(n) \\oplus so(N-n)$ ). The structure constants of the quadratic algebra themselves involve the Casimir operators of the two Lie algebras $so(n)$ and $so(N-n)$. Moreover, we obtain the finite dimensional unitary representations (unirreps) of the quadratic algebra and present an algebraic derivation of the degenerate energy spectrum of the superintegrable model.

  7. Genetic and physical mapping of the Treacher Collins syndrome locus with respect to loci in the chromosome 5q3 region

    SciTech Connect (OSTI)

    Jabs, E.W.; Li, Xiang; Coss, C.; Taylor, E. (Johns Hopkins School of Medicine, Baltimore, MD (United States)); Lovett, M. (Univ. of Texas Southwestern Medical Center, San Antonio, TX (United States)); Yamaoka, L.H.; Speer, M.C. (Duke Univ. Medical Center, Durham, NC (United States)); Cadle, R.; Hall, B. (Univ. of Kentucky, Lexington, KY (United States)); Brown, K. (Albert Einstein College of Medicine and Montefiore Medical Center, Bronx, NY (United States)) (and others)

    1993-10-01

    Treacher Collins syndrome is an autosomal dominant, craniofacial developmental disorder, and its locus (TCOF1) has been mapped to chromosome 5q3. To refine the location of the gene within this region, linkage analysis was performed among the TCOF1 locus and 12 loci (IL9, FGFA, GRL, D5S207, D5S210, D5S376, CSF1R, SPARC, D5S119, D5S209, D5S527, FGFR4) in 13 Treacher Collins syndrome families. The highest maximum lod score was obtained between loci TCOF1 and D5S210 (Z = 10.52; [theta] = 0.02 [+-] 0.07). The best order, IL9-GRL-D5S207/D5S210-CSF1R-SPARC-D5S119, and genetic distances among these loci were determined in the 40 CEPH families by multipoint linkage analysis. YAC clones were used to establish the order of loci, centromere-5[prime]GRL3[prime]-D5S207-D5S210-D5S376-CSF1R-SPARC-D5S119-telomere. By combining known physical mapping data with ours, the order of chromosome 5q3 markers is centomere-IL9-FGFA-5[prime]GRL3[prime]-D5s207-D5S210-D5S376-CSF1R-SPARC-D5S119-D5S209-FGFR4-telomere. Based on this order, haplotype analysis suggests that the TCOF1 locus resides distal CSF1R and proximal to SPARC within a region less than 1 Mb in size. 29 refs., 2 figs., 2 tabs.

  8. Q3 1997 STEO, Final

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets160Product: TotalCoalbed7 (Released July 8,

  9. Alcator C-MOD Quarterly Reports

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

    Reports Reports for 1997 Q1 (HTML) Q2 (HTML) Q3 (HTML) Q4 (HTML) Reports for 1998 Q1 (HTML) Q2 (HTML) Q3 (HTML) Q4 (HTML) Reports for 1999 Q1 (HTML) Q2 (HTML) Q3 (HTML) Q4 (HTML)...

  10. FY11 Q4 SHPM Whitepaper DRAFT

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

    Track Paper European Wind Energy Conference (EWEA) Annual Event April 16-19, 2012; Copenhagen, Denmark Prognostic Control to Enhance Offshore Wind Turbine Operations and...

  11. Microchannel Receiver Development- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Oregon State University project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  12. FY11 Q4 SHPM Whitepaper DRAFT

    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 -ORGANIZATION FY 2013MayUncosted of Energyf i c eN

  13. Adjustment patterns to commodity terms of trade shocks: the role of exchange rate and international reserves policies

    E-Print Network [OSTI]

    Aizenman, Joshua; Edwards, Sebastian; Riera-Crichton, Daniel

    2012-01-01

    Q3 1997 Q3 2003 Uruguay Q2 2004 Q4 2009 Venezuela, Rep. Bol.Q1 1989 Q1 1989 Venezuela, Rep. Bol. Q4 1990 Q1 1992 End Q4Peru, Uruguay and Venezuela. The data in this table show

  14. FOIA Quarterly Reports (Q3 2014)

    Broader source: Energy.gov [DOE]

    Report that captures quarterly FOIA data at the DOE level. Through the use of an Applied Programming Interface (or API), the information will display on www.FOIA.gov.

  15. FOIA Quarterly Reports (Q3 2013)

    Broader source: Energy.gov [DOE]

    The DOE’s mission is to advance the national, economic, and energy security of the United States; to promote scientific and technological innovation in support of that mission; and to ensure the...

  16. Q3 1996 STEO TEXT/TABLES

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1Markets160Product: TotalCoalbed

  17. Scattering Solar Thermal Concentrators- FY12 Q4

    Office of Energy Efficiency and Renewable Energy (EERE)

    This document summarizes the progress of this Penn State project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  18. Advanced Manufacture of Reflectors- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this University of Arizona project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  19. Next Generation Solar Collectors for CSP- FY12 Q4

    Office of Energy Efficiency and Renewable Energy (EERE)

    This document summarizes the progress of this 3M project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  20. Supercritical Carbon Dioxide Turbo-Expander- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this SWRI project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  1. CSP Tower Air Brayton Combustor- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this SWRI project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  2. Poison Control Center Management of Benzocaine Exposures

    E-Print Network [OSTI]

    Suchard, Jeffrey; Rudkin, Scott

    2004-01-01

    V:3, Jul-Sep 2004 Page 55 Poison Control Center Managementthe American Association of Poison Control Centers (AAPCC)answering the general poison information line of each PCC

  3. EERE PowerPoint 97-2004 Template: Green Version

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

    analysis; planned for Q3 to Q4 Calculated for Quaternary faults using stress field from borehole breakouts and fault-kinematic data March '15 & in progress Major Technical...

  4. Quantified Traveler: Travel Feedback Meets the Cloud to Change Behavior

    E-Print Network [OSTI]

    2013-01-01

    spent traveling (time, cost, CO2, and calories) was able toemissions (kg of CO2), calories burned, cost ($), and traveland cost (Q4) spent traveling did not shift awareness, the information on calories (Q3) and CO2 (

  5. Fluorescent Pigments for High-Performance Cool Roofing

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

    Identified, End Q2 3. 500g of 2 New Pigments, End Q3 4. ESR Measured on New Cool Roof Coating, End Q4 Budget: Total DOE to date: 474,132 Total future DOE : 0 Key Partners:...

  6. Flexible Assembly Solar Technology- FY13 Q3

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this BrightSource Energy project, funded by SunShot, for the second quarter of fiscal year 2013.

  7. Observations from The EV Project in Q3 2013

    SciTech Connect (OSTI)

    John Smart

    2013-12-01

    This is a brief report that summarizes results published in numerous other reports. It describes the usage of electric vehicles and charging units in the EV Project over the past 3 months. There is no new data or information provided in this report, only summarizing of information published in other reports (which have all been approved for unlimited distribution publication). This report will be posted to the INL/AVTA website for viewing by the general public.

  8. Microsoft Word - DOE_ANNUAL_METRICS_2009Q3.docx

    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 wouldMass map shines light on77 PAGE OF PAGESpersonal March 3, 2015CMMarchDOEER-0670T14404 Third

  9. Fluorescent Pigments for High-Performance Cool Roofing

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

    Q2 and Q6 2. 500g of 2 New Pigments, End Q3 and Q7 3. ESR Measured on New Cool Roof Coating, End Q4 and Q8 4. Potential Manufacturing Partner, Q3 and ongoing 5. Update BTO...

  10. Self-Cleaning CSP Optics with EDS- FY12 Q4

    Office of Energy Efficiency and Renewable Energy (EERE)

    This document summarizes the progress of this Boston University project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  11. On the physics of the $so_q(4)$ hydrogen atom

    E-Print Network [OSTI]

    P. G. Castro; R. Kullock

    2015-03-05

    In this work we investigate the $q$-deformation of the $so(4)$ dynamical symmetry of the hydrogen atom using the theory of the quantum group $su_q(2)$. We derive the energy spectrum in a physically consistent manner and find a degeneracy breaking as well as a smaller Hilbert space. We point out that using the deformed Casimir as was done before leads to inconsistencies in the physical interpretation of the theory.

  12. Baseload CSP Generation Integrated with Sulfur-Based Thermochemical Heat Storage- FY12 Q4

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this General Atomics project, funded by SunShot, for the fourth quarter of fiscal year 2012.

  13. Enclosure - FY 2015 Q4 Metrics Report 2015-11-02.xlsx

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:FinancingPetroleum Based|DepartmentStatementofAprilofEnergyEnSys Energy communities

  14. High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles - FY12 Q4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:FinancingPetroleum12,ExecutiveFinancing ProgramsDepartmentHigh-Efficiency Parking Lighting|

  15. FY 2014 Q4 Metrics Report 2014-11-06.xlsx

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:FinancingPetroleum12, 2015Executive Order14, 20111,FY 2007 FeeFederal Realin

  16. Microsoft PowerPoint - SRS Headcount by County of Residence Q4 FY 2013.pptx

    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 Room NewsInformationJesse BergkampCentermillionStockpileEqualArraysstructural stabilityInto

  17. Dish Stirling High Performance Thermal Storage FY14Q4 Quad Chart.

    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 submit theCovalentLaboratory | National(Technical Report) | SciTech Connect Dish

  18. SRS Employee Headcount by County of Residence Q4 FY15

    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 RoomPreservation of Fe(II) byMultidayAlumni > The2/01/12 Page 1NEWS MEDIA16,3 rd Quarter FY 20154

  19. Communication and Control for Quantum Circuits

    E-Print Network [OSTI]

    Patel, Yatish

    2010-01-01

    to Output. Classical bits cx and cz are trans- mitted to thePure Quantum h x y z s t cx yes yes yes yes yes yes yes czH q3 q4 zmeasure Correct c3 X cx q1, q0; cx q1, q2; correct

  20. Alcator C-Mod FY2007 Research Totals by Quarter

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

    7 Research Operations as of 83107 Research Days Research Weeks Total FY07 Research Weeks Q1 0.0 0.0 0.0 Q2 1.06 0.27 0.27 Q3 36.20 9.05 9.32 Q4 21.50 5.37 14.69 Detailed run run...

  1. Alcator C-Mod FY2008 Research Totals by Quarter

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

    8 Research Operations as of 52708 Research Days Research Weeks Total FY08 Research Weeks Q1 4.25 1.06 1.06 Q2 34.5 8.6 9.7 Q3 24.2 6.1 15.7 Q4 Detailed run descriptions can be...

  2. Second Quarter 2014 Volume 7, number 2

    E-Print Network [OSTI]

    .5% in Q2, 4.1% in Q3, and 2.6% in Q4. March projections for annual average real GDP provided, the Bureau of Labor Statistics (BLS) reported the Consumer Price Index for All Urban Consumers rose 1.1% year- over-year in February, while core inflation was up 1.6% for the same period. Consumer prices

  3. High-Temperature Falling-Particle Receiver- FY13 Q3

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this SNL project, funded by SunShot, for the third quarter of fiscal year 2013.

  4. More Than Smart Overview of Discussions Q3 2014 thru Q1 2015

    E-Print Network [OSTI]

    Stoltz, Brian M.

    Resources (DERs) · DERs include distributed renewable generation, energy efficiency, energy storage California's vision for making Distributed Energy Resources (DER) significant contributors to resource Resources Plan Requirements · Identifies optimal locations for the deployment of Distributed Energy

  5. More Than Smart Overview of Discussions Q3 2014 thru Q1 2015

    E-Print Network [OSTI]

    Desbrun, Mathieu

    and energy policy targets regarding renewable and distributed energy resources. · Participants: · Caltech to scale adoption of renewables and distributed energy resources. · Identified key issues that needed and distributed resources in California began at Caltech-Resnick Institute Grid2020 workshop in Fall 2011

  6. Research Snapshot Third Quarter, Fiscal Year 2015 Proposals by Quarter Proposals Submitted Q3

    E-Print Network [OSTI]

    Bertini, Robert L.

    ,827; MCECS Cal Santiago, Raul B; Collaborative Research: Advantages and Impacts of a Multi-scale Wind Farm To Sediment Transfer Across Continental Margins And The Construction Of Delta Stratigraphic Architecture

  7. Research Snapshot Third Quarter, Fiscal Year 2015 Awards by Quarter Awards Received Q3

    E-Print Network [OSTI]

    Bertini, Robert L.

    Decision Making; Department of Health and Human Services; $500,000; SSW; Renewal Cahn, Katharine; Leadership Academy for Middle Managers; Department of Health and Human Services; $428,351; SSW; Renewal Models in Variational Data Assimilation; Naval Research Laboratory; $163,284; CLAS; Amendment Daim

  8. Low-Cost Metal Hydride TES Systems- FY13 Q3

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this SRNL project, funded by SunShot, for the third quarter of fiscal year 2013.

  9. Microsoft Word - Q3 MDA 8_11_2015 Update of $172M for Reposting...

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

    to deliver on its mission. BPA also funds regional efforts to protect and enhance fish and wildlife populations affected by hydropower development in the Columbia River...

  10. Dish/Stirling High-Performance Thermal Storge- FY13 Q3

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this SNL project, funded by SunShot, for the third quarter of fiscal year 2013.

  11. High-Efficiency Thermal Energy Storage System for CSP- FY13 Q3

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this ANL project, funded by SunShot, for the third quarter of fiscal year 2013.

  12. FY 2014 Q3 RCA CAP Performance Metrics Report 2014-09-05.xlsx

    Energy Savers [EERE]

    no later than CD-3. ContractProject Management Performance Metrics FY12-FY14: 52 completions through 3rd Qtr. CD-4: Critical Decision-4, Approve Start of OperationsProject...

  13. Advanced Low-Cost Recievers for Parabolic Troughs- FY13 Q3

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this Norwich project, funded by SunShot, for the third quarter of fiscal year 2013.

  14. A Small Particle Solar Receiver for High Temperature Brayton Power Cycles- FY13 Q3

    Broader source: Energy.gov [DOE]

    This document summarizes the progress of this San Diego State University project, funded by SunShot, for the third quarter of fiscal year 2013.

  15. Enclosure - FY 2015 Q3 Metrics Report 2015-08-12.xlsx

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:FinancingPetroleum Based|DepartmentStatementofAprilofEnergyEnSys Energy communities depend

  16. High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles - FY13 Q3

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:FinancingPetroleum12,ExecutiveFinancing ProgramsDepartmentHigh-Efficiency Parking Lighting||

  17. FY 2014 Q3 RCA CAP Performance Metrics Report 2014-09-05.xlsx

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:FinancingPetroleum12, 2015Executive Order14, 20111,FY 2007 FeeFederal Realin TargetEnergy4

  18. Dish Stirling High Performance Thermal Storage FY14Q3 Quad Chart.

    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 submit theCovalentLaboratory | National

  19. Dish Stirling High Performance Thermal Storage FY15Q3 Quad Chart (Technical

    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 submit theCovalentLaboratory | National(Technical Report) | SciTechReport) | SciTech

  20. SRS Employee Headcount by County of Residence Q3 FY15

    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 RoomPreservation of Fe(II) byMultidayAlumni > The2/01/12 Page 1NEWS MEDIA16,3 rd Quarter FY 2015

  1. Discovery of oscillatory dynamics of city-size distributions in world

    E-Print Network [OSTI]

    White, Douglas R.

    of pdf thru Skype you can ask questions, thru Humberto he will have a chat box to relay questions I test) China leads by 50 years in its Q values ­ up to 1850 PART III: Scaling Examples: Chinese-results are very similar, as reported for the 1- factor test. Q1 Q3 Q5 Q2 Q4 Q6 #12;7 Multiple measures of Q

  2. QuaRC Data Acquisition Card Support

    E-Print Network [OSTI]

    Arslan, Gürdal

    Clear HiQ Aero Q3 ControlPaQ-FW Q4 Q8 MultiQ-PCI Gumstix Card Config Buffered I/O Immediate I/O Time Watchdog Watchdog Clear DAQCard-6024e DAQCard-6062e DAQCard-6715 PCI-6023e PCI-6024e PCI-6025e PCI-6032e PCI-6034e PCI-6035e PCI-6036e PCI-6040e PCI-6052e PCI-6220 #12;QuaRC Data Acquisition Card Support

  3. Microsoft Word - Q3 MDA 8_11_2015 Update of $172M for Reposting Final 4pm.docx

    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 Room NewsInformationJessework uses concrete7 Assessment ofLana Cox (803) TO:1 of 51Proposal FormThis

  4. 3Q/4Q99 F-Area Hazardous Waste Management Facility Corrective Action Report - Third and Fourth Quarter 1999, Volumes I and II

    SciTech Connect (OSTI)

    Chase, J.

    2000-05-12

    Savannah River Site (SRS) monitors groundwater quality at the F-Area Hazardous Waste management Facility (HWMF) and provides results of this monitoring to the South Carolina Department of Health and Environmental Control (SCDHEC) semiannually as required by the Resource Conservation and Recovery Act (RCRA) permit. SRS also performs monthly sampling of the Wastewater Treatment Unit (WTU) effluent in accordance with Section C of the Underground Injection Control (UIC) application.

  5. Environ. Sci. Technol. 19Q4,28, 1422-1429 Rapid Kinetics of Cu(I I) Adsorption/Desorption on Goethite

    E-Print Network [OSTI]

    Sparks, Donald L.

    /Desorption on Goethite Paul R. Grossl' and Donald L. Sparks Department of Piant and Soil Sciences, University of Delaware, Washington 99352 The kinetics of Cu2+adsorption/desorption on goethite (a-FeOOH) was evaluated using/desorption on goethite. The rate of these relaxations (7)decreased with an increase in pH, alongthe adsorption edge

  6. DOE/EIA-0202(84/4Q) Short-Term Energy Outlook Quarterly Projections

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct: Crude7)8)4)1Q)3Q)4Q)

  7. DOE/EIA-0202(85/1Q) Short-Term Energy Outlook Quarterly Projections

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct: Crude7)8)4)1Q)3Q)4Q)1Q)

  8. DOE/EIA-0202(85/2Q) Short-Term Energy Outlook

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct: Crude7)8)4)1Q)3Q)4Q)1Q)2Q)

  9. 1. (25 pts) Three point charges, q1, q2 and q3 that have the same +2 Coulomb charge are fixed to a circle of radius

    E-Print Network [OSTI]

    Akerib, Daniel S.

    of 6.0 nF and a plate area of 2 2 5.0 10 m- × is connected to a 12 V battery. a. What is the electric A wire and the magnetic field at point O is zero tesla. a. Determine the value of the current, I

  10. Canonical factorization and diagonalization of Baxterized braid matrices: Explicit constructions and applications

    E-Print Network [OSTI]

    A. Chakrabarti

    2003-05-07

    Braid matrices $\\hat{R}(\\theta)$, corresponding to vector representations, are spectrally decomposed obtaining a ratio $f_{i}(\\theta)/f_{i}(-\\theta)$ for the coefficient of each projector $P_{i}$ appearing in the decomposition. This directly yields a factorization $(F(-\\theta))^{-1}F(\\theta)$ for the braid matrix, implying also the relation $\\hat{R}(-\\theta)\\hat{R}(\\theta)=I$.This is achieved for $GL_{q}(n),SO_{q}(2n+1),SO_{q}(2n),Sp_{q}(2n)$ for all $n$ and also for various other interesting cases including the 8-vertex matrix.We explain how the limits $\\theta \\to \\pm \\infty$ can be interpreted to provide factorizations of the standard (non-Baxterized) braid matrices. A systematic approach to diagonalization of projectors and hence of braid matrices is presented with explicit constructions for $GL_{q}(2),GL_{q}(3),SO_{q}(3),SO_{q}(4),Sp_{q}(4)$ and various other cases such as the 8-vertex one. For a specific nested sequence of projectors diagonalization is obtained for all dimensions. In each factor $F(\\theta)$ our diagonalization again factors out all dependence on the spectral parameter $\\theta$ as a diagonal matrix. The canonical property implemented in the diagonalizers is mutual orthogonality of the rows. Applications of our formalism to the construction of $L-$operators and transfer matrices are indicated. In an Appendix our type of factorization is compared to another one proposed by other authors.

  11. SELF-CONSISTENT SIZE AND VELOCITY DISTRIBUTIONS OF COLLISIONAL CASCADES

    SciTech Connect (OSTI)

    Pan, Margaret [Department of Astronomy, University of California, Berkeley, CA 94720 (United States); Schlichting, Hilke E., E-mail: mpan@astro.berkeley.edu, E-mail: hilke@ucla.edu [Department of Earth and Space Sciences, University of California, Los Angeles, CA 90095 (United States)

    2012-03-10

    The standard theoretical treatment of collisional cascades derives a steady-state size distribution assuming a single constant velocity dispersion for all bodies regardless of size. Here we relax this assumption and solve self-consistently for the bodies' steady-state size and size-dependent velocity distributions. Specifically, we account for viscous stirring, dynamical friction, and collisional damping of the bodies' random velocities in addition to the mass conservation requirement typically applied to find the size distribution in a steady-state cascade. The resulting size distributions are significantly steeper than those derived without velocity evolution. For example, accounting self-consistently for the velocities can change the standard q = 3.5 power-law index of the Dohnanyi differential size spectrum to an index as large as q = 4. Similarly, for bodies held together by their own gravity, the corresponding power-law index range 2.88 < q < 3.14 of Pan and Sari can steepen to values as large as q = 3.26. Our velocity results allow quantitative predictions of the bodies' scale heights as a function of size. Together with our predictions, observations of the scale heights for different-sized bodies for the Kuiper belt, the asteroid belt, and extrasolar debris disks may constrain the mass and number of large bodies stirring the cascade as well as the colliding bodies' internal strengths.

  12. Energy Efficiency and Conservation Block Grant (EECBG): Better Buildings Neighborhood Program Final Report

    SciTech Connect (OSTI)

    Donnelly, Kat A.

    2014-01-10

    The Neighbor to Neighbor Energy Challenge (N2N) brought together a consortium of 14 leading clean energy rural, suburban, and low income communities throughout Connecticut. N2N was awarded $4.2 million from the U.S. Department of Energy (DOE) competitive BetterBuildings Neighborhood Program on August 10, 2010 to run a two-year pilot program (plus one year of transition and evaluation) (Award No. EMCBC- 00969-10). N2N tested innovative program models and hypotheses for improving Connecticut’s existing residential energy efficiency programs that are overseen by the ratepayer fund board and administered by CT utilities. N2N’s original goal was to engage 10 percent of households in participating communities to reduce their energy usage by 20 percent through energy upgrades and clean energy measures. N2N planned for customers to complete more comprehensive whole-home energy efficiency and clean energy measures and to achieve broader penetration than existing utility-administered regulated programs. Since this was an ARRA award, we report the following figures on job creation in Table 1. Since N2N is not continuing in its current form, we do not provide figures on job retention. Table 1 N2N Job Creation by Quarter Jobs Created 2010 Q4 6.65 2011 Q1 7.13 2011 Q2 4.98 2011 Q3 9.66 2011 Q4 5.43 2012 Q1 11.11 2012 Q2 6.85 2012 Q3 6.29 2012 Q4 6.77 2013 Q1 5.57 2013 Q2 8.35 2013 Q3 6.52 Total 85.31 The N2N team encountered several gaps in the existing efficiency program performance that hindered meeting N2N’s and DOE’s short-term program goals, as well as the State of Connecticut’s long-term energy, efficiency, and carbon reduction goals. However, despite the slow program start, N2N found evidence of increasing upgrade uptake rates over time, due to delayed customer action of one to two years from N2N introduction to completion of deeper household upgrades. Two main social/behavioral principles have contributed to driving deeper upgrades in CT: 1. Word of mouth, where people share their experience with others, which leads to others to take action; and 2. Self-herding, where people follow past behavior, which leads to deeper and deeper actions within individual households.

  13. Low voltage vertical recording preamplifier for hard disk drives 

    E-Print Network [OSTI]

    Mellachervu, Ramachandra Murthy

    2004-11-15

    CA1G mL + s2[CCgs+Cpi(C+Cgs)]g mNGmL 1 + s bracketleftBig 2C GmLAo + Cgs gmN + gpi(C+Cgs) gmNGmLAo bracketrightBig + s2 [2CCgs+Cpi(C+Cgs)]Aog mNGmL (6.22) The terms used have been shown in Fig.29. A1 = GmLRGmL where RGmL is the output resistance... Q2 Q4 Vout/2 Q3 RL Cpi Cpi GmL LR Cgs Ib 3Ib/8 3Ib/8 Vbias VCC VEE C Fig. 29. Schematic to understand signal feedthrough due to parasitic base-emitter ca- pacitor The equation can be simplified if we assume gmN >> GmLAo6 and can be written as, Vo Vin...

  14. Appl. Math. Lett. Vol. 3, No. 4, pp. 75-79, 1990 08934659pQ $3.00 + 0.00 Printed in Great Britain. All rights reserved Copyright@ 1990 Pergamon Press plc

    E-Print Network [OSTI]

    Hofbauer, Josef

    . All rights reserved Copyright@ 1990 Pergamon Press plc Adaptive Dynamics and Evolutionary Stability J

  15. Final_report_pub1.pdf

    SciTech Connect (OSTI)

    O'Brien, Nicholas

    2014-08-15

    The paper describes Soitecs project to plan,install,qualify and ramp a high volume CPV module manufactruing facility in Southern California. Soitec’s CPV module factory in San Diego was planned with an annual production capacity of 280MWDC. It was scheduled to be operational by the first quarter of 2013, and was expected to create several hundred direct and indirect jobs in the San Diego region. From ground breaking to facility readiness was completed in six months. This enabled the docking of equipment in the Q3’12 time frame. The first 140 MW of capacity was ready for operation in Q4’12. Production of the CX-M500 modules started in Q4 2012. The line yield and factory capacity were ramped in 2013. The annual production capacity demonstration was successfully completed in Q2 2014. The modules manufactured at the plant were used to supply utility scale demand in the US and also world markets.

  16. FY12 Quarter 3 Computing Utilization Report – LANL

    SciTech Connect (OSTI)

    Wampler, Cheryl L. [Los Alamos National Laboratory; McClellan, Laura Ann [Los Alamos National Laboratory

    2012-07-25

    DSW continues to dominate the capacity workload, with a focus in Q3 on common model baselining runs in preparation for the Annual Assessment Review (AAR) of the weapon systems. There remains unmet demand for higher fidelity simulations, and for increased throughput of simulations. Common model baselining activities would benefit from doubling the resolution of the models and running twice as many simulations. Capacity systems were also utilized during the quarter to prepare for upcoming Level 2 milestones. Other notable DSW activities include validation of new physics models and safety studies. The safety team used the capacity resources extensively for projects involving 3D computer simulations for the Furrow series of experiments at DARHT (a Level 2 milestone), fragment impact, surety theme, PANTEX assessments, and the 120-day study. With the more than tripling of classified capacity computing resources with the addition of the Luna system and the safety team's imminent access to the Cielo system, demand has been met for current needs. The safety team has performed successful scaling studies on Luna up to 16K PE size-jobs with linear scaling, running the large 3D simulations required for the analysis of Furrow. They will be investigating scaling studies on the Cielo system with the Lustre file system in Q4. Overall average capacity utilization was impacted by negative effects of the LANL Voluntary Separation Program (VSP) at the beginning of Q3, in which programmatic staffing was reduced by 6%, with further losses due to management backfills and attrition, resulting in about 10% fewer users. All classified systems were impacted in April by a planned 2 day red network outage. ASC capacity workload continues to focus on code development, regression testing, and verification and validation (V&V) studies. Significant capacity cycles were used in preparation for a JOWOG in May and several upcoming L2 milestones due in Q4. A network transition has been underway on the unclassified networks to increase access of all ASC users to the unclassified systems through the Yellow Turquoise Integration (YeTI) project. This will help to alleviate the longstanding shortage of resources for ASC unclassified code development and regression testing, and also make a broader palette of machines available to unclassified ASC users, including PSAAP Alliance users. The Moonlight system will be the first capacity resource to be made available through the YETI project, and will make available a significant increase in cycles, as well as GPGPU accelerator technology. The Turing and Lobo machines will be decommissioned in the next quarter. ASC projects running on Cielo as part of the CCC-3 include turbulence, hydrodynamics, burn, asteroids, polycrystals, capability and runtime performance improvements, and materials including carbon and silicone.

  17. Mechanism of runaway electron beam formation during plasma disruptions in tokamaks

    E-Print Network [OSTI]

    Abdullaev, S S; Wongrach, K; Tokar, M; Koslowski, H R; Willi, O; Zeng, L

    2015-01-01

    A new physical mechanism of the formation of runaway electron (RE) beams during plasma disruptions in tokamaks is proposed. The plasma disruption is caused by strong stochastic magnetic field formed due to nonlinearly excited low-mode number magnetohydrodynamic (MHD) modes. It is conjectured that the runaway electron beam is formed in the central plasma region confined inside the intact magnetic surface located between $q=1$ and the closest low--order rational magnetic surfaces [$q=3/2$, $q=4/3$, \\dots]. It results in that runaway electron beam current has a helical nature with a predominant $m/n=1/1$ component. The thermal quench and current decay times are estimated using the collisional models for electron diffusion and ambipolar particle transport in a stochastic magnetic field, respectively. Possible mechanisms of the decay of runaway electron current due to an outward drift electron orbits and resonance interaction of high--energy electrons with the $m/n=1/1$ MHD mode are discussed.

  18. Minimally non-local nucleon-nucleon potentials with chiral two-pion exchange including Delta resonances

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

    Piarulli, M; Girlanda, L; Schiavilla, R; Perez, R Navarro; Amaro, J E; Arriola, E Ruiz

    2015-02-01

    We construct a coordinate-space chiral potential, including ?-isobar intermediate states in its two-pion-exchange component up to order Q3 (Q denotes generically the low momentum scale).The contact interactions entering at next-to-leading and next-to-next-to-next-to-leading orders (Q2 and Q4, respectively) are rearranged by Fierz transformations to yield terms at most quadratic in the relative momentum operator of the two nucleons. The low-energy constant multiplying these contact interactions are fitted to the 2013 Granada database, consisting of 2309 pp and 2982 np data (including, respectively, 148 and 218 normalizations) in the laboratory-energy range 0--300 MeV. For the total 5291 $pp$ and $np$ data inmore »this range, we obtain a ?2 /datum of roughly 1.3 for a set of three models characterized by long- and short-range cutoffs, RL and RS respectively, ranging from (RL,RS)=(1.2,0.8) fm down to (0.8,0.6) fm. The long-range (short-range) cutoff regularizes the one- and two-pion exchange (contact) part of the potential.« less

  19. Mechanisms of plasma disruption and runaway electron losses in tokamaks

    E-Print Network [OSTI]

    Abdullaev, S S; Wongrach, K; Tokar, M; Koslowski, H R; Willi, O; Zeng, L

    2015-01-01

    Based on the analysis of data from the numerous dedicated experiments on plasma disruptions in the TEXTOR tokamak mechanisms of the formation of runaway electron beams and their losses are proposed. The plasma disruption is caused by strong stochastic magnetic field formed due to nonlinearly excited low-mode number MHD modes. It is hypothesized that the runaway electron beam is formed in the central plasma region confined inside the intact magnetic surface located between $q=1$ and the closest low--order rational [$q=4/3$ or $q=3/2$] magnetic surfaces. The thermal quench time caused by the fast electron transport in a stochastic magnetic field is calculated using the collisional transport model. The current decay stage is due to the ambipolar particle transport in a stochastic magnetic field. The runaway electron beam in the confined plasma region is formed due to their acceleration the inductive toroidal electric field. The runaway electron beam current is modeled as a sum of toroidally symmetric part and a ...

  20. Minimally nonlocal nucleon-nucleon potentials with chiral two-pion exchange including ? resonances

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

    Piarulli, M.; Girlanda, L.; Schiavilla, R.; Pérez, R. Navarro; Amaro, J. E.; Arriola, E. Ruiz

    2015-02-26

    In this study, we construct a coordinate-space chiral potential, including ?-isobar intermediate states in its two-pion-exchange component up to order Q3 (Q denotes generically the low momentum scale). The contact interactions entering at next-to-leading and next-to-next-to-next-to-leading orders (Q2 and Q4, respectively) are rearranged by Fierz transformations to yield terms at most quadratic in the relative momentum operator of the two nucleons. The low-energy constant multiplying these contact interactions are fitted to the 2013 Granada database, consisting of 2309 pp and 2982 np data (including, respectively, 148 and 218 normalizations) in the laboratory-energy range 0–300 MeV. For the total 5291 $pp$more »and $np$ data in this range, we obtain a ?2 /datum of roughly 1.3 for a set of three models characterized by long- and short-range cutoffs, RL and RS respectively, ranging from (RL,RS)=(1.2,0.8) fm down to (0.8,0.6) fm. The long-range (short-range) cutoff regularizes the one- and two-pion exchange (contact) part of the potential.« less

  1. 661PI?(SJV!I`l"d)03'8qlJOA'J~ll"%.398610OO'EOS61-66tOPo/98/f886-OPIO q3!q~u!`surs!u~q~aw`%up!Jdlods,uorCpua3aJauop

    E-Print Network [OSTI]

    Oren, Shmuel S.

    supply and demand (see Schweppe, Tabor and Kirtley C131). Incentive-based load management Differential of such pricing policies. Direct load management options. which allow an electric utility to curtail selectively capital cost. It is, therefore, beneficial to differentiate electric power service based on load

  2. Biochemical Platform Analysis Presentation for BETO 2015 Project...

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

    with NREL Catalytic Conversion of Sugars project - Q4 milestone * 2015 State of Technology assessment for FY15 R&D data - Q4 milestone * FY16 and beyond: TEA support for...

  3. Phonon-roton modes of liquid 4He beyond the roton in MCM-41

    SciTech Connect (OSTI)

    Azuah, Richard T NIST Center for Neutron Research , Gaithersburg, MD; Omar Diallo, Souleymane ORNL; Adams, Mark A. ISIS Facility, Rutherford Appleton Laboratory; Kirichek, Oleg ISIS Facility, Rutherford Appleton Laboratory; Glyde, Henry R University of Delaware

    2013-01-01

    We present neutron scattering measurements of the phonon-roton (P-R) mode of superfluid 4He confined in 47 A MCM-41 at T = 0.5 K at wave vectors, Q, beyond the roton wave vector (QR = 1.92 A-1). Measurements beyond the roton require access to high wave vectors (up to Q = 4 A-1) with excellent energy resolution and high statistical precision. The present results show for the first time that at T = 0.5 K the P-R mode in MCM-41 extends out to wave-vector Q 3.6 A-1 with the same energy and zero width (within precision) as observed in bulk superfluid 4He. Layer modes in the roton region are also observed. Specifically, the P-R mode energy, !Q, increases with Q for Q > QR and reaches a plateau at a maximum energy !Q = 2 where is the roton energy, = 0.74 0.01 meV in MCM-41. This upper limit means the P-R mode decays to two rotons when its energy exceeds 2 . It also means that the P-R mode does not decay to two layers modes. If the P-R could decay to two layer modes, !Q would plateau at a lower energy, !Q = 2 L where L = 0.60 meV is the energy of the roton like minimum of the layer mode. The observation of the P-R mode with energy up to 2 shows that the P-R mode and the layer modes are independent modes with apparently little interaction between them.

  4. Catalytic fast pyrolysis of lignocellulosic biomass

    SciTech Connect (OSTI)

    Liu, Changjun; Wang, Huamin; Karim, Ayman M.; Sun, Junming; Wang, Yong

    2014-11-21

    Increasing energy demand, especially in the transportation sector, and soaring CO2 emissions necessitate the exploitation of renewable sources of energy. Despite the large variety of new energy Q3 carriers, liquid hydrocarbon still appears to be the most attractive and feasible form of transportation fuel taking into account the energy density, stability and existing infrastructure. Biomass is an abundant, renewable source of energy; however, utilizing it in a cost-effective way is still a substantial challenge. Lignocellulose is composed of three major biopolymers, namely cellulose, hemicellulose and lignin. Fast pyrolysis of biomass is recognized as an efficient and feasible process to selectively convert lignocellulose into a liquid fuel—bio-oil. However bio-oil from fast pyrolysis contains a large amount of oxygen, distributed in hundreds of oxygenates. These oxygenates are the cause of many negative properties, such as low heating values, high corrosiveness, high viscosity, and instability; they also greatly Q4 limit the application of bio-oil particularly as transportation fuel. Hydrocarbons derived from biomass are most attractive because of their high energy density and compatibility with the existing infrastructure. Thus, converting lignocellulose into transportation fuels via catalytic fast pyrolysis has attracted much attention. Many studies related to catalytic fast pyrolysis of biomass have been published. The main challenge of this process is the development of active and stable catalysts that can deal with a large variety of decomposition intermediates from lignocellulose. This review starts with the current understanding of the chemistry in fast pyrolysis of lignocellulose and focuses on the development of catalysts in catalytic fast pyrolysis. Recent progress in the experimental studies on catalytic fast pyrolysis of biomass is also summarized with the emphasis on bio-oil yields and quality.

  5. Chromosome abnormalities in primary ovarian cancer

    SciTech Connect (OSTI)

    Yonescu, R.; Currie, J.; Griffin, C.A.

    1994-09-01

    Chromosome abnormalities that are specific and recurrent may occur in regions of the genome that are involved in the conversion of normal cells to those with tumorigenic potential. Ovarian cancer is the primary cause of death among patients with gynecological malignancies. We have performed cytogenetic analysis of 16 ovarian tumors from women age 28-82. Three tumors of low malignant potential and three granulosa cell tumors had normal karyotypes. To look for the presence of trisomy 12, which has been suggested to be a common aberration in this group of tumors, interphase fluorescence in situ hybridization was performed on direct preparations from three of these tumors using a probe for alpha satellite sequences of chromosome 12. In the 3 preparations, 92-98 percent of the cells contained two copies of chromosome 12, indicating that trisomy 12 is not a universal finding in low grade ovarian tumors. Endometrioid carcinoma of the ovary is histologically indistinguishable from endometial carcinoma of the uterus. We studied 10 endometrioid tumors to determine the degree of genetic similarity between these two carcinomas. Six out of ten endometrioid tumors showed a near-triploid modal number, and one presented with a tetraploid modal number. Eight of the ten contained structural chromosome abnormalities, of which the most frequent were 1p- (5 tumors), 19q+ (3 tumors), 6q- or ins(6) (4 tumors), 3q- or 3q+ (4 tumors). These cytogenetic results resemble those reported for papillary ovarian tumors and differ from those of endometrial carcinoma of the uterus. We conclude that despite the histologic similarities between the endometrioid and endometrial carcinomas, the genetic abnormalities in the genesis of these tumors differ significantly.

  6. Technology Performance Exchange

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

    Q3 Deliverable: Develop Site Workflows and Design Website Layout Q3 GoNo-Go DOE Decision Point: Passed Q1 Milestone: Develop Data Entry Forms Q2 Milestone: Release Technology...

  7. Purchase Obligations, Earnings Persistence and Stock Returns

    E-Print Network [OSTI]

    Lee, Kwang June

    2010-01-01

    inventory and raw materials Shipbuilding, Railroad EquipmentMean Median Q1 Q3 Min Max Shipbuilding, Railroad Equipment

  8. What Does a Scattering Pattern Tell US?

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

    Scattering Space sample light image Image Space lens Angular Space Q 4p sin(q) l Fourier Transform Scattering Pattern Fourier Transform Phase Problem Scattering Pattern...

  9. NNSA Corporate CPEP Process NNSA Honeywell FM&T PER NNSA/NA-00...

    National Nuclear Security Administration (NNSA)

    "meets expectations." Cyber Security - Honeywell's AOP metrics for Q4 and the year were Green, no issues. All AOP milestones were delivered on time. Cyber Security completed...

  10. SOUTHEAST REGIONAL CARBON SEQUESTRATION PARTNERSHIP (SECARB)

    SciTech Connect (OSTI)

    Kenneth J. Nemeth

    2004-09-01

    The Southeast Regional Carbon Sequestration Partnership (SECARB) is on schedule and within budget projections for the work completed during the first year of its two year program. Work during the semiannual period (third and fourth quarter) of the project (April 1--September 30, 2004) was conducted within a ''Task Responsibility Matrix.'' Under Task 1.0 Define Geographic Boundaries of the Region, Texas and Virginia were added during the second quarter of the project and no geographical changes occurred during the third or fourth quarter of the project. Under Task 2.0 Characterize the Region, general mapping and screening of sources and sinks has been completed, with integration and Geographical Information System (GIS) mapping ongoing. The first step focused on the macro level characterization of the region. Subsequent characterization will focus on smaller areas having high sequestration potential. Under Task 3.0 Identify and Address Issues for Technology Deployment, SECARB has completed a preliminary assessment of safety, regulatory, permitting, and accounting frameworks within the region to allow for wide-scale deployment of promising terrestrial and geologic sequestration approaches. Under Task 4.0 Develop Public Involvement and Education Mechanisms, SECARB has conducted a survey and focus group meeting to gain insight into approaches that will be taken to educate and involve the public. Task 5.0 and 6.0 will be implemented beginning October 1, 2004. Under Task 5.0 Identify the Most Promising Capture, Sequestration, and Transport Options, SECARB will evaluate findings from work performed during the first year and shift the focus of the project team from region-wide mapping and characterization to a more detailed screening approach designed to identify the most promising opportunities. Under Task 6.0 Prepare Action Plans for Implementation and Technology Validation Activity, the SECARB team will develop an integrated approach to implementing and setting up measurement, monitoring and verification (MMV) programs for the most promising opportunities. During this semiannual period special attention was provided to Texas and Virginia, which were added to the SECARB region, to ensure a smooth integration of activities with the other 9 states. Milestones completed and submitted during the third and fourth quarter included: Q3-FY04--Complete initial development of plans for GIS; and Q4-FYO4--Complete preliminary action plan and assessment for overcoming public perception issues.

  11. MEASURING THE ABUNDANCE OF SUB-KILOMETER-SIZED KUIPER BELT OBJECTS USING STELLAR OCCULTATIONS

    SciTech Connect (OSTI)

    Schlichting, Hilke E. [Department of Earth and Space Science, UCLA, 595 Charles East Young Drive East, Los Angeles, CA 90095 (United States); Ofek, Eran O.; Gal-Yam, Avishay [Faculty of Physics, Weizmann Institute of Science, P.O. Box 26, Rehovot 76100 (Israel); Sari, Re'em [Racah Institute of Physics, Hebrew University, Jerusalem 91904 (Israel); Nelan, Edmund P.; Livio, Mario [Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218 (United States); Wenz, Michael [Goddard Space Flight Center, 8800 Greenbelt Road, Greenbelt, MD 20771 (United States); Muirhead, Philip [Department of Astronomy, California Institute of Technology, MC 130-33, Pasadena, CA 91125 (United States); Javanfar, Nikta, E-mail: hilke@ucla.edu [Department of Physics, Physics Engineering and Astronomy, Queen's University, 99 University Avenue, Kingston, Ontario K7L 3N6 (Canada)

    2012-12-20

    We present here the analysis of about 19,500 new star hours of low ecliptic latitude observations (|b| {<=} 20 Degree-Sign ) obtained by the Hubble Space Telescope's Fine Guidance Sensors over a time span of more than nine years, which is in addition to the {approx}12, 000 star hours previously analyzed by Schlichting et al. Our search for stellar occultations by small Kuiper Belt Objects (KBOs) yielded one new candidate event corresponding to a body with a 530 {+-} 70 m radius at a distance of about 40 AU. Using bootstrap simulations, we estimate a probability of Almost-Equal-To 5% that this event is due to random statistical fluctuations within the new data set. Combining this new event with the single KBO occultation reported by Schlichting et al. we arrive at the following results: (1) the ecliptic latitudes of 6. Degree-Sign 6 and 14. Degree-Sign 4 of the two events are consistent with the observed inclination distribution of larger, 100-km-sized KBOs. (2) Assuming that small, sub-kilometer-sized KBOs have the same ecliptic latitude distribution as their larger counterparts, we find an ecliptic surface density of KBOs with radii larger than 250 m of N(r > 250 m) = 1.1{sup +1.5}{sub -0.7} Multiplication-Sign 10{sup 7} deg{sup -2}; if sub-kilometer-sized KBOs have instead a uniform ecliptic latitude distribution for -20 Degree-Sign < b < 20 Degree-Sign then N(r > 250 m) = 4.4{sup +5.8}{sub -2.8} Multiplication-Sign 10{sup 6} deg{sup -2}. This is the best measurement of the surface density of sub-kilometer-sized KBOs to date. (3) Assuming the KBO size distribution can be well described by a single power law given by N(> r){proportional_to}r{sup 1-q}, where N(> r) is the number of KBOs with radii greater than r, and q is the power-law index, we find q = 3.8 {+-} 0.2 and q = 3.6 {+-} 0.2 for a KBO ecliptic latitude distribution that follows the observed distribution for larger, 100-km-sized KBOs and a uniform KBO ecliptic latitude distribution for -20 Degree-Sign < b < 20 Degree-Sign , respectively. (4) Regardless of the exact power law, our results suggest that small KBOs are numerous enough to satisfy the required supply rate for the Jupiter family comets. (5) We can rule out a single power law below the break with q > 4.0 at 2{sigma}, confirming a strong deficit of sub-kilometer-sized KBOs compared to a population extrapolated from objects with r > 45 km. This suggests that small KBOs are undergoing collisional erosion and that the Kuiper Belt is a true analog to the dust producing debris disks observed around other stars.

  12. Report: Evaluating the Impact of Newer Researcher Training & Development: Which Direction Forward? (Report of a Joint Seminar)

    E-Print Network [OSTI]

    Gough, Martin

    2009-01-01

    , and a couple of feedback iterations. Q3a. Is this pass/fail distinction just appropriate for courses which contribute credits towards a qualification? Q3b. How can generic skills be assessed if not part of a wider/cohesive programme? - For those... contribute credits towards a qualification? Q3b. How can generic skills be assessed if not part of a wider/cohesive programme? ...

  13. The SEMATECH Berkeley MET: demonstration of 15-nm half-pitch in chemically amplified EUV resist and sensitivity of EUV resists at 6.x-nm

    E-Print Network [OSTI]

    Anderson, Christopher

    2013-01-01

    INTRODUCTION Phase shift mask (PSM) imaging enables pitchis suppressed. Pseudo PSM imaging enables pitch splittinga schematic of the pseudo PSM process. W = 9 '1-I C Q} 3

  14. 2010 Wind Technologies Market Report

    E-Print Network [OSTI]

    Wiser, Ryan

    2012-01-01

    1, 2011. Bloomberg New Energy Finance (Bloomberg NEF). 2011.2011. Bloomberg New Energy Finance (Bloomberg NEF). 2010. Q3Partnership for Renewable Energy Finance (US PREF). 2010.

  15. PowerPoint Presentation

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

    FY10 JFR activities in Q3 focused on data analysis and refurbishment of divertor heat flux instrumentation LH2 launcher installed and operational Progress thus far: * P...

  16. What Does a Scattering Pattern Tell US?

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

    amplitude e iwt Phase difference Phase difference S e i (ri Q) A(DK) fi A(Q) Fourier Transform ( ri ) DK Q 4p sin(q) l Lensless Imaging Sample Space Scattering Space...

  17. An Investigation into the Realities of a Quantum Datapath

    E-Print Network [OSTI]

    Isailovic, Nemanja

    2010-01-01

    Q0 being on the longest critical path, Q1 and Q4 on thequbit criticality or critical paths suffer from the drawbackdata. The bulk of the critical path involves independent

  18. Optimal Quantum Control Using Randomized Benchmarking R. Barends,1

    E-Print Network [OSTI]

    Martinis, John M.

    on subsequent gates, and identify control crosstalk in superconducting qubits. This method is able to correct). As a testbed, we use a five qubit (Q0-Q4) superconducting system [11] based on the Xmon transmon design [13

  19. High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles...

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

    2012. progressreportsunshotbraytonfy12q4.pdf More Documents & Publications High-Efficiency Low-Cost Solar Receiver for Use in a Supercritical CO2 Recompression Cycle - FY13 Q1...

  20. What Does a Scattering Pattern Tell US?

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

    light image Image Space lens Can we create the image without a lens? Angular Space Math Q 4p sin(q) l Lensless Imaging Sample Space Scattering Space sample light image lens...

  1. 4 Questions for a Better Buildings Case Competition Judge: Marc...

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

    more than ever, and fresh ideas can be the catalyst for new programs and success in our industry. Q4: Do you plan to participate in the next Better Buildings Case Competition?...

  2. Atmospheric Pressure Deposition for Electrochromic Windows

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

    and Charcaterize Performance FY12-Q4 Milestone: Demonstration Liquid Phase Spray for WO3 at 6" by 6" Current work and future research Work with Sage Electrochromics to Transfer...

  3. 3-point temperature anisotropies in WMAP: Limits on CMB non-Gaussianities and non-linearities

    E-Print Network [OSTI]

    E. Gaztanaga; J. Wagg

    2003-06-12

    We present a study of the 3-pt angular correlation function w_3= of (adimensional) temperature anisotropies measured by the Wilkinson Microwave Anisotropy Probe (WMAP). Results can be normalized to the 2-point function w_2 = in terms of the hierarchical: q_3 ~ w_3/w_2^2 or dimensionless: d_3 ~ w_2/w_2^{3/2}$ amplitudes. Strongly non-Gaussian models are generically expected to show d_3 > 1 or q_3 > 10^3 d_3. Unfortunately, this is comparable to the cosmic variance on large angular scales. For Gaussian primordial models, q_3 gives a direct measure of the non-linear corrections to temperature anisotropies in the sky: delta = delta_L + f_{NLT} (delta_L^2 - ) with f_{NLT} = q_3/2 for the leading order term in w_2^2. We find good agreement with the Gaussian hypothesis d_3 ~ 0 within the cosmic variance of LCDM simulations (with or without a low quadrupole). The strongest constraints on q_3 come from scales smaller than 1 degree. We find q_3 =19 +/-141 for (pseudo) collapsed configurations and an average of q_3 = 336 +/-218 for non-collapsed triangles. The corresponding non-linear coupling parameter, f_{NL}, for curvature perturbations Phi, in the Sachs-Wolfe (SW) regime is: f_{NL}^{SW} = q_3/6, while on degree scales, the extra power in acoustic oscillations produces f_{NL} ~ q_3/30 in the LCM model. Errors are dominated by cosmic variance, but for the first time they begin to be small enough to constrain the leading order non-linear effects with coupling of order unity.

  4. Annual Hanford Seismic Report for Fiscal Year 2010

    SciTech Connect (OSTI)

    Rohay, Alan C.; Clayton, Ray E.; Sweeney, Mark D.; Devary, Joseph L.; Hartshorn, Donald C.

    2010-12-27

    The Hanford Seismic Assessment Program (HSAP) provides an uninterrupted collection of high-quality raw and processed seismic data from the Hanford Seismic Network for the U.S. Department of Energy and its contractors. The HSAP is responsible for locating and identifying sources of seismic activity and monitoring changes in the historical pattern of seismic activity at the Hanford Site. The data are compiled, archived, and published for use by the Hanford Site for waste management, natural phenomena hazards assessments, and engineering design and construction. In addition, the HSAP works with the Hanford Site Emergency Services Organization to provide assistance in the event of a significant earthquake on the Hanford Site. The Hanford Seismic Network and the Eastern Washington Regional Network consist of 44 individual sensor sites and 15 radio relay sites maintained by the Hanford Seismic Assessment Team. During FY 2010, the Hanford Seismic Network recorded 873 triggers on the seismometer system, which included 259 seismic events in the southeast Washington area and an additional 324 regional and teleseismic events. There were 210 events determined to be local earthquakes relevant to the Hanford Site. One hundred and fifty-five earthquakes were detected in the vicinity of Wooded Island, located about eight miles north of Richland just west of the Columbia River. The Wooded Island events recorded this fiscal year were a continuation of the swarm events observed during fiscal year 2009 and reported in previous quarterly and annual reports (Rohay et al. 2009a, 2009b, 2009c, 2010a, 2010b, and 2010c). Most events were considered minor (coda-length magnitude [Mc] less than 1.0) with the largest event recorded on February 4, 2010 (3.0Mc). The estimated depths of the Wooded Island events are shallow (averaging approximately 1.5 km deep) placing the swarm within the Columbia River Basalt Group. Based upon the last two quarters (Q3 and Q4) data, activity at the Wooded Island area swarm has largely subsided. Pacific Northwest National Laboratory will continue to monitor for activity at this location. The highest-magnitude events (3.0Mc) were recorded on February 4, 2010 within the Wooded Island swarm (depth 2.4 km) and May 8, 2010 on or near the Saddle Mountain anticline (depth 3.0 km). This latter event is not considered unusual in that earthquakes have been previously recorded at this location, for example, in October 2006 (Rohay et al. 2007). With regard to the depth distribution, 173 earthquakes were located at shallow depths (less than 4 km, most likely in the Columbia River basalts), 18 earthquakes were located at intermediate depths (between 4 and 9 km, most likely in the pre-basalt sediments), and 19 earthquakes were located at depths greater than 9 km, within the crystalline basement. Geographically, 178 earthquakes were located in known swarm areas, 4 earthquakes occurred on or near a geologic structure (Saddle Mountain anticline), and 28 earthquakes were classified as random events. The Hanford Strong Motion Accelerometer (SMA) network was triggered several times by the Wooded Island swarm events and the events located on or near the Saddle Mountain anticline. The maximum acceleration value recorded by the SMA network during fiscal year 2010 occurred February 4, 2010 (Wooded Island swarm event), approximately 2 times lower than the reportable action level for Hanford facilities (2% g) with no action required.

  5. Abstract. In this paper, design and realization of a 4.5-5.8 GHz, Gm LC voltage controlled oscillator (VCO) for IEEE 802.11a

    E-Print Network [OSTI]

    Yanikoglu, Berrin

    . A well- designed VCO should send enough power to its output to drive the mixer and should dissipate), the LC tank (L and Cvar) and the buffer (Q3 and Q

  6. TheSNO+Experiment JeanneWilson,QMUL

    E-Print Network [OSTI]

    Agnor, Craig B.

    · Neutrinolessdoublebetadecayof150Nd · Reactorneutrinos · Geoneutrinos · Supernovaeneutrinos · Nucleondecay #12;Physicsgoals · Lowenergysolarneutrinos · Neutrinolessdoublebetadecayof150Nd · Reactorneutrinos · Geoneutrinos · Supernovaeneutrinos · Reactorneutrinos · Geoneutrinos · Supernovaeneutrinos · Nucleondecay #12;#12;Endpoint Energy Decay #12;· 150Nd ­Q=3

  7. State","Jan 2015","Feb 2015","Mar 2015","Q1 2015","Apr 2015"...

    U.S. Energy Information Administration (EIA) Indexed Site

    ,"Jul 2015","Aug 2015","Sep 2015","Q3 2015" "Alabama",1382932,1141885,1281975,3806792,1067587,1003155,958490,3029232,1120511,1210360,1145913,3476784 "Alaska",135396,111797,125356,3...

  8. High performance RF MEMS metal-contact switches and switching networks

    E-Print Network [OSTI]

    Patel, Chirag D.; Patel, Chirag D.

    2012-01-01

    A Compact Cantilever-Based RF MEMS Switch andA High-Performance RF MEMS Metal-Contact Switch and Switch-B High-Q 3-/4-Bit RF MEMS Digitally Tunable Capacitors for

  9. The SM8 Universal Solvation Model Christopher J. Cramer and Donald G. Truhlar, University of Minnesota

    E-Print Network [OSTI]

    Truhlar, Donald G

    constants, redox potentials, solubilities, temperature-dependent absolute free energies of solvation pollutants, and the thermodynamics of processes taking place in electrochemical fuel cells. q1 q2 q3 q2 q1 q

  10. Using Digital Elevation Data for Applications in Floodplain Mapping

    E-Print Network [OSTI]

    Kastens, Jude Heathcliff

    2007-11-14

    line work depicts FEMA Q3 100-year floodplain boundary for Shawnee County, Kansas. Floodplain Delineation Near-normal conditions (July 2000) 20-m Backfill Flood Zone map Cross-hatched area indicates FEMA Q3 100-year floodplain extent for Shawnee... County, Kansas. Flooded conditions (July 1993) Floodplain Delineation Channel Width Estimation Channel width was estimated from a Landsat scene depicting normal stream conditions. Width was estimated at 75 regularly spaced points along a nearly 20-km...

  11. Testing models of vacuum energy interacting with cold dark matter

    E-Print Network [OSTI]

    Li, Yun-He; Zhang, Xin

    2015-01-01

    We test the models of vacuum energy interacting with cold dark matter, and try to probe the possible deviation from the $\\Lambda$CDM model using current observations. We focus on two specific models, $Q=3\\beta H\\rho_{\\Lambda}$ and $Q=3\\beta H\\rho_c$. The data combinations come from the Planck 2013 data, the baryon acoustic oscillations measurements, the Type-Ia supernovae data, the Hubble constant measurement, the redshift space distortions data and the galaxy weak lensing data. For the $Q=3\\beta H\\rho_c$ model, we find that it can be tightly constrained by all the data combinations, while for the $Q=3\\beta H\\rho_{\\Lambda}$ model there still exist significant degeneracies between parameters. The tightest constraints for the coupling constant are $\\beta=-0.026^{+0.036}_{-0.053}$ (for $Q=3\\beta H\\rho_{\\Lambda}$) and $\\beta=-0.00045\\pm0.00069$ (for $Q=3\\beta H\\rho_c$) at $1\\sigma$ level. For all the fit results, we find that the null interaction $\\beta=0$ is always consistent with data. Our work completes the di...

  12. Quercetin 3-O-methyl ether protects FL83B cells from copper induced oxidative stress through the PI3K/Akt and MAPK/Erk pathway

    SciTech Connect (OSTI)

    Tseng, Hsiao-Ling, E-mail: lily1001224@gmail.com [Department of Life Sciences, Tzu Chi University, Hualien, Taiwan (China)] [Department of Life Sciences, Tzu Chi University, Hualien, Taiwan (China); Li, Chia-Jung, E-mail: 97751101@stmail.tcu.edu.tw [Institute of Medical Sciences, Tzu Chi University, Hualien, Taiwan (China)] [Institute of Medical Sciences, Tzu Chi University, Hualien, Taiwan (China); Huang, Lin-Huang, E-mail: yg1236@yahoo.com.tw [School of Medicine, Institute of Traditional Medicine, National Yang-Ming University, Taipei, Taiwan (China)] [School of Medicine, Institute of Traditional Medicine, National Yang-Ming University, Taipei, Taiwan (China); Chen, Chun-Yao, E-mail: cychen@mail.tcu.edu.tw [Department of Life Sciences, Tzu Chi University, Hualien, Taiwan (China)] [Department of Life Sciences, Tzu Chi University, Hualien, Taiwan (China); Tsai, Chun-Hao, E-mail: 100726105@stmail.tcu.edu.tw [Department of Life Sciences, Tzu Chi University, Hualien, Taiwan (China)] [Department of Life Sciences, Tzu Chi University, Hualien, Taiwan (China); Lin, Chun-Nan, E-mail: lincna@cc.kmu.edu.tw [Faculty of Pharmacy, College of Pharmacy, Kaohsiung Medical University, Kaohsiung, Taiwan (China) [Faculty of Pharmacy, College of Pharmacy, Kaohsiung Medical University, Kaohsiung, Taiwan (China); Department of Biological Science and Technology, School of Medicine, China Medical University, Taichung, Taiwan (China); Hsu, Hsue-Yin, E-mail: hsueyin@mail.tcu.edu.tw [Department of Life Sciences, Tzu Chi University, Hualien, Taiwan (China)] [Department of Life Sciences, Tzu Chi University, Hualien, Taiwan (China)

    2012-10-01

    Quercetin is a bioflavonoid that exhibits several biological functions in vitro and in vivo. Quercetin 3-O-methyl ether (Q3) is a natural product reported to have pharmaceutical activities, including antioxidative and anticancer activities. However, little is known about the mechanism by which it protects cells from oxidative stress. This study was designed to investigate the mechanisms by which Q3 protects against Cu{sup 2+}-induced cytotoxicity. Exposure to Cu{sup 2+} resulted in the death of mouse liver FL83B cells, characterized by apparent apoptotic features, including DNA fragmentation and increased nuclear condensation. Q3 markedly suppressed Cu{sup 2+}-induced apoptosis and mitochondrial dysfunction, characterized by reduced mitochondrial membrane potential, caspase-3 activation, and PARP cleavage, in Cu{sup 2+}-exposed cells. The involvement of PI3K, Akt, Erk, FOXO3A, and Mn-superoxide dismutase (MnSOD) was shown to be critical to the survival of Q3-treated FL83B cells. The liver of both larval and adult zebrafish showed severe damage after exposure to Cu{sup 2+} at a concentration of 5 ?M. Hepatic damage induced by Cu{sup 2+} was reduced by cotreatment with Q3. Survival of Cu{sup 2+}-exposed larval zebrafish was significantly increased by cotreatment with 15 ?M Q3. Our results indicated that Cu{sup 2+}-induced apoptosis in FL83B cells occurred via the generation of ROS, upregulation and phosphorylation of Erk, overexpression of 14-3-3, inactivation of Akt, and the downregulation of FOXO3A and MnSOD. Hence, these results also demonstrated that Q3 plays a protective role against oxidative damage in zebrafish liver and remarked the potential of Q3 to be used as an antioxidant for hepatocytes. Highlights: ? Protective effects of Q3 on Cu{sup 2+}-induced oxidative stress in vitro and in vivo. ? Cu{sup 2+} induced apoptosis in FL83B cells via ROS and the activation of Erk. ? Q3 abolishes Cu{sup 2+}-induced apoptosis through the PI3K/Akt and MAPK/Erk pathway.

  13. Next Generation DHCP Deployments

    E-Print Network [OSTI]

    Hull, Dave; Willard, George F. III

    2005-02-01

    Figure 9 ANSRdhcp request recording logic Figure 10 ANSR device entry Figure 11 DHCP snooping network topology Cisco Catalyst 2950G 48 C2950-I6K2L2Q4-M, Version 12.1(22)EA1 ip dhcp snooping vlan 123 ip dhcp snooping interface FastEthernet0... Figure 9 ANSRdhcp request recording logic Figure 10 ANSR device entry Figure 11 DHCP snooping network topology Cisco Catalyst 2950G 48 C2950-I6K2L2Q4-M, Version 12.1(22)EA1 ip dhcp snooping vlan 123 ip dhcp snooping interface FastEthernet0...

  14. Supplement of "Inversion of and emissions

    E-Print Network [OSTI]

    Meskhidze, Nicholas

    ppbv hydrogen £ ¡¥ : 311 ppbv nitrous oxide ¦§ ©¨ : 0.5 ppbv carbonyl sulfide ozone ¤ ¡¥ ©¡ hydrogen©¦ ¤ ¦ ¤ S ¤ ©¦ ¤ ¡%¦ ¤ Q©¦¢4¦ ¤ %$R¦ ¤ ©$ hydroxy carbonyls from ISOP Long-lived T 5 ¦!IU4¦ ¤ ¡¥QS¦ ¤ ¥¨ ¦ ¤ `$ dimethyl sulfide ¦§¨ ¡ carbon disulfide ¤ ¡¥¨ hydrogen sulfide 7 E $ oxygen atom (excited state

  15. JOURNAL DE PHYSIQUE CoZZoque C8, suppZ6ment au n08, Tome 41, aoGt 1980, page C8-163 STUDY OF LIQUID NICKEL-VANADIUM ALLOYS BY NEUTRON DIFFRACTION AND MODEL SIMULATION

    E-Print Network [OSTI]

    Boyer, Edmond

    , 28 i s the scattering angle, X the neutron wave- length, Q = 4n the modulus of the scattering vector NICKEL-VANADIUM ALLOYS BY NEUTRON DIFFRACTION AND MODEL SIMULATION J.L. Lemarchand, J. Bletry and P with model c a l c u l a t i o ~can lead to a quantitative interpreta- tion. In this paper, neutron

  16. NO. RIY. NO. TRANSMITTER DESIGN ANALYSIS ATM 897

    E-Print Network [OSTI]

    Rathbun, Julie A.

    NO. RIY. NO. TRANSMITTER DESIGN ANALYSIS ATM 897 PAGI 1 84 ( .e-,~·p·oe atam8 Dlvl8lon DATl! 7 - 6 TRANSMITTER DESIGN ANALYSIS PAGI 2 DATE 7-6-70 TABLE OF CONTENTS TRANSMITTER DESIGN ANALYSIS 1. INTRODUCTION AMPLIFIER 7. 4 Q4 OUTPUT NETWORK RE-CALCULATION 011 #12;TRANSMITTER DESIGN ANALYSIS ··-~·pace ltam8 Dlvlelon

  17. file://C:\\Documents%20and%20Settings\\VM3\\My%20Documents\\hc6-7a...

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

    Q 4.2 0.3 0.5 | 15.2 UnknownNo Answer... 7.1 0.7 1.0 0.6 0.2 | 14.0 | Air-Conditioning | | Central Air-Conditioning | Use a Central System... 58.6 1.3...

  18. Detailed Description of Key NIF Milestones for NNSA Description

    E-Print Network [OSTI]

    Operationally qualify ignition diagnostics [Neutron Activation Detector (Cooper), Magnetic Recoil Spectrometer ignition. Q4 FY2011 4073 Demonstrating we can light the "match" ­ alpha heating Conduct first DT implosion experimental campaign to demonstrate limited alpha heating Demonstrate cryogenic layered DT experiments

  19. Decomposing the Impact of Alternative Technology Sets on Future Carbon Emissions Growth1

    E-Print Network [OSTI]

    Wing, Ian Sue

    of carbon capture and storage, nuclear, and hydroelectric generation all lead to upward shifts in the long are the drivers of future global carbon dioxide (CO2) emissions growth and how would the availability of key Classification: D58, Q4, Q54, O1, Keywords: Asia, energy use, carbon emissions, global climate change, computable

  20. A.G.Ramm, Inverse scattering problem with data at fixed energy and fixed incident direction, Nonlinear Analysis: Theory, methods and Applications, 69, N4, (2008), 1478

    E-Print Network [OSTI]

    2008-01-01

    scattering problem with fixed­energy data consists in finding a potential q(x) from the knowledge of A q ([4]), who also gave a method for recovery of q from the exact fixed­energy data, an error estimate of q from noisy fixed­energy data, and an error estimate for this method [5], [6], [7]. Until now

  1. 7-135 A Carnot refrigeration cycle is executed in a closed system with a fixed mass of R-134a. The net work input and the maximum and minimum temperatures are given. The mass fraction of the refrigerant

    E-Print Network [OSTI]

    Bahrami, Majid

    7-61 7-135 A Carnot refrigeration cycle is executed in a closed system with a fixed mass of R-134aJ/kg (Table A-12). Analysis The coefficient of performance of the cycle is T v 20q 4 3 1 2 QH QL -8qC and #12

  2. Pion photo- and electroproduction in relativistic baryon ChPT

    E-Print Network [OSTI]

    Lothar Tiator; Stefan Scherer; Marius Hilt

    2014-02-04

    We present a calculation of pion photo- and electroproduction in manifestly Lorentz-invariant baryon chiral perturbation theory up to and including order q^4. We fix the low-energy constants by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID.

  3. Renewable Energy Finance Tracking Initiative (REFTI): Snapshot of Recent Geothermal Financing Terms, Fourth Quarter 2009 - Second Half 2011

    SciTech Connect (OSTI)

    Lowder, T.; Hubbell, R.; Mendelsohn, M.; Cory, K.

    2012-09-01

    This report is a review of geothermal project financial terms as reported in the National Renewable Energy Laboratory's Renewable Energy Finance Tracking Initiative (REFTI). The data were collected over seven analysis periods from the fourth quarter (Q4) of 2009 to the second half (2H) of 2011.

  4. Secondary constructions on generalized bent functions Brajesh Kumar Singh

    E-Print Network [OSTI]

    International Association for Cryptologic Research (IACR)

    Secondary constructions on generalized bent functions Brajesh Kumar Singh Department of Mathematics of Maiorana-McFarland class of bent functions, for Research supported by CSIR, INDIA. #12;2 B. K. Singh q = 4. Recently, Stanica, Gangopadhyay and Singh [13] studied several proper- ties generalized bent Boolean

  5. TIMES model for the Reunion Island: addressing reliability of electricity supply

    E-Print Network [OSTI]

    Paris-Sud XI, Université de

    energy sources. In 2008, the total primary energy consumption was 1295 ktoe, and as most of small islands% on renewable energy sources [1]. In 2008, the total primary energy consumption was 1295 ktoe, and as most. Keywords: Long-term energy planning. Reunion Island. Reliability of electricity supply. JEL: ­ Q4; O21; Q29

  6. Proposed Scope and Schedule for Scenario and

    E-Print Network [OSTI]

    conservation and demand response development. Sensitivity S2 ­ Scenarios 1B and 2C w/Lower Natural Gas Prices on resource development of significantly lower natural gas prices. Sensitivity S3 ­ Scenarios 1B and 2C w and chapters. 2 #12;2014 Q4 Q1 2015 Q2 2015 Demand/Price Forecasts Updated Methodology for Quantification

  7. Distributed seeding for narrow-line width hard x-ray free-electron lasers

    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:Speeding accessby aLED Street Lighting Host Site: City ofNovelQ3:Q3:

  8. Violence, Intimacy, and Vulnerability: Marriage and the Risk of HIV Infection Among Women in South India

    E-Print Network [OSTI]

    Vedanthan, Rajesh

    2000-01-01

    oo 23:52 A b?nmuz?ocuo A aosmuomoc om: Eocnou m.9o8 wEo==8=oo 33 um: wEo =ouoo. =: Q: 3 8o _o. :=oo c8_E§ A So u o oo

  9. the Next Step for FE in China beyond ITER 10 -11 Dec.2013 Washington DC

    E-Print Network [OSTI]

    -sustained with TBR 1.2 Relay on existing ITER physicalk~1. 8-2, q > 3, H~1) and technical bases The goal of our design is to try to build the engineering testing reactor for fusion energy as early. CFETR will be one of the best test facility to develop the suitable materials for DEMO or FPP under

  10. Chapter 3 x Integral Relations for a Control Volume 249 3.114 The 3-arm lawn sprinkler of

    E-Print Network [OSTI]

    Bahrami, Majid

    Chapter 3 x Integral Relations for a Control Volume 249 3.114 The 3-arm lawn sprinkler of Fig. P3 rotation rate in rev/min for (a) T 0°; (b) T 40°? Solution: The velocity exiting each arm is o 2 2 Q/3 2

  11. "Table HC12.11 Home Electronics Characteristics by Midwest Census...

    U.S. Energy Information Administration (EIA) Indexed Site

    "1.",26.3,5.8,4.3,1.5 "2.",3.6,0.9,0.6,"Q" "3 or More",0.6,"Q","Q","Q" "Plasma Television Sets",3.6,0.7,0.6,"Q" "1.",2.7,0.6,0.5,"Q" "2 or More",0.9,"Q","Q","Q"...

  12. " Million U.S. Housing Units"

    U.S. Energy Information Administration (EIA) Indexed Site

    "2.",3.6,2.9,0.2,"Q",0.2,"Q" "3 or More",0.6,0.4,"Q","N","Q","N" "Plasma Television Sets",3.6,2.6,0.3,"Q",0.4,"Q" "1.",2.7,2.1,0.2,"Q","Q","Q" "2 or...

  13. "Table HC3.11 Home Electronics Characteristics by Owner-Occupied...

    U.S. Energy Information Administration (EIA) Indexed Site

    "2.",3.6,3,2.6,"Q","Q","Q","Q" "3 or More",0.6,0.5,0.4,"Q","N","Q","N" "Plasma Television Sets",3.6,2.8,2.2,"Q","Q","Q","Q" "1.",2.7,2.1,1.8,"Q","Q","Q","N" "2 or...

  14. "Table HC4.11 Home Electronics Characteristics by Renter-Occupied...

    U.S. Energy Information Administration (EIA) Indexed Site

    "2.",3.6,0.7,0.3,"Q","Q",0.2,"Q" "3 or More",0.6,"Q","N","N","N","Q","N" "Plasma Television Sets",3.6,0.8,0.4,"Q","Q",0.3,"Q" "1.",2.7,0.6,0.2,"Q","Q","Q","Q" "2 or...

  15. "Table HC11.11 Home Electronics Characteristics by Northeast...

    U.S. Energy Information Administration (EIA) Indexed Site

    "1.",26.3,4,3,1.1 "2.",3.6,0.6,0.5,"Q" "3 or More",0.6,"Q","Q","N" "Plasma Television Sets",3.6,0.7,0.5,0.2 "1.",2.7,0.5,0.3,"Q" "2 or More",0.9,0.2,"Q","Q"...

  16. Targeting X Repression: Recruitment, Binding and Function of the C. elegans Dosage Compensation Complex

    E-Print Network [OSTI]

    Pferdehirt, Rebecca Ruth

    2011-01-01

    +689! 69! ,! )B06;69MC0+,! G=+,9+! G8=;03! Immunology! 125I!0+! ,B3! 455V3! (! ;0X=0910! G8+6:! Y6+*69! 1*-8G,+69! 09+-O=11*0;6! Q&3! ]ZZL3! G8:. ! ,! <=+,+670! ,10+AB! +-,9;:0-,;

  17. Deutsche Telekom to offer Microsoft Office on a monthly payment plan Jun 11, 2009

    E-Print Network [OSTI]

    Deutschmann, Rainer

    Deutsche Telekom to offer Microsoft Office on a monthly payment plan Jun 11, 2009 · Customers able · Offer available first to T-Mobile Austria mobile broadband customers and Deutsche Telekom business customers in Germany from Q3 2009 · Deutsche Telekom is the first telecommunications provider to offer

  18. Art, Spirituality, and the Ethic of Care: Alternative Masculinities in Chinese American Literature

    E-Print Network [OSTI]

    Cheung, KK

    2015-01-01

    om mo- mm? 3 wmoomEHrm sw?mnoh 883%». owe rum .8mom :§§ ::. =o:. _wHrm Sonar B983 rm Baum? nro no3.5m mnrors Q§.Q_. = 3.5 Hrm Boa mm- Boom oaaoa mxa?mmmm.

  19. Available

    E-Print Network [OSTI]

    2015-01-25

    Feb 12, 2014 ... B. ?2,?1, 2. 3. ? C. ?34. 13. ,0, 51. 13. ? (correct). D. ? 4. 13. ,? 1. 13 ... Find the area of the triangle with vertices P(1,?1,0),Q(3,?2,2) and R(2,?2 ...

  20. GJI gji_4751 Dispatch: August 12, 2010 CE: VBF Journal MSP No. No. of pages: 14 PE: JM

    E-Print Network [OSTI]

    41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 Geophys. J. Int. (2010) doi Key words: ???. Q3 1 I N T RO D U C T I O N Induced polarization represents the measurement

  1. J. Am. Chem. SOC.1994,116, 11151-11152 11151 Evidence for a Cyclic Mechanism in

    E-Print Network [OSTI]

    Keinan, Ehud

    J. Am. Chem. SOC.1994,116, 11151-11152 11151 Evidence for a Cyclic Mechanism in (q3-Al. TetrahedronLett. 1978,2075. (b)Trost, B. M.; Verhoeven,T. R.; Fortunak,J. M. Tetrahedron Lett. 1979, 2301. (c

  2. A System Call-Centric Analysis and Stimulation Technique to Automatically Reconstruct Android Malware Behaviors

    E-Print Network [OSTI]

    Cavallaro, Lorenzo

    A System Call-Centric Analysis and Stimulation Technique to Automatically Reconstruct Android.cavallaro@rhul.ac.uk ABSTRACT With more than 500 million of activations reported in Q3 2012, Android mobile devices are becoming soon attracted the interests of cyber- criminals too with malware now hitting Android devices

  3. Universality and criticality of a second-order granular solid-liquid-like phase transition

    E-Print Network [OSTI]

    Gustavo Castillo; Nicolás Mujica; Rodrigo Soto

    2015-01-20

    We experimentally study the critical properties of the non-equilibrium solid-liquid-like transition that takes place in vibrated granular matter. The critical dynamics is characterized by the coupling of the density field with the bond-orientational order parameter $Q_4$, which measures the degree of local crystallization. Two setups are compared, which present the transition at different critical accelerations as a a result of modifying the energy dissipation parameters. In both setups five independent critical exponents are measured, associated to different properties of $Q_4$: the correlation length, relaxation time, vanishing wavenumber limit (static susceptibility), the hydrodynamic regime of the pair correlation function, and the amplitude of the order parameter. The respective critical exponents agree in both setups and are given by $\

  4. A study of the middle Dutch poem, Van den vos Reynaerde and its sources in the branches of the old French Roman de Renard

    E-Print Network [OSTI]

    Appelboom, Peter Anton Frederik

    1917-01-01

    col. R. v.1199 Want eer hyt wiste, was hem een strec Omme sinesi bale arde vast.'** 41 R#R# v. BEG Con plus tret, plus eatrcint li las R. v.l£Q4 Rr.de sprang voert; dat strec liep toe R#R« v.860 Qar Martinez li clercono saut 'Or cug> or bug' fet... col. R. v.1199 Want eer hyt wiste, was hem een strec Omme sinesi bale arde vast.'** 41 R#R# v. BEG Con plus tret, plus eatrcint li las R. v.l£Q4 Rr.de sprang voert; dat strec liep toe R#R« v.860 Qar Martinez li clercono saut 'Or cug> or bug' fet...

  5. The influence of temperatures and mechanical treatments on pre- and post-emergence growth of peach and plum seedlings 

    E-Print Network [OSTI]

    Alsalih, Kamil Khidher

    1961-01-01

    , the possibility of variation between speoies SCAPI ICI ~ ~ IA NI A ~ ~ ~ 0 0 0 ~ ~ O IO Ch 33m R R CII CII CII ~ ~ A 4 SI S 0 0 0 '4l Q 4l Q s CII r 0 O ~ ~ as ~8 ~gA ICI IO 0 N Ill OE 0 CIA CIN Ch CO ~ ~ ~ t N ~ ~ 0 CCI ICI 0 0 0...W goeio4 oo ~. f As ooe ~ oero. eheea&eriheIL Q aeero%o areae ia i' piIaoale. Q4e oeaooivagg coal, 4 have hoea oaaee4 Q %he high O~erafeee, '()IIkaeee 4; ea4 0)? . gheee eee4lxlwge 4L4 aos groo ee sapL41p ehoa tirei Osaaeferro4 4e ~ gro hoaa? ?e 4L4...

  6. Power Corrections and Renormalons in Deep Inelastic Structure Functions

    E-Print Network [OSTI]

    M. Dasgupta; B. R. Webber

    1996-04-23

    We study the power corrections (infrared renormalon contributions) to the coefficient functions for non-singlet deep inelastic structure functions due to gluon vacuum polarization insertions in one-loop graphs. Remarkably, for all the structure functions $F_1$, $F_2$, $F_3$ and $g_1$, there are only two such contributions, corresponding to $1/Q^2$ and $1/Q^4$ power corrections. We compute their dependence on Bjorken $x$. The results could be used to model the dominant higher-twist contributions.

  7. Pion Photo- and Electroproduction and the Chiral MAID Interface

    E-Print Network [OSTI]

    Hilt, M; Scherer, S; Tiator, L

    2015-01-01

    We discuss the extended on-mass-shell scheme for manifestly Lorentz-invariant baryon chiral perturbation theory. We present a calculation of pion photo- and electroproduction up to and including order $q^4$. The low-energy constants have been fixed by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID (http://www.kph.uni-mainz.de/MAID/chiralmaid/).

  8. MIE 230-Thermodynamics Professor Rothstein

    E-Print Network [OSTI]

    Rothstein, Jonathan

    below. Steam enters the turbine at p1 = 10MPa and T1=640 C and exits at p2=50kPa. Steam leaves Steam Generator 2 3 1 Turbine Condenser Pump p2 = 50kPa p3 = 50kPa sat. liquid . Q4-1 = 200 MW T1 = 640 the steam power plant shown in the figure below. The cycle requires 150MWinQ of heat to operate as shown

  9. Pion Photo- and Electroproduction and the Chiral MAID Interface

    E-Print Network [OSTI]

    M. Hilt; B. C. Lehnhart; S. Scherer; L. Tiator

    2015-10-15

    We discuss the extended on-mass-shell scheme for manifestly Lorentz-invariant baryon chiral perturbation theory. We present a calculation of pion photo- and electroproduction up to and including order $q^4$. The low-energy constants have been fixed by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID (http://www.kph.uni-mainz.de/MAID/chiralmaid/).

  10. Pion photo- and electroproduction with chiral MAID

    E-Print Network [OSTI]

    M. Hilt; B. C. Lehnhart; S. Scherer; L. Tiator

    2013-09-13

    We present a calculation of pion photo- and electroproduction in manifestly Lorentz-invariant baryon chiral perturbation theory up to and including order $q^4$. We fix the low-energy constants by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID. We explain how our program works and how it can be used for further analysis.

  11. hepph/9512272 ON THE THEORETICAL STATUS OF

    E-Print Network [OSTI]

    (š)N scattering processes are described by six further structure functions W š;\\Sigma 2 , xW š;\\Sigma 3 , F 2Z structure at short distances. Since both charged leptons (e \\Sigma ; ¯ \\Sigma ) and neutrinos (š; š) may ) collects couplings and propagator terms, e.g. P l \\Sigma ;fl (Q 2 ) = 2�ff 2 =Q 4 , P š;W +(Q 2 ) = G 2 F M

  12. Adequacy of milk manufacturing plants in the North Texas marketing area to handle surplus milk, 1953-54 

    E-Print Network [OSTI]

    Humphrey, Mabern David

    1954-01-01

    S St e S lek" Fer Cent de Pe Cent 63 Axe kdgh school Vmaatt + k farsssr lo olcuooo ao Oavlois a cist~- ~ ools & he rayortsso A. vo or vore sLslk corn. lj / e4~a isis ruhr& 5l 4~i' k MLcLX tftu4 4jMZi Q4 ~i 'iisV ~ sX GOiL4l'~~ ~'1'X. % Ftc...

  13. Making a virtue out of virtual communities: working electronically with an advisory panel of library users

    E-Print Network [OSTI]

    Collins, Anne; Kuhn, Isla; Morgan, Peter

    that the Panel's eventual membership provided, as far as possible, a balanced reflection of our actual registered client base.) Launching the Panel The initial invitation (which was reissued after about three weeks) ran for six weeks to the end... we should conduct a comprehensive stock check, proposing some possible options such as closing completely for a week, or a number of less drastic but more complex alternatives. • Q.4 - we listed a range of social networking technologies (FaceBook...

  14. Factors influencing the growth of Sclerotium rolfsii in various soils 

    E-Print Network [OSTI]

    Menon, Sankara Kochukrishna

    1953-01-01

    ~ hssishanh taefossox of hho loyarhasah of Plant Sqrsiahogf ael Pnthologye 'glhRS 4 05ICSN%. XgSSII00%4 4 ~ t ~ 4 g 4 4 4 4+ ~ ~ 0 ~ 4 ~ ~ 1 I t 4* ~ +t gggS4F Q%%4%$$ O. 0 0 ~ 4 0 4 4 ~ ~ f 4 % ~ ~ 1 4'1 0 II 856% 4NP %@IIX@) 's ~ ~ ~ s a e'e ~ i o + t a...

  15. Selected non-holonomic functions in lattice statistical mechanics and enumerative combinatorics

    E-Print Network [OSTI]

    S. Boukraa; J-M. Maillard

    2015-10-15

    We recall that the full susceptibility series of the Ising model, modulo powers of the prime 2, reduce to algebraic functions. We also recall the non-linear polynomial differential equation obtained by Tutte for the generating function of the q-coloured rooted triangulations by vertices, which is known to have algebraic solutions for all the numbers of the form $2 +2 \\cos(j\\pi/n)$, the status of the q= 4 being unclear. We focus on the analysis of the q= 4 case, showing that the corresponding series is quite certainly non-holonomic. Along the line of a previous work on the susceptibility of the Ising model, we consider this q=4 series modulo the first eight primes 2, 3, ... 19, and show that this (probably non-holonomic) function reduces, modulo these primes, to algebraic functions. We conjecture that this probably non-holonomic function reduces to algebraic functions modulo (almost) every prime, or power of prime numbers. This raises the question to see whether such remarkable non-holonomic functions can be seen as ratio of diagonals of rational functions, or even rational, or algebraic, functions of diagonals of rational functions.

  16. High-p(T) pi(0) production with respect to the reaction plane in Au plus Au collisions at s(NN)=200 GeV 

    E-Print Network [OSTI]

    Afanasiev, S.; Aidala, C.; Ajitanand, N. N.; Akiba, Y.; Alexander, J.; Al-Jamel, A.; Aoki, K.; Aphecetche, L.; Armendariz, R.; Aronson, S. H.; Averbeck, R.; Awes, T. C.; Azmoun, B.; Babintsev, V.; Baldisseri, A.; Barish, K. N.; Barnes, P. D.; Bassalleck, B.; Bathe, S.; Batsouli, S.; Baublis, V.; Bauer, F.; Bazilevsky, A.; Belikov, S.; Bennett, R.; Berdnikov, Y.; Bjorndal, M. T.; Boissevain, J. G.; Borel, H.; Boyle, K.; Brooks, M. L.; Brown, D. S.; Bucher, D.; Buesching, H.; Bumazhnov, V.; Bunce, G.; Burward-Hoy, J. M.; Butsyk, S.; Campbell, S.; Chai, J. -S; Chernichenko, S.; Chiba, J.; Chi, C. Y.; Chiu, M.; Choi, I. J.; Chujo, T.; Cianciolo, V.; Cleven, C. R.; Cobigo, Y.; Cole, B. A.; Comets, M. P.; Constantin, P.; Csanad, M.; Csorgo, T.; Dahms, T.; Das, K.; David, G.; Delagrange, H.; Denisov, A.; d'Enterria, D.; Deshpande, A.; Desmond, E. J.; Dietzsch, O.; Dion, A.; Drachenberg, J. L.; Drapier, O.; Drees, A.; Dubey, A. K.; Durum, A.; Dzhordzhadze, V.; Efremenko, Y. V.; Egdemir, J.; Enokizono, A.; En'yo, H.; Espagnon, B.; Esumi, S.; Fields, D. E.; Fleuret, F.; Fokin, S. L.; Forestier, B.; Fraenkel, Z.; Frantz, J. E.; Franz, A.; Frawley, A. D.; Fukao, Y.; Fung, S. -Y; Gadrat, S.; Gastineau, F.; Germain, M.; Glenn, A.; Gonin, M.; Gosset, J.; Goto, Y.; de Cassagnac, R. Granier; Grau, N.; Greene, S. V.; Perdekamp, M. Grosse; Gunji, T.; Gustafsson, H. A.; Hachiya, T.; Henni, A. Hadj; Haggerty, J. S.; Hagiwara, M. N.; Hamagaki, H.; Harada, H.; Hartouni, E. P.; Haruna, K.; Harvey, M.; Haslum, E.; Hasuko, K.; Hayano, R.; Heffner, M.; Hemmick, T. K.; Heuser, J. M.; He, X.; Hiejima, H.; Hill, J. C.; Hobbs, R.; Holmes, M.; Holzmann, W.; Homma, K.; Hong, B.; Horaguchi, T.; Hur, M. G.; Ichihara, T.; Imai, K.; Inaba, M.; Isenhower, D.; Isenhower, L.; Ishihara, M.; Isobe, T.; Issah, M.; Isupov, A.; Jacak, B. V.; Jia, J.; Jin, J.; Jinnouchi, O.; Johnson, B. M.; Joo, K. S.; Jouan, D.; Kajihara, F.; Kametani, S.; Kamihara, N.; Kaneta, M.; Kang, J. H.; Kawagishi, T.; Kazantsev, A. V.; Kelly, S.; Khanzadeev, A.; Kim, D. J.; Kim, E.; Kim, Y. -S; Kinney, E.; Kiss, A.; Kistenev, E.; Kiyomichi, A.; Klein-Boesing, C.; Kochenda, L.; Kochetkov, V.; Komkov, B.; Konno, M.; Kotchetkov, D.; Kozlov, A.; Kroon, P. J.; Kunde, G. J.; Kurihara, N.; Kurita, K.; Kweon, M. J.; Kwon, Y.; Kyle, G. S.; Lacey, R.; Lajoie, J. G.; Lebedev, A.; Le Bornec, Y.; Leckey, S.; Lee, D. M.; Lee, M. K.; Leitch, M. J.; Leite, M. A. L.; Lim, H.; Litvinenko, A.; Liu, M. X.; Li, X. H.; Maguire, C. F.; Makdisi, Y. I.; Malakhov, A.; Malik, M. D.; Manko, V. I.; Masui, H.; Matathias, F.; McCain, M. C.; McGaughey, P. L.; Miake, Y.; Miller, T. E.; Milov, A.; Mioduszewski, Saskia; Mishra, G. C.; Mitchell, J. T.; Morrison, D. P.; Moss, J. M.; Moukhanova, T. V.; Mukhopadhyay, D.; Murata, J.; Nagamiya, S.; Nagata, Y.; Nagle, J. L.; Naglis, M.; Nakamura, T.; Newby, J.; Nguyen, M.; Norman, B. E.; Nyanin, A. S.; Nystrand, J.; O'Brien, E.; Ogilvie, C. A.; Ohnishi, H.; Ojha, I. D.; Okada, H.; Okada, K.; Omiwade, O. O.; Oskarsson, A.; Otterlund, I.; Ozawa, K.; Pal, D.; Palounek, A. P. T.; Pantuev, V.; Papavassiliou, V.; Park, J.; Park, W. J.; Pate, S. F.; Pei, H.; Peng, J. -C; Pereira, H.; Peresedov, V.; Peressounko, D. Yu; Pinkenburg, C.; Pisani, R. P.; Purschke, M. L.; Purwar, A. K.; Qu, H.; Rak, J.; Ravinovich, I.; Read, K. F.; Reuter, M.; Reygers, K.; Riabov, V.; Riabov, Y.; Roche, G.; Romana, A.; Rosati, M.; Rosendahl, S. S. E.; Rosnet, P.; Rukoyatkin, P.; Rykov, V. L.; Ryu, S. S.; Sahlmueller, B.; Saito, N.; Sakaguchi, T.; Sakai, S.; Samsonov, V.; Sato, H. D.; Sato, S.; Sawada, S.; Semenov, V.; Seto, R.; Sharma, D.; Shea, T. K.; Shein, I.; Shibata, T. -A; Shigaki, K.; Shimomura, M.; Shohjoh, T.; Shoji, K.; Sickles, A.; Silva, C. L.; Silvermyr, D.; Sim, K. S.; Singh, C. P.; Singh, V.; Skutnik, S.; Smith, W. C.; Soldatov, A.; Soltz, R. A.; Sondheim, W. E.; Sorensen, S. P.; Sourikova, I. V.; Staley, F.; Stankus, P. W.; Stenlund, E.; Stepanov, M.; Ster, A.; Stoll, S. P.; Sugitate, T.; Suire, C.; Sullivan, J. P.; Sziklai, J.; Tabaru, T.; Takagi, S.; Takagui, E. M.; Taketani, A.; Tanaka, K. H.; Tanaka, Y.; Tanida, K.; Tannenbaum, M. J.; Taranenko, A.; Tarjan, P.; Thomas, T. L.; Togawa, M.; Tojo, J.; Torii, H.; Towell, R. S.; Tram, V. -N; Tserruya, I.; Tsuchimoto, Y.; Tuli, S. K.; Tydesjo, H.; Tyurin, N.; Vale, C.; Valle, H.; van Hecke, H. W.; Velkovska, J.; Vertesi, R.; Vinogradov, A. A.; Vznuzdaev, E.; Wagner, M.; Wang, X. R.; Watanabe, Y.; Wessels, J.; White, S. N.; Willis, N.; Winter, D.; Woody, C. L.; Wysocki, M.; Xie, W.; Yanovich, A.; Yokkaichi, S.; Young, G. R.; Younus, I.; Yushmanov, I. E.; Zajc, W. A.; Zaudtke, O.; Zhang, C.; Zimanyi, J.; Zolin, L.; PHENIX Collaboration.

    2009-01-01

    library l i b rayy?hyI a? OQItj'Q4'4g68 nS (g??g'M y'AQ,8w, Q4g'? 5u?5...g??M ,84 6 5 49, Q,EugQ,M,84s 56Q 49, 1,CQ,, 6 5 ?arOaT a? eopyaQ4'4g68 nS (g??g'M y'AQ,8w,

  17. Weak-Coupling Model for Pb-212 and Pb-204 

    E-Print Network [OSTI]

    Ko, Che Ming; Kuo, T. T. S.; McGrory, J. B.

    1973-01-01

    g??M ,84 6 5 49, Q,EugQ,M,84s 56Q 49, 1,CQ,, 6 5 ?arOaT a? eopyaQ4'4g68 nS (g??g'M y'AQ,8w, Q4M,84 6Q <4u1,84 l1?gs6Q? b'S x_HH x ? pPOTa?mrOpaP ? ? T.?p.( a? Oo. ypO.TlOmT. ?? PlOmTly arrmTT.Pr.< a? Oo. ?p<.l<. ? ? .?e.Tpb.POly eTa?mrOpaP a? Oo. ?p<.l<. H? op

  18. The transfer of heat and mass to a vertical plate under frosting conditions 

    E-Print Network [OSTI]

    Poth, Louis Joseph

    1960-01-01

    "7~ Excluding the latent heat transfer (26. & Stu/hr) the overall coefficient of heat transfer So le + 19+2 linea/IK' apeak 21 ajjjt~~ oa, oat%, asa '%, wa 1 - l. eS e. B 8. 4 ey. o aN. 4 aa. o 6$. $2 00 ~ 26. 0 1. 99 2, 18 2 $Q $3 ao 6 33 0 96i9 9i4 6$ea...

  19. Monthly energy review, May 1995

    SciTech Connect (OSTI)

    1995-05-24

    Energy production during Feb 95 totaled 5.4 quadrillion Btu (Q), 3.1% over Feb 94. Energy consumption totaled 7.4 Q, 0.7% below Feb 94. Net imports of energy totaled 1.3 Q, 5.6% below Feb 94. This publication is divided into energy overview, energy consumption, petroleum, natural gas, oil and gas resource development, coal, electricity, nuclear energy, energy prices, and international energy.

  20. E3 : Mathematical Programming H 2010 Problem Set 1 Introduction and Simplex Method

    E-Print Network [OSTI]

    . Q5 A gasoline refinery has two types of crude oil, A and B, which may be used to produce fuel oil function value.] Q3 A manufacturer has stocks of three factors A, B and C and also hires labour from factor B 3 5 4 2 C 2 1 1 0 The stocks available of the three factors are 25, 11, 2 respectively

  1. Asymmetric rotor analysis of DSOD spectra up to the r

    E-Print Network [OSTI]

    Giesen, Thomas

    West, Onagawa l6-1, Tsukuba 305-8569, Japan Received 17 January 2005; revised 18 January 2005; accepted, the a-type transitions are expected to appear at most only in the microwave and in the longer millimeter-wave of discharge-generated DSOD. At that time we had observed the r Q0 and r Q2 branches. The r Q3 branch

  2. Kemiteknik -Vrme-och strmningsteknik Processteknikens grunder (PTG) 2015

    E-Print Network [OSTI]

    Zevenhoven, Ron

    , Z = Pv/RT (for n=1mole) 5. KJ05 Q3-1 An arctic explorer builds a temporary shelter from wind, , the enthalpies h, and the energy flows Q (heat) and W (power), as given in the Table. Calculate all (8) values tar emot W2 = 50 kJ energi i form av arbete, efter vilket den är vid tillstånd "2". Från detta

  3. Kemiteknik -Vrme-och strmningsteknik Processteknikens grunder (PTG) 2014

    E-Print Network [OSTI]

    Zevenhoven, Ron

    , Z = Pv/RT (for n=1mole) 5. KJ05 Q3-1 An arctic explorer builds a temporary shelter from wind, , the enthalpies h, and the energy flows Q (heat) and W (power), as given in the Table. Calculate all (7) valuesJ värme medan den tar emot W2 = 50 kJ energi i form av arbete, efter vilket den är vid tillstånd "2". Från

  4. A disease of swine caused by a chromobacterium species 

    E-Print Network [OSTI]

    Sippel, William Lawrence

    1955-01-01

    ?Pa(y.?h.b.PO< TABLE OF CONTENTS x? pPOTa?mrOpaP O9, 1gs,'s, w'us,1 VS r9Q6M6V'w4, Q?uM ?g6?'w,uM 9's 864 V,,8 1,swQgV,1 JQ,?g6us?S g8 sAg8,? p4 A's w68sg1,Q,1 65 su55gwg'84 gM? J6Q4'8w, 56Q ' 1gss,Q4'4g68 JQ6V?,M 56Q 49, 56??6Ag8C Q,'s68s7 ?'? p4 'JJ,'Qs 's '8...M,?? 1gs4g8w4?S 6 5 9S1Q6C,8 wS'8g1, 5xA9gw9 A's JQ61uw,1 g8 Eu'84g4S?xx P6 649,Q Q,5,Q,8w,s 46 49gs J9,86M,868 A,Q, ,8w6u84,Q,1? I 7I <,Q4gw '81 n6u?C'?6? x?? gs6?'4,1 5g? , 1g55,Q,84 sJ,wg,s 65 V 'w4,Qg? 6J9'C, 56Q ?r? ?g6?'w,uM 5Q6M 49, s,A,Q A...

  5. Large-$q$ expansion of the specific heat for the two-dimensional $q$-state Potts model

    E-Print Network [OSTI]

    H. Arisue; K. Tabata

    1998-07-03

    We have calculated the large-$q$ expansion for the specific heat at the phase transition point in the two-dimensional $q$-state Potts model to the 23rd order in $1/\\sqrt{q}$ using the finite lattice method. The obtained series allows us to give highly convergent estimates of the specific heat for $q>4$ on the first order transition point. The result confirm us the correctness of the conjecture by Bhattacharya et al. on the asymptotic behavior of the specific heat for $q \\to 4_+$.

  6. Effect of soil temperature on resistance of rice to seedling blight caused by Sclerotium rolfsii Sacc 

    E-Print Network [OSTI]

    Weerapat, Praphas

    1964-01-01

    I":". . -"';-'. , ;::::, RP9?C2 '|GZ - GGt'W "ZR%Zh&'~I'Tgfi *" zo?: 3~Gh'&IPWI|tG! Eh QZ 'BXCAK. - TQ '-, ';: ?' ! ', -':;, i", , ;. :;?-i;'!:G :. BGGZZIIG BBIZGGG, ':G"G", Kl'GZ' h il 'ZZZIIGXIIXGLGZGBZZ;::"BGG. ''::, . :":G ';"', . '?'i... . ". -", "!4&, ";;. . "-TQj:. :. W$4'j@"+hg4ja, " gp, . '. ~@@i"-W? i:RICO, ". "keX5 q -4X'q '. "' ~= ', , '- -', '-' ", . ' ' '-, , . ?' Sxe ?-:. yx4tib&"-Mph'ig. . :t0. :-py$e'gi&Xg' 4hagpk- 'Qg ' . "; P...

  7. The accuracy, stability and convergence characteristics of solution procedures for nonlinear structural analysis 

    E-Print Network [OSTI]

    Malek, Michele

    1974-01-01

    causes a large change in displacement, then the solution is likely to become unstable. However, if the structure stiffens as the load is increased then the solution will be stable. 28 aK NL, O fI q a. Unstabl. e Solution aK . o gq b. Stable... of stability is evident when the fourth-order Milne predictor-corrector equations are used to solve a simple first order linear differential equation. The Milne predictor equation is given by 33 q. =- q. + ?, dP [2g(q. ) ? g(q. , ) + 2g(q. )] 4 (III-30...

  8. Pion photo- and electroproduction and the chiral MAID interface

    E-Print Network [OSTI]

    M. Hilt; B. C. Lehnhart; S. Scherer; L. Tiator

    2015-11-18

    We discuss the extended on-mass-shell scheme for manifestly Lorentz-invariant baryon chiral perturbation theory. We present a calculation of pion photo- and electroproduction up to and including order $q^4$. The low-energy constants have been fixed by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID (http://www.kph.uni-mainz.de/MAID/chiralmaid/). We explain how our program works and how it can be used for further analysis.

  9. 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...

  10. Pion photo- and electroproduction and the chiral MAID interface

    E-Print Network [OSTI]

    Hilt, M; Scherer, S; Tiator, L

    2015-01-01

    We discuss the extended on-mass-shell scheme for manifestly Lorentz-invariant baryon chiral perturbation theory. We present a calculation of pion photo- and electroproduction up to and including order $q^4$. The low-energy constants have been fixed by fitting experimental data in all available reaction channels. Our results can be accessed via a web interface, the so-called chiral MAID (http://www.kph.uni-mainz.de/MAID/chiralmaid/). We explain how our program works and how it can be used for further analysis.

  11. PowerConsumption(mW) Radio in sleeping state/periodic poll

    E-Print Network [OSTI]

    x q 4 Radio on Radio in sleeping state/periodic poll 1 2 3 H ' Gc ( G8 ( P E A c P '@ 8E 'E ' 9 0 P 5 0( A E 9 8 P0 A ( W 0 (A G '@ 8 ( G & b8 ( I A P 3 3 '8E b A A E G0( 8 P A E 2 B P 3 ' 5 8E ' b A ( ( ' b P ' G G8 V P@ P A A I@ P8 b6 '@ 8 ( G P A V A 6A 5 } A '@ (A P c @ ' ' A E 8 V 30 b

  12. 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...

  13. Engineering exotic phases for topologically protected quantum computation by emulating quantum dimer models RID B-7826-2008 

    E-Print Network [OSTI]

    Albuquerque, A. Fabricio; Katzgraber, Helmut G.; Troyer, Matthias; Blatter, Gianni.

    2008-01-01

    1934. 5, Osgood, N ~ R "A Theory of Flexure for Beams uith Nonparallel Extreme Fibers. " Journal of ~Alied Eechanics3 Vol. VIS No. 13 (SePtemberp 1939). PP. A 122-126. 6. Saksena~ G. B. "Shear Stress in Tapering Beam. " Aircraft Engineer inE, Vol... derived in mgr tcnct on the theory of elastioity, ox ccrc ~ Y(p-q) ? 4-&x The plus or adnus sign is used depending on the angle 8 and ths shear Sheol groyono/ Figure 13 If 9 is batsmen the shear diagonal and Og, then Oj is aigsbraioa13y ~ than OX...

  14. Grazing activities of cattle on the Jornada Experimental Range during the summer growing season of 1950 

    E-Print Network [OSTI]

    Kilpatrick, Henry Metz

    1955-01-01

    on ~ ? ~ ? ~ ~ ~ ~ ~ ~ ~ ~ ~ 44 ZXST OF FX0USS6 (eOSTZSUS0) 14 ~ 15m 17 ~ 18' Slo Timed aotivit1es of cattle in Al+ K~ 1960 ~ ~ ~ ~ ~ ~ ~ Timed activities of cattle in Angus't 6S 1950 ~ ~ ~ s ~ ~ Timed activities of cattle in August 6s 1950 ~ ~ i ~ ~ ~ Timed... cattle in August Sls 1950 ~ ~ ~ ~ ~ ~ Timed activities of cattle in August Q4S 1960 ~ ~ ~ e ~ ~ Timed activities of cattle in August SVS 1950 s ~ ~ ~ ~ ~ Timed activities of cattle in August Sly 1960 ~ ~ ~ ~ ~ ~ Timed activities of oattle...

  15. SANS (small angle neutron scattering) measurement of deuterium-dislocation correlation in palladium

    SciTech Connect (OSTI)

    Heuser, B.J.; Summerfield, G.C.; King, J.S. ); Epperson, J.E. )

    1989-11-01

    Small angle neutron scattering (SANS) measurements have been made on deformed polycrystal palladium samples with and without deuterium dissolved in the solution phase ({alpha}) at room temperature. Concentrations were held constant during SANS experiments by an equilibrium gas pressure cell. The difference scattering cross section for the same sample with and without deuterium loading has a 1/Q behavior (Q=4{pi}/{lambda} sin{theta}/2) at intermediate values of Q. At very low values of Q the dependence is much stronger than 1/Q. The 1/Q behavior is attributed to deuterium trapping close to long dislocation cores forming rod-like scattering structures.

  16. Coal Distribution Database, 2008

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming963 1.969 1.979Coal4Cubic Feet) Gas Wells (Million7 December3Q4Q 2009

  17. Colorado Associated-Dissolved Natural Gas, Wet After Lease Separation,

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming963 1.969 1.979Coal4Cubic Feet) Gas Wells (Million7 December3Q4Q

  18. Milk fat composition of a lactating dairy cow as influenced by abomasal infusion of various long chain fatty acids 

    E-Print Network [OSTI]

    Switzer, Leonard Anderson

    1971-01-01

    Ql 0 tD E IQ CD 4 ID 3 0 0 0 4 Q? 0 ttl CQ 0 0 4 4 LQ 0 Ln CJ 4 tD 3 0 Q- Q? IQ cnl 4 tD 3 Ql 0 CI 0 0 Q- 4 L- ID 0 Gl Lnl o cn 0 4 CQ 3 tD 0 0 0 C Q- 4 Q- IQ 0 Ql cnl cl cn ID 37 IQ V tl In U 4 O cnl 0 CO F ll O... in the same column uith dif'ferent superscripts (a, b, c) differed significantly (P&0. 05). 20 03 C 'I Cll IO LO I CO M OI IO N M IO N IO H C7I 4 LC3 D N M C LO CO D rt W N t N D Ot Cll N N CO LO IO (O CO D D D N \\0 IO LO (8 N N N LO M D f71 CII...

  19. The Fourth Positive System of Carbon Monoxide in the Hubble Space Telescope Spectra of Comets

    E-Print Network [OSTI]

    Roxana E. Lupu; Paul D. Feldman; Harold A. Weaver; Gian-Paolo Tozzi

    2007-08-22

    The rich structure of the Fourth Positive System (A-X) of carbon monoxide accounts for many of the spectral features seen in long slit HST-STIS observations of comets 153P/Ikeya-Zhang, C/2001 Q4 (NEAT), and C/2000 WM1 (LINEAR), as well as in the HST-GHRS spectrum of comet C/1996 B2 Hyakutake. A detailed CO fluorescence model is developed to derive the CO abundances in these comets by simultaneously fitting all of the observed A-X bands. The model includes the latest values for the oscillator strengths and state parameters, and accounts for optical depth effects due to line overlap and self-absorption. The model fits yield radial profiles of CO column density that are consistent with a predominantly native source for all the comets observed by STIS. The derived CO abundances relative to water in these comets span a wide range, from 0.44% for C/2000 WM1 (LINEAR), 7.2% for 153P/Ikeya-Zhang, 8.8% for C/2001 Q4 (NEAT) to 20.9% for C/1996 B2 (Hyakutake). The subtraction of the CO spectral features using this model leads to the first identification of a molecular hydrogen line pumped by solar HI Lyman-beta longward of 1200A in the spectrum of comet 153P/Ikeya-Zhang. (Abridged)

  20. Diophantine properties for q-analogues of Dirichlet's beta function at positive integers

    E-Print Network [OSTI]

    Jouhet, Frederic

    2008-01-01

    small In this paper, we define $q$-analogues of Dirichlet's beta function at positive integers, which can be written as $\\beta_q(s)=\\sum_{k\\geq1}\\sum_{d|k}\\chi(k/d)d^{s-1}q^k$ for $s\\in\\N^*$, where $q$ is a complex number such that $|q|transcendance of the numbers $\\beta_q(2s+1)$ for $q$ algebraic such that $0numbers $\\beta_q(2s)$: we give a lower bound for the dimension of the vector space over $\\Q$ spanned by $1,\\beta_q(2),\\beta_q(4),...,\\beta_q(A)$, where $1/q\\in\\Z\\setminus\\{-1;1\\}$ and $A$ is an even integer. As consequences, for $1/q\\in\\Z\\setminus\\{-1;1\\}$, on the one hand there is an infinity of irrational numbers among $\\beta_q(2),\\beta_q(4),...$, and on the other hand at least one of the numbers $\\beta_q(2),\\...

  1. Systematics of ground-state quadrupole moments of odd-A deformed nuclei determined with muonic M x rays

    SciTech Connect (OSTI)

    Tanaka, Y.; Steffen, R.M.; Shera, E.B.; Reuter, W.; Hoehn, M.V.; Zumbro, J.D.

    1984-05-01

    The ground-state quadrupole moments of /sup 151/Eu, /sup 153/Eu, /sup 159/Tb, /sup 163/Dy, /sup 167/Er, /sup 177/Hf, /sup 179/Hf, /sup 191/Ir, and /sup 193/Ir were determined by measuring the quadrupole hyperfine-splitting energies of muonic M x rays. The results are Q = 0.903(10) e b for /sup 151/Eu, Q = 2.412(21) e b for /sup 153/Eu, Q = 1.432(8) e b for /sup 159/Tb, Q = 2.648(21) e b for /sup 163/Dy, Q = 3.565(29) e b for /sup 167/Er, Q = 3.365(29) e b for /sup 177/Hf, Q = 3.793(33) e b for /sup 179/Hf, Q = 0.816(9) e b for /sup 191/Ir, and Q = 0.751(9) e b for /sup 193/Ir. The present quadrupole moments, compared with values obtained from electronic-atom hyperfine measurements, show that the Sternheimer correction factors used in the rare-earth electronic-atom analysis are unreliable. Systematics of deformation parameters ..beta../sub 2/ calculated from the present quadrupole moments for odd-A nuclei, and from B(E2) values of Coulomb excitation measurements for even-A nuclei, also indicate that the largest deformation change so far known exists between /sup 151/Eu and /sup 153/Eu. Except at the onset of nuclear deformation, the deformation parameters of the odd-A nuclei are quite consistent with those of the even-A neighbors.

  2. Suction recirculation and its effects upon axial-flow pump power consumption 

    E-Print Network [OSTI]

    Prince, Tony M.

    1983-01-01

    1 Test Procedure Outline 2 Section and Pump Critical Flowrates and Speeds. 63 91 3 Power Coefficient and Reynolds Number Based on Cone Radius. 100 4 Power Coefficient and Reynolds Number Based on Surface Area. 101 5 Power Coefficient... Variation with NPSH with Q rl 54 Head Variation with NPSH with Q 2 . r2 55 Head Variation with NPSH with Q 3. r3' 120 128 129 130 131 134 135 136 CHAPTER I INTRODUCTION Pumps of different types are used to displace liquids from one location...

  3. Fabrication of triangular nanobeam waveguide networks in bulk diamond using single-crystal silicon hard masks

    SciTech Connect (OSTI)

    Bayn, I.; Mouradian, S.; Li, L.; Goldstein, J. A.; Schröder, T.; Zheng, J.; Chen, E. H.; Gaathon, O.; Englund, Dirk; Lu, M.; Stein, A.; Ruggiero, C. A.; Salzman, J.; Kalish, R.

    2014-11-24

    A scalable approach for integrated photonic networks in single-crystal diamond using triangular etching of bulk samples is presented. We describe designs of high quality factor (Q?=?2.51?×?10{sup 6}) photonic crystal cavities with low mode volume (V{sub m}?=?1.062?×?(?/n){sup 3}), which are connected via waveguides supported by suspension structures with predicted transmission loss of only 0.05?dB. We demonstrate the fabrication of these structures using transferred single-crystal silicon hard masks and angular dry etching, yielding photonic crystal cavities in the visible spectrum with measured quality factors in excess of Q?=?3?×?10{sup 3}.

  4. The non-Gaussian character of gravity wave displacements 

    E-Print Network [OSTI]

    Pickett, Robert E. Lee

    1965-01-01

    ?, it is insuf- fioiscct for the dosysr insight tuto tho process that we recydre. " S. ~ (15) U RAPTER I INEROPUUFXog In Hovsabsr 196l a severe storm ~ ARGUS XKMD Boeosroh Tower ~ 22 vCllss soccthwost of ~ During this stern mcvos up to AA feet in hckght... 14. 5 16 5 7C 17. 5 . 06 2 2 7 15 26 62 -5 93 82 93 C6 83 21 85 81 44 '1 5 18 )7 15 6 6 4 1 1 1200 Ths seoond rex lists the ~ of seconds a Q3n3saian ~bu- tion with the ease mean and warianos weald have spent in ~ble...

  5. Jump Chaotic Behaviour of Ultra Low Loss Bulk Acoustic Wave Cavities

    E-Print Network [OSTI]

    Maxim Goryachev; Warrick G. Farr; Serge Galliou; Michael E. Tobar

    2014-06-16

    We demonstrate a previously unobserved nonlinear phenomenon in an ultra-low loss quartz Bulk Acoustic Wave cavity ($Q>3\\times10^9$), which only occurs below 20 milli-Kelvin in temperature and under relatively weak pumping. The phenomenon reveals the emergence of several stable equilibria (at least two foci and two nodes) and jumps between these quasi states at random times. The degree of this randomness as well as separations between levels can be controlled by the frequency of the incident carrier signal. It is demonstrated that the nature of the effect lays beyond the standard Duffing model.

  6. Jump chaotic behaviour of ultra low loss bulk acoustic wave cavities

    SciTech Connect (OSTI)

    Goryachev, Maxim, E-mail: maxim.goryachev@uwa.edu.au; Farr, Warrick G.; Tobar, Michael E. [ARC Centre of Excellence for Engineered Quantum Systems, University of Western Australia, 35 Stirling Highway, Crawley WA 6009 (Australia); Galliou, Serge [Department of Time and Frequency, FEMTO-ST Institute, ENSMM, 26 Chemin de l'Épitaphe 25000 Besançon (France)

    2014-08-11

    We demonstrate a previously unobserved nonlinear phenomenon in an ultra-low loss quartz bulk acoustic wave cavity (Q>3>10{sup 9}), which only occurs below 20 mK in temperature and under relatively weak pumping. The phenomenon reveals the emergence of several stable equilibria (at least two foci and two nodes) and jumps between these quasi states at random times. The degree of this randomness as well as separations between levels can be controlled by the frequency of the incident carrier signal. It is demonstrated that the nature of the effect lies beyond the standard Duffing model.

  7. BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY

    E-Print Network [OSTI]

    Kantor, William M.

    (/, Z[l/p]) denote the intersection PSO(/, Qp)'nPGL(n, Z[l/p]) within PGL(n,Qp), and similarly PGO(/, Z- (i) Let = eg, &7,ci6,66*^6* or as, and let A be the affine building of PSO(/,Q2). Here T can be any and reflections. (ii) Let = &5,e6, or b'e = Xax ? + ^x h a n ( l let A be the building of PSO(/,Q3). The group rm

  8. Isolation of indole-producing bacteria from white shrimp (Penaeus setiferus) 

    E-Print Network [OSTI]

    Smith, Rodney Lee

    1981-01-01

    . 26 5. 40 &3. 0 &3. 0 7. 20 5. 04 7. 36 &3. 0 &3. 0 9. 04 4. 38 8. 57 &3. 0 &3. 0 9. 80 4. 20 9. 04 &3, Q &3. 0 10. 43 12 8+ C 8+ D 8+ I 8+ CDT 8 NT NT NT NT NT 4. 98 5. 23 &3, 0 &3. 0 6. 94 4. 48 6. 49 &3. 0 &3. 0 8... (Member) (Head of Departm nt) December 1981 1804861 ABSTRACT Isolation of Indole-producing Bacteria from White Shrimp (Penaeus setiferus). (December 1981) Rodney Lee Smith, B. S. , Texas A&M University Chairman of Advisory Committee: Dr. Ranzell...

  9. Range versus confinement rearing of pullets of five egg strains and crosses on all-mash and mash and oats diets 

    E-Print Network [OSTI]

    Taylor, Jimmy Neal

    1958-01-01

    Vit. k 2, 2 f0, 000 I, U. psx' ton Vit. Q 3. , $62, 000 I. U. pex ton Feed uireaant The avexage veekiF food conauaption pex chick fox tho i'ive stocks is given in Table 2. A graph of these data is given in Figure 2, Ths vooklF feed intake dux'ing... yercent oats after eleven veeks vhich caused the total food consumption to be soaovhat highex than if only aaah had been fed to all birds. 10 Table 2. Average voskly feed consumption per cMck for f ive ccasaercial strains of egg pPodl10tion stoclc I...

  10. 3.3V Low Power EIA/TIA562 Transceiver

    E-Print Network [OSTI]

    Berns, Hans-Gerd

    Low, IOUT = ­ 1.6mA (VCC = 3.3V) q 0.2 0.4 V Output High, IOUT = 160µA (VCC = 3.3V) q 3.0 3.2 V Output Supply Generator V+ Output Voltage IOUT = 0mA 5.7 V IOUT = 5mA 5.5 V V­ Output Voltage IOUT = 0mA ­5.3 V Narrow Package s Uses Small Capacitors: 0.1µF s Operates to 120kBaud s Output Overvoltage Does Not Force

  11. Interstat Issue 10 

    E-Print Network [OSTI]

    1978-01-01

    -t O CD Cu to CO M 01 - a K - 3 3 r t ro p> co o q " a ro . H - O O O Q 3 * M 3 " Pl r t 3 *- oi ro H . 01 3 • a O ^ W r | o . 01 H - H - 3 3 * r r o i r r o ro o n i- h i- h H - O r o h o r t ro c < r t x 01 3 o q n ^ O O O < 3 3...

  12. Statistical models for noise-robust speech recognition

    E-Print Network [OSTI]

    van Dalen, Rogier Christiaan

    2011-11-08

    (·) , ? Element-wise exponentiation, logarithm, multiplication Distributions p Real distribution q Approximate distribution p˜ Empirical distribution E{a} Expected value of a Ep{a} Expected value of a under p Var{a} Variance of a KL(p?q) Kullback... -Leibler divergence to p from q H(p?q) Cross-entropy of p and q 3 contents H(p) Entropy of p 1(·) Indicator function (Kronecker delta): evaluates to 1 if the argument is true and to 0 otherwise ?a(x) Dirac delta: distribution with non-zero density only at x = a, where...

  13. Development of a Web-based Emissions Reduction Calculator for Street Light and Traffic Light Retrofits 

    E-Print Network [OSTI]

    Liu, Z.; Gilman, D.; Haberl, J. S.; Culp, C.

    2005-01-01

    Page C.l - PROJECT D E S C R I P T I O N ........................................ ^5 C.2 - ASSUMPTION OF RESPONSIBILITY........................... ... 51 C.2.1 - PLANNING AND SCHEDULING........................... ... 51 C.2.2 - TRACKING AND C O N... \\ 5-1 O O ?H ?H a} CU PM P-i w X n ? PL, Q <3 PQ CJ P w CJ EC 5-1O 4JcdL

  14. The bipolar charging of submicrometer particles (0.03 [micrometers is less than or equal to] Dp [is less than or equal to] 0.31 [ micrometers]) by bipolar air ions: an experimental study 

    E-Print Network [OSTI]

    Laughlin, Gary Jay

    1982-01-01

    accumul ates charge . The char gi ng rate resulting from this treatment is given by: 3KE 2 u N ~ ? - Q - u N ~~+ ? + Q (3) where: E = the electric f1eld strength (statvolt/cm) K = the d1electric constant (dimensionless) + + The product term... in these experiments were 3, 10 and (unipolar posit1ve), and the time dependence of charging, characterized by the dom1nant ion conductivity- + + charging t1me product (u N t), was investigated between the limits ot 10 and 10 (statvolts ~ cm) . The result1ng aerosol...

  15. An analysis of modified convective available potential energy and Richardson number in mid-latitude squall line environments 

    E-Print Network [OSTI]

    Stricherz, James Nicholas

    1989-01-01

    10 April is indicated by heavy solid line, position at 0135 UTC 11 April by heavy dotted line. 45 N 40 N 35 N 30 N 35 N tgF '. . OQN "". . ?, , . . . ~ p" -- PIA . ". : . '/ / / DEN r - '. "" ' TOP:: 1 A r/. Q ? 3P ' DDC ? 80-- 'I... UTC 09 May 1979 F' . 10. Surface chart for tg. Fig. 11. Radar summaries fur 0235 UTC, 09 May 1979 (a), aud 0435 UTC& 09 May 1979 (b). was the shortest squall line of the cases studied, averaging less than 400 km. At about 0735 UTC 10 May...

  16. Possible experimental evidence for the presence of double octupole states in {sup 240}Pu

    SciTech Connect (OSTI)

    Pascu, S.; Spieker, M.; Bucurescu, D.; Faestermann, T.; Hertenberger, R.; Skalacki, S.; Weber, S.; Wirth, H. F.; Zamfir, N. V.; Zilges, A.

    2012-10-20

    Excited states in the {sup 240}Pu nucleus have been studied by means of the (p,t) reaction using the Q3D spectrometer and the focal plane detector from Munich. The comparison between experimental angular distributions and the DWBA calculations allowed the extraction of relative two-neutron transfer strengths. These observables may reveal important information about the structure of different states. The experimental two neutron strength for the 0{sup +}{sub 2} and 0{sup +}{sub 3} states is found in good agreement with the predictions of the IBA model, confirming the double octupole nature for the 0{sup +}{sub 2} state proposed in the previous studies.

  17. THE AEROSPACE CORPORATION '

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE

  18. THE AEROSPACE CORPORATION /

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/ @

  19. THE AEROSPACE CORPORATION Suite X00, 955 L'

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/ @X00,

  20. THE AEROSPACE CORPORATION \

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/

  1. THE NRC HAS ISSUED Ati ACTION PLAN FOR CLEANUP OF 46 SfTES that;;ece

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRC HAS

  2. THE SCIOTO ORDNANCE PLANT

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRC HAS'

  3. THE UNIVERSITY' OF CHICAGO

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRC

  4. THIS CONTRACT, entered into this

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRCTHIS

  5. TITLE

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRCTHIS

  6. TITLE

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRCTHIS

  7. TITLE

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRCTHIS

  8. TITLE

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRCTHIS

  9. TITLE

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRCTHIS

  10. TITLE

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3 THE/NRCTHIS,

  11. TITLE

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3

  12. TITLE

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages 12 and

  13. TO

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages 12 and

  14. TO

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages 12

  15. TO

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages 12J.

  16. TO : John T. Sherman, Assistant Director for

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages

  17. TO : R. f. Snlth, Jr. Assistmt Director, DATE:

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages: R. f.

  18. TO : S. R. Sapirie, Manager C&c Ridge Operations Office FROM

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages: R.

  19. TO : W. B. Harris

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages: R./:'

  20. TO :Lyall E. Johnson, Chief Licensing Branch

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages:

  1. TO I

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages: . PBOM

  2. TO I PROM'

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages: .

  3. TO I Ppi B. Harris, Chief, Industrial Rygiene Branah

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages: .Ppi

  4. TO J. A. QuigUy, M.D. NATIONALLPADCW~

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages: .PpiJ.

  5. TO UT ICA METAIS DIVISIONOF THEUTICADROPFORGEQ TOOT, CORP. NATIONAL LEAD COMPANY

    Office of Legacy Management (LM)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of NaturalDukeWakefield Municipal Gas &SCE-SessionsSouth DakotaRobbins and700, 1. .&. ' , c 1 1; -.ll 1q 3Pages:

  6. Dish Stirling High Performance Thermal Storage FY15Q1 Quad Chart

    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:Speeding accessby aLED Street Lighting Host Site: City ofNovelQ3: Charles1800

  7. Dish Stirling High Performance Thermal Storage FY15Q2 Quad Chart

    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:Speeding accessby aLED Street Lighting Host Site: City ofNovelQ3:

  8. Lone Star II (1Q08) Wind Farm | 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 APPENDIXsource History ViewInformationWindsCompressedListguided wavesLone Star I (4Q07)Q3)II

  9. the Y-12 Times, March 2010

    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 m m mDiurnalCarbonU CDesigning* .:q / ~ ~ -3

  10. Historic Patterns of CO

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would likeUniverse (JournalvivoHigh energyHighland View school4-TP59.01 C5;44 4 o (Q3 a - -c15

  11. Historical

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would likeUniverse (JournalvivoHigh energyHighland View school4-TP59.01 C5;44 4 o (Q3 a -

  12. Historical Average Priority Firm Power Rates (rates/previous)

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would likeUniverse (JournalvivoHigh energyHighland View school4-TP59.01 C5;44 4 o (Q3 a

  13. Historical Liquid Discharges and Outfalls

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration would likeUniverse (JournalvivoHigh energyHighland View school4-TP59.01 C5;44 4 o (Q3

  14. DOE/EIA-0202(84/3Q) Short-Term Energy Outlook

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct: Crude7)8)4)1Q)3Q)

  15. DOE/EIA-0202(88/3Q) Energy Information Administration Short-Term

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct:5/4Q)2Q) Energy4Q)2Q)3Q)

  16. DOE/EIA-0202(89/2Q)

    Gasoline and Diesel Fuel Update (EIA)

    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 Natural GasAdjustments (Billion Cubic Feet) Wyoming Dry NaturalPrices1 Table 1.101CompanyProduct:5/4Q)2Q) Energy4Q)2Q)3Q)2Q)

  17. The 40m General Purpose Small-Angle Neutron Scattering Instrument at Oak Ridge National Laboratory

    SciTech Connect (OSTI)

    Wignall, George D [ORNL; Bailey, Katherine M [ORNL; Buchanan, Michelle V [ORNL; Butler, Paul D [ORNL; Heller, William T [ORNL; Littrell, Ken [ORNL; Lynn, Gary W [ORNL; Melnichenko, Yuri B [ORNL; Myles, Dean A A [ORNL; Urban, Volker S [ORNL

    2012-01-01

    A high-flux, 40m long small-angle neutron scattering (SANS) instrument has been constructed at Oak Ridge National Laboratory (ORNL). The facility utilizes a mechanical velocity selector, pinhole collimation and a high count-rate (> 105 Hz), large-area (1m2) two-dimensional position-sensitive detector. The incident wavelength ( ), resolution ( / ), incident collimation and sample-detector distance are independently variable under computer control. The detector can translate 45cm off axis to increase the overall Q-range (< 0.001 < Q = 4 -1sin < 1 -1), where 2 is the angle of scatter. The design and characteristics of this instrument are described along with examples of scattering data to illustrate the performance.

  18. Digital Doppler radial velocity data compared objectively with digital reflectivity radar data 

    E-Print Network [OSTI]

    Beaver, Thomas Foster

    1980-01-01

    . , few components toward or away from the radar greater than -1 5 m s . However at 3 km and 4 km a def1n1te area of convergence is noted (Figs. 9 and 10). Although neither the ref lect1vity nor radial veloc1ty analyses at th1s time ind1cate any def1... I N 4 N CLI ILI IL O J ILI 6 0 ) Id CC OE IC + ILI IC I Vl ?T T W 0 0 0 LLI 0 Z 4( W 3 C- 7: LLI ri 4 4 I I N 0' 0 \\L III gQ ~ 4 N NZ WO 8 I 4l zj WN ~4I III W I- g I 0 R 0 O. I 0 0 ~ N 0 0 LI 0 0...

  19. Chebyshev polynomial approximation of the solution to an ordinary differential equation 

    E-Print Network [OSTI]

    Kim, Gil Chang

    1965-01-01

    DQ 50Q 4~( e 15 IF (D(I)+GAD(J)) GQ TO 500 DENQM~D ( I ) D(I)~D(J) D(V)~DENOM CONT INVE CONT I NVE 're ~ a ~ RRINT THE RESULTS osse ~ DQ 666 I~)e )5 C ( I ) ~DEXP ( D ( I li ) 5 ( I ) ~EVAI if O ( I ) ) YX(1)ARABS(C(I ) B(l ) ) CONT IN VE...120)o KEY IIQ FOFXY~YVALPDEXP(T(2e&))-YVALoooe2-YVAL GQ TQ )30 120 FOFXY~DEXP(-T(2oJ)) 2eO~YVAL -IeQ 130 RETURN END DOVBLE PRECI S I GN FVNCTI ON EVAL tl X ) C C THIS ROVTINE EVAl VATES Y(X) AT Xs C DIMENSION TX((5& 15) eXT(15s 15) & VX (15...

  20. Uncertainty Quantification of the Pion-Nucleon Low-Energy Coupling Constants up to Fourth Order in Chiral Perturbation Theory

    E-Print Network [OSTI]

    K. A. Wendt; B. D. Carlsson; A. Ekström

    2014-10-02

    We extract the statistical uncertainties for the pion-nucleon ($\\pi N$) low energy constants (LECs) up to fourth order $\\mathcal{O}(Q^4)$ in the chiral expansion of the nuclear effective Lagrangian. The LECs are optimized with respect to experimental scattering data. For comparison, we also present an uncertainty quantification that is based solely on \\pin{} scattering phase shifts. Statistical errors on the LECs are critical in order to estimate the subsequent uncertainties in \\textit{ab initio} modeling of light and medium mass nuclei which exploit chiral effective field theory. As an example of the this, we present the first complete predictions with uncertainty quantification of peripheral phase shifts of elastic proton-neutron scattering.

  1. An accounting system for a Class I motor common carrier of property 

    E-Print Network [OSTI]

    Packenham, Edward S

    1950-01-01

    QL 'be thoee a?4? to ecsssoetiag lgaoa fee therma Iwstim ef ~ swww ~ J4llkl sw%swl? 1$ %Ash QR OOMMtlaI lllWI leap%&~ S4? 4?ysHag+ f?ea ?see@tel eaah haaliieg ynreo4ese ia ws4? eoeoeasrg 'hy tho ical oat?WLieh?4 ~o of aet oetMomsctct wheseia a aanrsoe...?ahar wiD ba grayer?4g yr?yegg eyg?ci??4 e?4 yeiC. thC? CrrL?a yreei?C?e tha yassihglitf ef fLNlacc? t??a?t ee ahliC?CC??at ~?g. Cll ?f ths ?cyley?es will be yes ee e waahig basis* Vega?CX y?re? ??4 y?y?aaA 4?tes vill bs acCaaCcQ?4 se ee ts yaaac...

  2. Field Notes, Middle America (1956-1968) 

    E-Print Network [OSTI]

    Davis, William B.

    2012-04-09

    &&dLdI f{. L & ? P'3< a3Lc t xLQc32s_? 42...T3{3k VL!e Cat5 j/b) [&vvL,L t e{Q 4Ur te{Qc{3c2YLc p&?2e2&Q X r ?Z t e{ . ! 2Q C }2eL X t e{ . ! 2Q $ &vc...

  3. Bacteriology of cottage cheese: Sources of microorganisms causing spoilage and relative numbers at various stages during processing and storage. 

    E-Print Network [OSTI]

    Maury, James B

    1951-01-01

    ~gi h ~ 4' h I 'I a 8 . 1, ~* tk' gM W . j I 1 " -'; ' '" tsee~jA-~'e", . ig. :+ epeiAe?sr . . ~;"iI?4LiIX. :~r s?I: 4@, .I ~ 4~&rd if. :4s~ 6%54i~'lreeeuse 4t Qii. . ~' @&at, ' tee440% 54 ' of . L0$: ?NAssste! a. . . ' &'e, +?4%4~'4+~~4?I.... 8 (& ' lc )i @~4 8 l l :jjfg, I --4 ~ ~ ~Aj ~u 4 Il A8 C5P 850 gkpg5. A'j q4j, p I ". Ji1 7 ~ , l ~ gK' * . lj I' jp:;. 'i p . l 4 me ~Xj . a'jikkjjb4 'kfi~so, , W iLLl"-, g~W':, . ~. ~ Mes hqt, . 'k wis etc~ &os...

  4. Ebensburg folio, Pennsylvania 

    E-Print Network [OSTI]

    Butts, Charles, 1863-1946.

    1905-01-01

    ~zsisreet. diMrI'F44 BQ EMicer kcteet3 4ccQi, ~&? Eel'1$er rt GRtch ?t 'iezks 484 Vakvera~ wttb lkLreeJI, b-g5 bad ~teated tbet it bshe eb AatidL~'rr~ . t '0 ectido ixh t~ ~-'. ~ ~ a4 cQkvee& PeLleted . ~lg cr ' ~ 'r ead ?Bek:~ Rgb vere giveKL ee a feme ciao... MS' L~t~ @beg M. '' calves vere I. . ~i%'~ to eet et eve Qs~. + c4; age ~ ~~-'& ~t11 tbsp ead yf t:- -""-. . :rimeeti Thy j@r~ ~. . ';alf QCa~'~~ ~ ea ho P~p~74 ~+'QQ pQLQIQo H0 ~L ~&~ Q H 4@h eg pQ 4~a eZ eku 4~~~~ w& eR C&m @ALL~~. "~~ egml~a 'E...

  5. Measurement of B(d) mixing using opposite-side flavor tagging

    E-Print Network [OSTI]

    Baringer, Philip S.; Bean, Alice; Coppage, Don; Hensel, Carsten; Moulik, Tania; Wilson, Graham Wallace

    2006-12-15

    identification algorithm can be found in Ref. [9]. DØ 0 1000 -1 -0.5 0 0.5 1 Muon jet charge N um be r o f e ve nt s (a) q(brec) 0 0 500 -1 -0.5 0 0.5 1 Muon jet charge N um be r o f e ve nt s (b) 0 250 -1 -0.5 0 0.5 1 Electron jet charge N um... for electrons QeJ. Here q#4;brec#7; is the charge of the muon from the reconstruction side. DØ 0 200 -1 -0.5 0 0.5 1 SV charge N um be r o f e ve nt s (a) q(brec) 0 0 1000 -1 -0.5 0 0.5 1 SV charge N um be r o f e ve nt s (b) 0 2000 -1 -0.5 0 0.5...

  6. An investigation of relationships between meso- and synoptic-scale phenomena 

    E-Print Network [OSTI]

    Wood, James Eugene

    1971-01-01

    . The figure shows the trough sloping westward from '04i . 0, &47' . ' / 'I I la 2:-, f WQQ. ' gf' , I g I. . I . ?, i&9 I +3~o . . --'; (a) 850 mb 34 ) 1- K . g(7!- . I , p6. (c) 500 mb 'r 'I 9" . 3O8 303 , . 3l 2 1 332 (b) 700 mb Fig. 6...'. '. '" "147 ~; C . r, t I' l. , 4 I -s 430 , 1I 1/0 3- 156 147 I 44, , $4 (a) 850 mb '652 6 fy, '". 534~53'4 &0 1540% P q'', -4 65$ 'g' )( C' ~i5~7 (c) 500 mb 0910 ' 88 I, ' ' 8196gp ', 70 -" - . - : . , '- ' ' ' ' ' ' . 'F4 0 . 97p 000...

  7. Waterfowl utilization characteristics of floodwater retarding structures in north-central Texas 

    E-Print Network [OSTI]

    Hobaugh, William Carl

    1977-01-01

    of the physical and limnological characteristics of 55 flood prevention lakes. Parameters +I IU Ql 0 E 0. 0 Ql Ql 0 QI Ql O IQ 4 lQ L Ql 5- I/I cL Ql IQ K L. LI QI QI CL Ol ) CU cC cC CU 0 O LI IU I IQ I- Ql 5- Ql Cll IU IV O lQ 4 IU I...- CO M IQ O 3 ~ 0 GL 0 E/) LL III z 0. cC Ql 0 lU CL Ql OI Ul QI OI IQ CL Ul O C O IQ Ql L 0 0 0 L 0 Ql IU CL Ql Lll CQ Shoreline development Surface area ++ ++ ++ Age Average depth Drainage area to surface area...

  8. An economic evaluation of fertilizer application to Coastal Bermudagrass under irrigation on Lufkin fine sandy loam 

    E-Print Network [OSTI]

    Prochaska, Frank Charles

    1958-01-01

    AZ:-V@~'. W. . ; j)~303;. ~t42@~6 W. 't5e':, X eqv Ny@ee4. . - gW':. Mi': 6e~m. qZ k '. 5g:~~ "'~M~'. 4pggiRCS; , . 'A~t?'. "Xgg8, . ' ?- ~qi ''Sijb] johns' A~S~i@tmeX'%e~~m = ', 1 il l:, . "i 'i":. ", , i:;:, :, . 'ilia. ;:;::. ::." ' Ag ggMSI iC!L V... ''. '. . . =, . '=;;;-"i-"' A&~Mf@$. C@';40 'g5$XS. ; @4i6"-Cli'PS~4. , 6$$ '0 . (@Bi?' ' 'Q~' Qm'MM') 1 (kg', K4'. X. 4AQCi~wWQw ) A~mC'. 3@~8 1 J +; r ! ~BV~~RVS - - SyeeQ4:. -jp~t44vide La;~assai-to. . ~-. 8? -4+-. '-NLlMqth? -: -. kaa~~ie& MM...

  9. Trends in U.S. Venture Capital Investments Related to Energy: 1980 through the Third Quarter of 2010

    SciTech Connect (OSTI)

    Dooley, James J.

    2010-11-08

    This report documents trends in U.S. venture capital investments over the period 1980 through the third quarter of calendar year 2010 (2010 Q1+Q2+Q3). Particular attention is given to U.S. venture capital investments in the energy/industrial sector over the period 1980-2010 Q1+Q2+Q3 as well as in the more recently created cross-cutting category of CleanTech over the period 1995-2010 Q1+Q2+Q3. During the early 1980s, U.S. venture capital investments in the energy/industrial sector accounted for more than 20% of all venture capital investments. However subsequent periods of low energy prices, the deregulation of large aspects of the energy industry, and the emergence of fast growing new industries like computers (both hardware and software), biotechnology and the Internet quickly reduced the priority accorded to energy/industrial investments. To wit, venture capital investments related to the energy/industrial sector accounted for only 1% of the $132 billion (in real 2010 US$) invested in 2000 by the U.S. venture capital community. The significant increase in the real price of oil that began in 2003-2004 correlates with renewed interest and increased investment by the venture capital community in energy/industrial investment opportunities. Venture capital investments for 2009 for the energy/industrial sector accounted for $2.4 billion or slightly more than 13% of all venture capital invested that year. The total venture capital invested in energy/industrial during the first three quarters of 2010 is close to $2.4 billion accounting for slightly less than 15% of all venture capital investments during the first three quarters of 2010. In 2009, the aggregate amount invested in CleanTech was $2.1 billion (11% of the total US venture capital invested in that lean year) and for the first three quarters of 2010 US venture capital investments in CleanTech have already exceeded $2.8 billion (18% of all US venture capital investments made during the first three quarters of 2010). Between 2004 and 2009, U.S. venture capital investments in energy/industrial as well as CleanTech have more than quadrupled in real terms.

  10. Compressibility factors for retrograde gases: a new correlation 

    E-Print Network [OSTI]

    Corredor Real, Jairo Hernando

    1991-01-01

    CI o CD ID CI N O CD IA O O CD O 00 CD 00 O O CQ CD CD F) 0& CD O CD O CD N N o o CO IA N 00 CD N N Q) CD CD ID CO P3 O N O O o O VO O 00 N O O CD N CO ICI O O IA LD N N P O N CD O CD O N CO IA N... CD N IA 00 N O ID dl CL O CL Cd O ID 0 e 12 &C O CI O h O e O) O C dl OI O 13 z e Cd CL O 0 e Id K O ID e Cd Q3 Cd Cd ID D I O ID 0$ C e D I e Cd X e Id CL e C Cd 0 0) C dl Cd Cd 0 O Z CI...

  11. Calculation of K-shell fluorescence yields for low-Z elements

    SciTech Connect (OSTI)

    Nekkab, M.; Kahoul, A.; Deghfel, B.; Aylikci, N. Küp; Aylikçi, V.

    2015-03-30

    The analytical methods based on X-ray fluorescence are advantageous for practical applications in a variety of fields including atomic physics, X-ray fluorescence surface chemical analysis and medical research and so the accurate fluorescence yields (?{sub K}) are required for these applications. In this contribution we report a new parameters for calculation of K-shell fluorescence yields (?{sub K}) of elements in the range of 11?Z?30. The experimental data are interpolated by using the famous analytical function (?{sub k}/(1??{sub k})){sup 1/q} (were q=3, 3.5 and 4) vs Z to deduce the empirical K-shell fluorescence yields. A comparison is made between the results of the procedures followed here and those theoretical and other semi-empirical fluorescence yield values. Reasonable agreement was typically obtained between our result and other works.

  12. The {sup 14}C-Cluster and Molecular bands in the Oxygen Isotopes {sup 18,20}O

    SciTech Connect (OSTI)

    Oertzen, W. von [Helmholtz-Zentrum Berlin, Glienicker Strasse 100, D-14109 Berlin (Germany); Fachbereich Physik, Freie Universitaet Berlin (Germany); Dorsch, T.; Bohlen, H. G. [Helmholtz-Zentrum Berlin, Glienicker Strasse 100, D-14109 Berlin (Germany)

    2009-08-26

    We have studied states in {sup 18}O and {sup 20}O with the ({sup 7}Li,p) reaction on {sup 12}C and {sup 14}C targets at E{sub lab}({sup 7}Li) = 44 MeV, using the high resolution Q3D magnetic spectrometer at the Maier-Leibnitz-Laboratory in Munich. The systematics of the excitation energies and cross sections were used to construct rotational bands with high moments of inertia. The bands observed are discussed in terms of underlying ({sup 14}C x {sup 4}He)-cluster structure for {sup 18}O, and for {sup 20}O the cluster structures are ({sup 14}C x {sup 6}He) and ({sup 14}C x 2n x alpha). The intrinsically reflection asymmetric shapes give rise to molecular bands, which appear as parity inversion doublets.

  13. Probing Nilsson states in {sup 233}U

    SciTech Connect (OSTI)

    Kotthaus, T.; Reiter, P.; Hess, H.; Kalkuehler, M.; Wendt, A.; Wiens, A. [Institut fuer Kernphysik, Universitaet zu Koeln, D-50937 Koeln (Germany); Hertenberger, R.; Morgan, T.; Thirolf, P. G.; Wirth, H.-F. [Fakultaet fuer Physik, Ludwig-Maximilians-Universitaet Muenchen, D-85748 Garching (Germany); Faestermann, T. [Physik Department E12, Technische Universitaet Muenchen, D-85748 Garching (Germany)

    2011-07-15

    The reaction {sup 234}U(d-vector, t){sup 233}U was measured at the Munich Q3D magnetic spectrometer with a polarized deuteron beam. The beam energy was 22 MeV, and a vector polarization of the deuterons of 80% was achieved. Angular distributions of the reaction cross section and analyzing power at seven angles between 5 deg. and 35 deg. were analyzed. Spin and parity assignments for 33 states were determined by comparison with results from distorted wave Born approximation (DWBA) calculations. Based on these assignments and energy systematics, the observed states were sorted into rotational bands. The Nilsson configurations of the bands are identified by examining the population strengths within each band. Two rotational bands with Nilsson configurations 1/2[501] and 3/2[501] could be identified for the first time.

  14. High-resolution study of 0{sup +} and 2{sup +} excitations in {sup 168}Er with the (p,t) reaction

    SciTech Connect (OSTI)

    Bucurescu, D. [Horia Hulubei National Institute of Physics and Nuclear Engineering, P.O. Box MG-6, R-76900 Bucharest (Romania); Graw, G.; Hertenberger, R. [Sektion Physik, Ludwig Maximilians Universitaet Muenchen, Am Coulombwall 1, D-85748 Garching (Germany); Wirth, H.-F.; Faestermann, T.; Kruecken, R.; Mahgoub, M. [Physik Department, Technische Universitaet Muenchen, D-85748 Garching (Germany); Lo Iudice, N. [Dipartimento di Scienze Fisiche, Universita di Napoli 'Federico II' and Istituto Nazionale di Fisica Nucleare, Monte S Angelo, Via Cintia I-80126 Naples (Italy); Sushkov, A.V.; Shirikova, N.Yu. [Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, RU-141980 Dubna (Russian Federation); Sun, Y. [Department of Physics and Joint Institute for Nuclear Astrophysics, University of Notre Dame, Notre Dame, Indiana 46556 (United States); Department of Physics, Tsinghua University, Beijing 100084 (China); Department of Physics, Xuzhou Normal University, Xuzhou, Jiangsu 221009 (China); Jolie, J.; Brentano, P. von; Braun, N.; Heinze, S.; Moeller, O.; Muecher, D.; Scholl, C. [Institut fuer Kernphysik, Universitaet zu Koeln, D-50937 Cologne (Germany); Casten, R.F.; Meyer, D.A. [Wright Nuclear Structure Laboratory, Yale University, New Haven, Connecticut 06520-8124 (United States)

    2006-06-15

    Excited states in the deformed nucleus {sup 168}Er have been studied with high-energy resolution, in the (p,t) reaction, with the Munich Q3D spectrograph. A number of 25 excited 0{sup +} states (four tentative) and 63 2{sup +} states have been assigned up to 4.0 MeV excitation energy. This unusually rich characterization of the 0{sup +} and 2{sup +} states in a deformed nucleus, close to a complete level scheme, offers a unique opportunity to check, in detail, models of nuclear structure that incorporate many excitation modes. A comparison of the experimental data is made with two such models: the quasiparticle-phonon model (QPM), and the projected shell model (PSM). The PSM wave functions appear to contain fewer correlations than those of the QPM and than required by the data.

  15. Review: Saskia Pronk-Tiethoff: The Germanic Loanwords in Proto-Slavic

    E-Print Network [OSTI]

    Holzer, Georg

    2014-06-26

    ;#3;]#17;#3; %#17;#3; LQ#3;37#3;#21;#19;#15;#3;ZR#3;VLH#3;HUZlKQW#15;#3;GDVV#3;.L#3;#16; SDUVN\\#3; IU#3; GLH#3; HUVWHQ#3; QDFK#3;FKULVW#3;OL#3;FKHQ#3; -DKU#3;KXQ#3;GHU#3;WH#3;PLW#3;VODYLVFK#16;JHUPDQLVFKHQ#3; .RQWDNWHQ#3;LQ#3;2VW#3;SUHX?HQ#3;UHFKQHW#12;#17;#3;9JO...;#3; ,Q#3; DOW#3;NU#17;#3; clez#3; LVW#3; GLHVH#3; DOW#16; EXO#3;JD#3;ULVFKH#3;'LVVL#3;PL#3;OD#3;WLRQ#3; QDWXU#3;JH#3;Pl?#3; DXV#3;JH#3;EOLHEHQ#3; #11;ZlKUHQG#3; HV#3; NU#17;#3; GHQQRFK#3; Y?W?]#3;KHL?W#12;#17; =XPLQGHVW#3; HUZlKQW#3; XQG#3; DP#3;EHVWHQ#3...

  16. Inflection points of microcanonical entropy: Monte Carlo simulation of q state Potts model on a finite square lattice

    SciTech Connect (OSTI)

    Praveen, E. Satyanarayana, S. V. M.

    2014-04-24

    Traditional definition of phase transition involves an infinitely large system in thermodynamic limit. Finite systems such as biological proteins exhibit cooperative behavior similar to phase transitions. We employ recently discovered analysis of inflection points of microcanonical entropy to estimate the transition temperature of the phase transition in q state Potts model on a finite two dimensional square lattice for q=3 (second order) and q=8 (first order). The difference of energy density of states (DOS) ? ln g(E) = ln g(E+ ?E) ?ln g(E) exhibits a point of inflexion at a value corresponding to inverse transition temperature. This feature is common to systems exhibiting both first as well as second order transitions. While the difference of DOS registers a monotonic variation around the point of inflexion for systems exhibiting second order transition, it has an S-shape with a minimum and maximum around the point of inflexion for the case of first order transition.

  17. The crystal structure of the triphenylphosphine sulfide - iodine addition complex 

    E-Print Network [OSTI]

    Schweikert, William Walter

    1966-01-01

    -6 -8 -1 ? 1 -2 36. &BGQ 4. &. 7 -&GO 32. 7 (Gn &3. 5. on 'S &GO 3'i. 5 7 n!3 34. 75OO 2 5. 1 7 C(, ' 3 ') . 7 ( (i !i ? 7. 2 3 Gin ? '3. 7 COO Zci. C ( GO ?5 ~ 73QO 2 '- . I 3 6 F' , G 43. B?Qn 1'3. 7 )no 2 ~ '& 2 n Q ?&3. 4& n Bc.... Zan 1 120 ~ Zl-! p ~ 4 117. 7a5. 2 125. 2i4. 5 115. 9+5. 5 127, 2+4, 3 118 ' 3+4, 4 113, 4+4. 5 125, 6+5. 8 113 ' 4a4o7 124. ~ 1+4. ~ 6 116. 3a5. 7 C(17) -C(10) -C(13) C(10) -C (13) -C( 1)g) 10)i ~ 9+6. 3 131. 3+6. 3 29 Table 7...

  18. Noise reduction control strategy of a permanent magnet synchronous machine for vehicle applications 

    E-Print Network [OSTI]

    Doolittle, Randy Gene

    2009-05-15

    that was not available: 1. V S (secant voltage) or a phase voltage to give a value to the BackEMF (E) 2. L A , L B , L C (phase inductances), L S (secant inductance), or L D and L Q 3. M D ? (magnet flux linkage) or B G (air gap flux density) The thesis... T EM,rated d-q rated Torque 309Nm V S,rated Secant Voltage I S,rated,rms Secant Rated RMS Current 300A P ,rated Rated Machine Power P ,max Maximum Machine Power 64.5kW ? ,max Top Speed E Back EMF @ Top Speed 400V (assumed could be 600V...

  19. A symplectic subgroup of a pseudounitary group as a subset of Clifford algebra

    E-Print Network [OSTI]

    Nikolai Marchuk; Roman Dyabirov

    2008-10-18

    Let Cl1(1,3) and Cl2(1,3) be the subsets of elements of the Clifford algebra Cl(1,3) of ranks 1 and 2 respectively. Recently it was proved that the subset Cl2(p,q)+iCl1(p,q) of the complex Clifford algebra can be considered as a Lie algebra. In this paper we prove that for p=1, q=3 the Lie algebra Cl2(p,q)+iCl1(p,q) is isomorphic to the well known matrix Lie algebra sp(4,R) of the symplectic Lie group Sp(4,R). Also we define the so called symplectic group of Clifford algebra and prove that this Lie group is isomprphic to the symplectic matrix group Sp(4,R).

  20. Electron-Transport Properties of Amorphous (Zr0.64ni0.36)1-Xalx Alloys 

    E-Print Network [OSTI]

    BHATNAGAR, AK; PAN, R.; Naugle, Donald G.

    1989-01-01

    .06 ?~x=0.15 ?x=0. 1 0 x=0.20 C; 210- 1.04- OO x =0.25~ . . ::.- -? .~x=0.05 185 . 1.02-. x=0.0~ '- 160 0.1 0.2 0.3 FIG. 2. Room-temperature (300-K) resistivity p as a function of Al concentration x for amorphous (ZrQ 64NiQ 3{j), Al... coefficient 8& for amorphous (ZrQ 64NiQ 36) ) Al . 0 0.05 0.10 0.15 0.20 0.25 0.30 Tcryst (K) 679' 747" 718" 785" 764' 792' 800' T. (K) 2.54' 2.560' 2.68g 2.05' 2.33g 1.62' 1.810 pm (g/cm ) 7.25' 7.10' 6.96' 6.73' 6.53' 6...

  1. THE TAOS PROJECT: RESULTS FROM SEVEN YEARS OF SURVEY DATA

    SciTech Connect (OSTI)

    Zhang, Z.-W.; Lehner, M. J.; Wang, J.-H.; Wen, C.-Y.; Wang, S.-Y.; King, S.-K.; Cook, K. H.; Lee, T. [Institute of Astronomy and Astrophysics, Academia Sinica. 11F of Astronomy-Mathematics Building, National Taiwan University. No. 1, Sec. 4, Roosevelt Road, Taipei 10617, Taiwan (China); Granados, A. P. [Instituto de Astronomia, Universidad Nacional Autonoma de Mexico, Apdo. Postal 106, Ensenada, Baja California 22800 (Mexico); Alcock, C.; Protopapas, P. [Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138 (United States); Axelrod, T. [Steward Observatory, 933 North Cherry Avenue, Room No. 204, Tucson AZ 85721 (United States); Bianco, F. B. [Center for Cosmology and Particle Physics, New York University, 4 Washington Place, New York, NY 10003 (United States); Byun, Y.-I. [Department of Astronomy and University Observatory, Yonsei University, 134 Shinchon, Seoul 120-749 (Korea, Republic of); Chen, W. P. [Institute of Astronomy, National Central University, No. 300, Jhongda Road, Jhongli City, Taoyuan County 320, Taiwan (China); Coehlo, N. K. [Department of Statistics, University of California Berkeley, 367 Evans Hall, Berkeley, CA 94720 (United States); De Pater, I. [Department of Astronomy, University of California Berkeley, 601 Campbell Hall, Berkeley, CA 94720 (United States); Kim, D.-W. [Max Planck Institute for Astronomy, Koenigstuhl 17, D-69117 Heidelberg (Germany); Lissauer, J. J. [Space Science and Astrobiology Division 245-3, NASA Ames Research Center, Moffett Field, CA 94035 (United States); Marshall, S. L., E-mail: zwzhang@asiaa.sinica.edu.tw [Kavli Institute for Particle Astrophysics and Cosmology, 2575 Sand Hill Road, MS 29, Menlo Park, CA 94025 (United States); and others

    2013-07-01

    The Taiwanese-American Occultation Survey (TAOS) aims to detect serendipitous occultations of stars by small ({approx}1 km diameter) objects in the Kuiper Belt and beyond. Such events are very rare (<10{sup -3} events per star per year) and short in duration ({approx}200 ms), so many stars must be monitored at a high readout cadence. TAOS monitors typically {approx}500 stars simultaneously at a 5 Hz readout cadence with four telescopes located at Lulin Observatory in central Taiwan. In this paper, we report the results of the search for small Kuiper Belt objects (KBOs) in seven years of data. No occultation events were found, resulting in a 95% c.l. upper limit on the slope of the faint end of the KBO size distribution of q = 3.34-3.82, depending on the surface density at the break in the size distribution at a diameter of about 90 km.

  2. An experimental and mathematical investigation of hydrocarbon steam distillation 

    E-Print Network [OSTI]

    Langhoff, John Allan

    1984-01-01

    I LIJ D D CO D CIC D P1a L), OOLQLI [ [ LQS LQ WP8Q$ ?7) I/I I?I hl m ~ III O I?I I/I O & P) ?I- 0 O nj (Z) 4J Q O E III ID Cl ?I ?I Q ?/ ??: PJ Cl C C I?l ICl E ?J ??I I III 0 az I? I W K Q3 Ctl IQ C) PV... decreases near the end of the run. Th1s occurs when the volume of hydrocarbon 1n the 11quid phase of the distillation cell becomes small and cannot support 1ts vapor pressure. 07 C5 0 III QI 5- I/I QI 5- 0- 5- 0 CL IQ ) 0 CQ Ol O 0 4J Itl...

  3. Ki-67 Is an Independent Predictor of Metastasis and Cause-Specific Mortality for Prostate Cancer Patients Treated on Radiation Therapy Oncology Group (RTOG) 94-08

    SciTech Connect (OSTI)

    Verhoven, Bret [University of Wisconsin Carbone Cancer Center, Madison, Wisconsin (United States)] [University of Wisconsin Carbone Cancer Center, Madison, Wisconsin (United States); Yan, Yan [RTOG Statistical Center, Philadelphia, Pennsylvania (United States)] [RTOG Statistical Center, Philadelphia, Pennsylvania (United States); Ritter, Mark, E-mail: ritter@humonc.wisc.edu [University of Wisconsin Carbone Cancer Center, Madison, Wisconsin (United States)] [University of Wisconsin Carbone Cancer Center, Madison, Wisconsin (United States); Khor, Li-Yan [Case Medical Center, Cleveland, Ohio (United States)] [Case Medical Center, Cleveland, Ohio (United States); Hammond, Elizabeth [LDS Hospital, Salt Lake City, Utah (United States)] [LDS Hospital, Salt Lake City, Utah (United States); Jones, Christopher [Radiological Associates of Sacramento, Sacramento, California (United States)] [Radiological Associates of Sacramento, Sacramento, California (United States); Amin, Mahul [Cedars-Sinai Medical Center, Los Angeles, California (United States)] [Cedars-Sinai Medical Center, Los Angeles, California (United States); Bahary, Jean-Paul [Centre Hospitalier de l'Université de Montréal-Notre Dame, Montreal, Ontario (Canada)] [Centre Hospitalier de l'Université de Montréal-Notre Dame, Montreal, Ontario (Canada); Zeitzer, Kenneth [Albert Einstein Medical Center, Philadelphia, Pennsylvania (United States)] [Albert Einstein Medical Center, Philadelphia, Pennsylvania (United States); Pollack, Alan [University of Miami Miller School of Medicine, Miami, Florida (United States)] [University of Miami Miller School of Medicine, Miami, Florida (United States)

    2013-06-01

    Purpose: The association of Ki-67 staining index (Ki67-SI) with overall survival (OS), disease-specific mortality (DSM), distant metastasis (DM), and biochemical failure (BF) was examined in men with favorable- to intermediate-risk prostate cancer receiving radiation therapy (RT) alone or with short-term androgen deprivation (ADT) in Radiation Therapy Oncology Group (RTOG) 94-08. Methods and Materials: 468 patients (23.6%) on RTOG 94-08 had sufficient tissue for Ki67-SI analysis. The median follow-up time was 7.9 years. Ki67-SI was determined by immunohistochemistry and quantified manually and by image analysis. Correlative analysis versus clinical outcome was performed using the third quartile (?Q3) cutpoint. A proportional hazards multivariable analysis (MVA) dichotomized covariates in accordance with trial stratification and randomization criteria. Results: In MVAs adjusted for all treatment covariates, high Ki67-SI (?Q3) was correlated with increased DSM (hazard ratio [HR] 2.48, P=.03), DM (HR 3.5, P=.002), and BF (HR 3.55, P<.0001). MVA revealed similar Ki67-associated hazard ratios in each separate treatment arm for DSM, DM, and BF; these reached significance only for DM in the RT-alone arm and for BF in both arms. Ki67-SI was not a significant predictor of intraprostatic recurrence assessed by repeated biopsy 2 years after treatment. Patients with a high or low Ki67-SI seemed to experience a similar relative benefit from the addition of ADT to radiation. Conclusions: High Ki67-SI independently predicts for increased DSM, DM, and protocol BF in primarily intermediate-risk prostate cancer patients treated with RT with or without ADT on RTOG 94-08 but does not predict for local recurrence or for increased relative benefit from ADT. This and prior studies lend support for the use of Ki67-SI as a stratification factor in future trials.

  4. The EB factory project. II. Validation with the Kepler field in preparation for K2 and TESS

    SciTech Connect (OSTI)

    Parvizi, Mahmoud; Paegert, Martin; Stassun, Keivan G.

    2014-12-01

    Large repositories of high precision light curve data, such as the Kepler data set, provide the opportunity to identify astrophysically important eclipsing binary (EB) systems in large quantities. However, the rate of classical “by eye” human analysis restricts complete and efficient mining of EBs from these data using classical techniques. To prepare for mining EBs from the upcoming K2 mission as well as other current missions, we developed an automated end-to-end computational pipeline—the Eclipsing Binary Factory (EBF)—that automatically identifies EBs and classifies them into morphological types. The EBF has been previously tested on ground-based light curves. To assess the performance of the EBF in the context of space-based data, we apply the EBF to the full set of light curves in the Kepler “Q3” Data Release. We compare the EBs identified from this automated approach against the human generated Kepler EB Catalog of ?2600 EBs. When we require EB classification with ?90% confidence, we find that the EBF correctly identifies and classifies eclipsing contact (EC), eclipsing semi-detached (ESD), and eclipsing detached (ED) systems with a false positive rate of only 4%, 4%, and 8%, while complete to 64%, 46%, and 32%, respectively. When classification confidence is relaxed, the EBF identifies and classifies ECs, ESDs, and EDs with a slightly higher false positive rate of 6%, 16%, and 8%, while much more complete to 86%, 74%, and 62%, respectively. Through our processing of the entire Kepler “Q3” data set, we also identify 68 new candidate EBs that may have been missed by the human generated Kepler EB Catalog. We discuss the EBF's potential application to light curve classification for periodic variable stars more generally for current and upcoming surveys like K2 and the Transiting Exoplanet Survey Satellite.

  5. Tax decisions involving the cost method of inventory valuation 

    E-Print Network [OSTI]

    McMenamy, Bobby Benton

    1950-01-01

    '. ?1'pQ@lg'QP ig, ". t O'Q@ ". 'Q J. '~" @~i 8 GXG C4 S6 7) PQ. &3. C'5'c' 'P~$. C" 'v'1&~ PIC&/'~%CD%'b ". QCO~1"10@7'8 ZRGQ4 3;4-'i;", ZCQQgpy P&C. $~tQ jf&53 ~~'1 $1 lg ~CXXQi1 d') + s. 2 ( C ) c XZ 3iQC9 'Nl& ACt Gf 1~1'3 y v~l8 BO&~il-"". 'XC...~15QXCX 8 pPQVXSXGlh 'KVQ~ 'K'lg OGB'5 9" Q2g p~5Q~B l&PQBQCGG. 8211CC @18 DC'. i', $Q~NDg Qf 4-. !'w QQQX' Bit&11 LAC3M8 ROC & GZ'WZl66 Q. MXQGA~ 49 M16'- BCC&QQG~g f, Q?" 4V pX'GQU4510'1 Qa iI-'Q "36~'43%43. ~~ 81 t9. @18 ' gX153TXc?:XHg ig, g. '?XO...

  6. Depression among abused or neglected children in substitute care 

    E-Print Network [OSTI]

    Woodward, Gail Cohn

    1985-01-01

    CJ I OI CJ CO COCh 0?0?Q Q HIO 0 4J V t0 00 0 N t0 0 Cl 4J 0 Cl nl~ JO g 0 ttt 0 ?0 R M mW ?II M&?CI CJQYI NQN0?I 0 V t0 0 0 4J CJ I/I Q A ?a IOI 0?CO MCJ COI 0?mQ~ OC Cl 44 CI 4J 44 m04~ CO 4J 4J 44 5 A CI 0 Q... Ch CJ CO t?t U1 Cl '0 Q 00 0 44 IJ 0, 44 44 0 84?04 84A' 4J 44 0 IH 6 A t0 44 0 Q CO Q 4J JJ 0 8)8 ttl 44 CI Q 0 0 4J 0 al Cl 0 ?0 0 CI 44 04 M t0 A I A V ?n Cl o 0 0 C4 [00 A 26 the clinical group scores. Each...

  7. Liouville Brownian motion at criticality

    E-Print Network [OSTI]

    Rémi Rhodes; Vincent Vargas

    2015-02-15

    In this paper, we construct the Brownian motion of Liouville Quantum Gravity with central charge $c=1$ (more precisely we restrict to the corresponding free field theory). Liouville quantum gravity with $c=1$ corresponds to two-dimensional string theory and is the conjectural scaling limit of large planar maps weighted with a $O(n=2)$ loop model or a $Q=4$-state Potts model embedded in a two dimensional surface in a conformal manner. Following \\cite{GRV1}, we start by constructing the critical LBM from one fixed point $x\\in\\mathbb{R}^2$ (or $x\\in\\S^2$), which amounts to changing the speed of a standard planar Brownian motion depending on the local behaviour of the critical Liouville measure $M'(dx)=-X(x)e^{2X(x)}\\,dx$ (where $X$ is a Gaussian Free Field, say on $\\mathbb{S}^2$). Extending this construction simultaneously to all points in $\\mathbb{R}^2$ requires a fine analysis of the potential properties of the measure $M'$. This allows us to construct a strong Markov process with continuous sample paths living on the support of $M'$, namely a dense set of Hausdorff dimension $0$. We finally construct the associated Liouville semigroup, resolvent, Green function, heat kernel and Dirichlet form. In passing, we extend to quite a general setting the construction of the critical Gaussian multiplicative chaos that was initiated in \\cite{Rnew7,Rnew12} and also establish new capacity estimates for the critical Gaussian multiplicative chaos.

  8. New method to measure proper motions of microlensed sources: Application to candidate free-floating-planet event MOA-2011-BLG-262

    SciTech Connect (OSTI)

    Skowron, Jan [Warsaw University Observatory, Al. Ujazdowskie 4, 00-478 Warszawa (Poland); Department of Astronomy, Ohio State University, 140 W. 18th Ave., Columbus, OH 43210 (United States); Udalski, Andrzej; Szyma?ski, Micha? K., E-mail: jskowron@astrouw.edu.pl, E-mail: udalski@astrouw.edu.pl, E-mail: msz@astrouw.edu.plm [Warsaw University Observatory, Al. Ujazdowskie 4, 00-478 Warszawa (Poland); and others

    2014-04-20

    We develop a new method to measure source proper motions in microlensing events, which can partially overcome problems due to blending. It takes advantage of the fact that the source position is known precisely from the microlensing event itself. We apply this method to the event MOA-2011-BLG-262, which has a short timescale t {sub E} = 3.8 day, a companion mass ratio q = 4.7 × 10{sup –3}, and a very high or high lens-source relative proper motion ?{sub rel} = 20 mas yr{sup –1} or 12 mas yr{sup –1} (for two possible models). These three characteristics imply that the lens could be a brown dwarf or a massive planet with a roughly Earth-mass 'moon'. The probability of such an interpretation would be greatly increased if it could be shown that the high lens-source relative proper motion was primarily due to the lens rather than the source. Based on the long-term monitoring data of the Galactic bulge from the Optical Gravitational Lensing Experiment, we measure the source proper motion that is small, ?{sub s}=(?2.3,?0.9)±(2.8,2.6) mas yr{sup ?1} in a (north, east) Galactic coordinate frame. These values are then important input into a Bayesian analysis of the event presented in a companion paper by Bennett et al.

  9. Physics in Ultra-strong Magnetic Fields

    E-Print Network [OSTI]

    Duncan, R C

    2000-01-01

    In magnetic fields stronger than B_Q = 4.4 X 10^13 Gauss, an electron'sLandau excitation energy exceeds its rest energy. I review the physics of thisstrange regime and some of its implications for the crusts and magneto- spheresof neutron stars. In particular, I describe how ultra-strong fields >> render the vacuum birefringent and capable of distorting and magnifying images ("magnetic lensing"); >> change the self-energy of electrons: as B increases they are first slightly lighter than $m_e$, then slightly heavier; >> cause photons to rapidly split and merge with each other; >> distort atoms into long, thin cylinders and molecules into strong, polymer-like chains; >> enhance the pair density in thermal pair-photon gases; >> stronglysuppress photon-electron scattering, and >> drive the vacuum itself unstable,at extremely large B. In a concluding section, I discuss recent observations of the spindownhistories of soft gamma repeaters and anomalous X-ray pulsars. The magnetarmodel gives a promising framework for...

  10. Physics in Ultra-strong Magnetic Fields

    E-Print Network [OSTI]

    Robert C. Duncan

    2000-02-23

    In magnetic fields stronger than B_Q = 4.4 X 10^13 Gauss, an electron's Landau excitation energy exceeds its rest energy. I review the physics of this strange regime and some of its implications for the crusts and magneto- spheres of neutron stars. In particular, I describe how ultra-strong fields >> render the vacuum birefringent and capable of distorting and magnifying images ("magnetic lensing"); >> change the self-energy of electrons: as B increases they are first slightly lighter than $m_e$, then slightly heavier; >> cause photons to rapidly split and merge with each other; >> distort atoms into long, thin cylinders and molecules into strong, polymer-like chains; >> enhance the pair density in thermal pair-photon gases; >> strongly suppress photon-electron scattering, and >> drive the vacuum itself unstable, at extremely large B. In a concluding section, I discuss recent observations of the spindown histories of soft gamma repeaters and anomalous X-ray pulsars. The magnetar model gives a promising framework for understanding these data.

  11. Minimally non-local nucleon-nucleon potentials with chiral two-pion exchange including $?$'s

    E-Print Network [OSTI]

    M. Piarulli; L. Girlanda; R. Schiavilla; R. Navarro Pérez; J. E. Amaro; E. Ruiz Arriola

    2015-02-16

    We construct a coordinate-space chiral potential, including $\\Delta$-isobar intermediate states in its two-pion-exchange component. The contact interactions entering at next-to-leading and next-to-next-to-next-to-leading orders ($Q^2$ and $Q^4$, respectively, $Q$ denoting generically the low momentum scale) are rearranged by Fierz transformations to yield terms at most quadratic in the relative momentum operator of the two nucleons. The low-energy constants multiplying these contact interactions are fitted to the 2013 Granada database, consisting of 2309 $pp$ and 2982 $np$ data (including, respectively, 148 and 218 normalizations) in the laboratory-energy range 0--300 MeV. For the total 5291 $pp$ and $np$ data in this range, we obtain a $\\chi^2$/datum of roughly 1.3 for a set of three models characterized by long- and short-range cutoffs, $R_{\\rm L}$ and $R_{\\rm S}$ respectively, ranging from $(R_{\\rm L},R_{\\rm S})=(1.2,0.8)$ fm down to $(0.8,0.6)$ fm. The long-range (short-range) cutoff regularizes the one- and two-pion exchange (contact) part of the potential.

  12. Latest Results of ILC High-Gradient R&D 9-cell Cavities at JLAB

    SciTech Connect (OSTI)

    Rongli Geng

    2008-02-11

    It has been over a year since JLAB started processing and testing ILC 9-cell cavities in the frame work of ILC high-gradient cavity R&D, aiming at the goal of a 35 MV/m gradient at a Q #4; of 1E10 with a yield of 90%. The necessary cavity processing steps include field flatness tuning, electropolishing (EP), hydrogen out-gassing under vacuum, high-pressure water rinsing, clean room assembly, and low temperature bake. These are followed by RF test at 2 Kelvin. Ultrasonic cleaning with Micro-90, an effective post-EP rinsing recipe discovered at JLAB, is routinely used. Seven industry manufactured 9-cell TESLAshape cavities are processed and tested repeatedly. So far, 33 EP cycles are accumulated, corresponding to more than 65 hours of active EP time. An emphasis put on RF testing is to discern cavity quench characteristics, including its nature and its location. Often times, the cavity performance is limited by thermal-magnetic quench instead of field emission. The quench field in some cavities is lower than 20 MV/m and remains unchanged despite repeated EP, implying material and/or fabrication defects. The quench field in some other cavities is high but changes unpredictably after repeated EP, suggesting processing induced defects. Based on our experience and results, several areas are identified where improvement is needed to improve cavity performance as well as yield.

  13. Elements of Greek tragedy in three Eugene O'Neill plays 

    E-Print Network [OSTI]

    Koinm, Albert Julius

    1963-01-01

    '-&o &%3 A eel ~Re~ AG"" VV'"L"XVZ K ~' ' 0 X f&Qkh M R~ SPY 8o Pe 6'bhWCC ~ =-'g* K@ Ey ZQk~~ SQP CAW'~ GR~~~BC ERA 5". '499~ 48VXCC QD 86VQi, CL~. ~G~K~ %~CD ~QQ I'LL tJ::N tNl5~ Qf &98 MQS So ~ 638v e. "~8'~ M mains g ~~ vre~M e Mxm'8... ~ -'Pe Se Se f'~ ZQZ' ll& ~q& ~WC~ QZ ~X Q~& ~%~%I XQ Q% FG~~' Q~ ~~Q Q4RG TJCQ'L 9. B'GQ 5F~@ ~ pPI?3QCC o l j AU~ ~ ~ . a. e :*' e i s s a 0 o s 0 e e e e o e o e s s XVe C JJKU3SXGii e s y s o e o e s o e o e @ o e LXST GF 56K'=3 CGPiSVL~M e a...

  14. The unexpected role of D waves in low-energy neutral pion photoproduction

    E-Print Network [OSTI]

    C. Fernandez-Ramirez

    2009-12-21

    It has been commonly assumed that low-energy neutral pion photoproduction from the proton can be described accounting only for S and P waves, and that higher partial waves are irrelevant. We have found that this assumption is not correct and that the inclusion of D waves is necessary to obtain a reliable extraction of the $E_{0+}$ multipole from experimental data. This is due in large measure to the spontaneous breaking of chiral symmetry in QCD which leads to very small S-wave contributions. This makes the usual partial wave expansion less accurate and although D waves are small, their contribution is enhanced through the interference with P waves, which compromises the S-wave extraction from data if D waves are not taken into account. In our work we have used Heavy Baryon Chiral Perturbation Theory to one loop, and up to ${\\cal O}(q^4)$, to account for the S and P waves, while D waves are added in an almost model-independent way using standard Born terms and vector mesons. We also show that higher partial waves do not play an important role.

  15. Plano de la Habana 

    E-Print Network [OSTI]

    Garcia, Francisco Rojo

    1963-01-01

    , ", '' XOiQ. t ?T-'1:. ". iiX, ', . @X"lc:. :". iC;3X'661871 f'&)p iQQQ~~Q4MW~XCy w~~~' 8"', ~+~~'~6&, . ". "XCXGSp QD&' GCCQUQ0AB4ay A. QO54pi99 KAXCh XVIAi'-" ~CCG~lCJXC '@16 "QDf3 iC t:$Q&~ 0 3X'3iOB8 '". ""GQM PQPYQt 5Q "M~ 8~' Xg5Ai'lG 4~ pL'354"'C...~ QAC'. PG3, $, GVr* '4"'b% CWLPO84XOXl "'A~~Q &"' fhl~u&PX191 BBVG'XikC? c. ' Q+848~% 'iklf, Cgl WQ'gg~ Qg vpgg~ iV'!=8V@1'"g W9. 2. 1 g3. 'O', "MBA fl&~V@V QC X'CGlig@l. y XD p~@QC!X'Q1 i v Q~tX', V@X'~ CgZR~ M1Q VD3. 'QGtiS, GD 0'"' '&'z1VC;1'u...

  16. 8D likelihood effective Higgs couplings extraction framework in h ? 4?

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

    Chen, Yi; Di Marco, Emanuele; Lykken, Joe; Spiropulu, Maria; Vega-Morales, Roberto; Univ. Paris-Sud, Orsay Cedex; Northwestern Univ., Evanston, IL; Xie, Si

    2015-01-23

    We present an overview of a comprehensive analysis framework aimed at performing direct extraction of all possible effective Higgs couplings to neutral electroweak gauge bosons in the decay to electrons and muons, the so called ‘golden channel’. Our framework is based primarily on a maximum likelihood method constructed from analytic expressions of the fully differential cross sections for h ? 4l and for the dominant irreducible $ q\\overline{q} $ ? 4l background, where 4l = 2e2?, 4e, 4?. Detector effects are included by an explicit convolution of these analytic expressions with the appropriate transfer function over all center of massmore »variables. Utilizing the full set of observables, we construct an unbinned detector-level likelihood which is continuous in the effective couplings. We consider possible ZZ, Z?, and ?? couplings simultaneously, allowing for general CP odd/even admixtures. A broad overview is given of how the convolution is performed and we discuss the principles and theoretical basis of the framework. This framework can be used in a variety of ways to study Higgs couplings in the golden channel using data obtained at the LHC and other future colliders.« less

  17. The coincidence problem and interacting holographic dark energy

    SciTech Connect (OSTI)

    Karwan, Khamphee

    2008-05-15

    We study the dynamical behaviour of the interacting holographic dark energy model whose interaction term is Q = 3H({lambda}{sub d}{rho}{sub d}+{lambda}{sub c}{rho}{sub c}), where {rho}{sub d} and {rho}{sub c} are the energy densities of dark energy and cold dark matter respectively. To satisfy the observational constraints from type Ia supernovae, the cosmic microwave background shift parameter and baryon acoustic oscillation measurements, if {lambda}{sub c} = {lambda}{sub d} or {lambda}{sub d},{lambda}{sub c}>0, the cosmic evolution will only reach the attractor in the future and the ratio {rho}{sub c}/{rho}{sub d} cannot be slowly varying at present. Since the cosmic attractor can be reached in the future even when the present values of the cosmological parameters do not satisfy the observational constraints, the coincidence problem is not really alleviated in this case. However, if {lambda}{sub c}{ne}{lambda}{sub d} and they are allowed to be negative, the ratio {rho}{sub c}/{rho}{sub d} can be slowly varying at present and the cosmic attractor can be reached near the present epoch. Hence, the alleviation of the coincidence problem is attainable in this case. The alleviation of the coincidence problem in this case is still attainable when confronting this model with Sloan Digital Sky Survey data.

  18. The effect of a synthetic cytokinin, 6-benzylaminopurine, and light quality on Ficus benjamina under low light intensities 

    E-Print Network [OSTI]

    Meadows, Sylvia Elise

    1979-01-01

    CU CU CU CU CU CU CU CU CU CU CU CU CU CU CU Cg CU CU CU CU CU CU R M M LC M SL' R hC R M R M M M M M R R M GC SC LC CU Gf (J Ia 5 Gl CL O f(f CU LA JJ 0 GS JJ GJ GJ 000 J S 3 3 3 S S S J J'j J 3 3 3'7 3 J J J S 3 LLJ IJJ UJ IJJ LJJ LLJ... the lowest levels. All treatments exhibited more activity I C5W IX: I Q? U CI RQ CS Cl tJ W CL CS CI ~ '? I IU 5- CU O 0 O Ql ;U ) Cl Qt V) X rU rU 5- ) CD 0 QJ 0. 4 0) CU ?t C Q3 O 5 O Ql V) E C 0 I. 'I IU C C C 0 5- 0 (1...

  19. Envelope excitations in electronegative plasmas with electrons featuring the Tsallis distribution

    SciTech Connect (OSTI)

    Bains, A. S.; Li, Bo; Tribeche, Mouloud

    2013-09-15

    We examine the modulational instability (MI) of ion-acoustic waves (IAWs) in an electronegative plasma containing positive and negative ions as well as electrons that follow the nonextensive statistics proposed by Tsallis [J. Stat. Phys. 52, 479 (1988)]. Using the reductive perturbation method, the nonlinear Schrödinger equation that governs the modulational instability of the IAWs is obtained. Inspired by the experimental work of Ichiki et al.[Phys. Plasmas 8, 4275 (2001)], three types of electronegative plasmas are investigated. The effects of various parameters on the propagation of IAWs are discussed in detail numerically. We find that the plasma supports both bright and dark solutions. The presence of the non-extensively distributed electrons is found to play a crucial role in the formation of envelope excitations. The region in the parameter space where the MI exists depends sensitively on the positive to negative ion mass ratio (M) and negative to positive ion density ratio (?). An extensive range of the nonextensive q-parameters (?1<q<3) is considered and in each case the MI sets in under different conditions. The finding of this investigation is useful for understanding stable wave propagation of envelope ion-acoustic solitary waves in space and laboratory plasmas comprising ions with both positive and negative charges as well as non-Maxwellian electrons.

  20. q-state Potts-glass neural network based on pseudoinverse rule

    SciTech Connect (OSTI)

    Xiong Daxing; Zhao Hong [Department of Physics and Institute of Theoretical Physics and Astrophysics, Xiamen University, Xiamen 361005 (China)

    2010-08-15

    We study the q-state Potts-glass neural network with the pseudoinverse (PI) rule. Its performance is investigated and compared with that of the counterpart network with the Hebbian rule instead. We find that there exists a critical point of q, i.e., q{sub cr}=14, below which the storage capacity and the retrieval quality can be greatly improved by introducing the PI rule. We show that the dynamics of the neural networks constructed with the two learning rules respectively are quite different; but however, regardless of the learning rules, in the q-state Potts-glass neural networks with q{>=}3 there is a common novel dynamical phase in which the spurious memories are completely suppressed. This property has never been noticed in the symmetric feedback neural networks. Free from the spurious memories implies that the multistate Potts-glass neural networks would not be trapped in the metastable states, which is a favorable property for their applications.

  1. Coupled Transient Finite Element Simulation of Quench in Jefferson Lab's 11 GeV Super High Momentum Spectrometer Superconducting Magnets

    SciTech Connect (OSTI)

    E. Sun, P. Brindza, S. Lassiter, M. Fowler, E. Xu

    2010-06-01

    This paper presents coupled transient thermal and electromagnetic finite element analysis of quench in the Q2, Q3, and dipole superconducting magnets using Vector Fields Quench code. Detailed temperature distribution within coils and aluminum force collars were computed at each time step. Both normal (quench with dump resistor) and worst-case (quench without dump resistor) scenarios were simulated to investigate the maximum temperatures. Two simulation methods were utilized, and their algorithms, implementation, advantages, and disadvantages are discussed. The first method simulated the coil using nonlinear transient thermal analysis directly linked with the transient circuit analysis. It was faster because only the coil was meshed and no eddy current was modeled. The second method simulated the whole magnet including the coil, the force collar, and the iron yoke. It coupled thermal analysis with transient electromagnetic field analysis which modeled electromagnetic fields including eddy currents within the force collar. Since eddy currents and temperature in the force collars were calculated in various configurations, segmentation of the force collars was optimized under the condition of fast discharge.

  2. Magnetohydrodynamic modes analysis and control of Fusion Advanced Studies Torus high-current scenarios

    SciTech Connect (OSTI)

    Villone, F.; Mastrostefano, S. [Euratom-ENEA-CREATE Ass., DIEI, Univ. di Cassino e Lazio Merid., Cassino (Italy); Calabrò, G.; Vlad, G.; Crisanti, F.; Fusco, V. [C. R. Frascati, Euratom-ENEA Ass., Via E. Fermi 45, 00044 Frascati (Italy); Marchiori, G.; Bolzonella, T.; Marrelli, L.; Martin, P. [Cons. RFX, Euratom-ENEA-RFX Ass., Corso Stati Uniti 4, 35127 Padova (Italy); Liu, Y. Q. [Euratom/CCFE Fusion Association, Culham Science Centre, Abingdon OX14 3DB (United Kingdom); Mantica, P. [IFP-CNR, Euratom-ENEA-CNR Ass. Via Cozzi 53, 20125 Milano (Italy)

    2014-08-15

    One of the main FAST (Fusion Advanced Studies Torus) goals is to have a flexible experiment capable to test tools and scenarios for safe and reliable tokamak operation, in order to support ITER and help the final DEMO design. In particular, in this paper, we focus on operation close to a possible border of stability related to low-q operation. To this purpose, a new FAST scenario has then been designed at I{sub p}?=?10 MA, B{sub T}?=?8.5?T, q{sub 95}???2.3. Transport simulations, carried out by using the code JETTO and the first principle transport model GLF23, indicate that, under these conditions, FAST could achieve an equivalent Q???3.5. FAST will be equipped with a set of internal active coils for feedback control, which will produce magnetic perturbation with toroidal number n?=?1 or n?=?2. Magnetohydrodynamic (MHD) mode analysis and feedback control simulations performed with the codes MARS, MARS-F, CarMa (both assuming the presence of a perfect conductive wall and using the exact 3D resistive wall structure) show the possibility of the FAST conductive structures to stabilize n?=?1 ideal modes. This leaves therefore room for active mitigation of the resistive mode (down to a characteristic time of 1?ms) for safety purposes, i.e., to avoid dangerous MHD-driven plasma disruption, when working close to the machine limits and magnetic and kinetic energy density not far from reactor values.

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

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

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

    2015-01-01

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

  4. Spin Glass Models of Syntax and Language Evolution

    E-Print Network [OSTI]

    Siva, Karthik; Marcolli, Matilde

    2015-01-01

    Using the SSWL database of syntactic parameters of world languages, and the MIT Media Lab data on language interactions, we construct a spin glass model of language evolution. We treat binary syntactic parameters as spin states, with languages as vertices of a graph, and assigned interaction energies along the edges. We study a rough model of syntax evolution, under the assumption that a strong interaction energy tends to cause parameters to align, as in the case of ferromagnetic materials. We also study how the spin glass model needs to be modified to account for entailment relations between syntactic parameters. This modification leads naturally to a generalization of Potts models with external magnetic field, which consists of a coupling at the vertices of an Ising model and a Potts model with q=3, that have the same edge interactions. We describe the results of simulations of the dynamics of these models, in different temperature and energy regimes. We discuss the linguistic interpretation of the paramete...

  5. Structure of rhenium-containing sodium borosilicate glass

    SciTech Connect (OSTI)

    Goel, Ashutosh; McCloy, John S.; Windisch, Charles F.; Riley, Brian J.; Schweiger, Michael J.; Rodriguez, Carmen P.; Ferreira, Jose M.

    2013-03-01

    A series of sodium borosilicate glasses were synthesized with increasing fractions of KReO4 or Re2O7, to 10000 ppm (1 mass%) target Re in glass, to assess the effects of large concentrations of rhenium on glass structure and to estimate the solubility of technetium, a radioactive component in typical low active waste nuclear waste glasses. Magic angle spinning nuclear magnetic resonance (MAS-NMR), Fourier transform infrared (FTIR) spectroscopy, and Raman spectroscopy were performed to characterize the glasses as a function of Re source additions. In general, silicon was found coordinated in a mixture of Q2 and Q3 structural units, while Al was 4-coordinated and B was largely 3-coordinate and partially 4-coordinated. The rhenium source did not appear to have significant effects on the glass structure. Thus, at the up to the concentrations that remain in dissolved in glass, ~3000 ppm Re by mass maximum. , the Re appeared to be neither a glass-former nor a strong glass modifier., Rhenium likely exists in isolated ReO4- anions in the interstices of the glass network, as evidenced by the polarized Raman spectrum of the Re glass in the absence of sulfate. Analogous to SO42-¬ in similar glasses, ReO4- is likely a network modifier and forms alkali salt phases on the surface and in the bulk glass above solubility.

  6. Discovery of $^{34g,m}$Cl$(p,\\gamma)^{35}$Ar resonances activated at classical nova temperatures

    E-Print Network [OSTI]

    Fry, C; Bishop, S; Brown, B A; Chen, A A; Faestermann, T; Hertenberger, R; Parikh, A; Pérez-Loureiro, D; Wirth, H -F; García, A; Ortez, R

    2015-01-01

    Background: The thermonuclear $^{34g,m}$Cl($p,\\gamma$)$^{35}$Ar reaction rates are unknown due to a lack of experimental nuclear physics data. Uncertainties in these rates translate to uncertainties in $^{34}$S production in models of classical novae on oxygen-neon white dwarfs. $^{34}$S abundances have the potential to aid in the classification of presolar grains. Purpose: Determine resonance energies for the $^{34g,m}$Cl($p,\\gamma$)$^{35}$Ar reactions within the region of astrophyical interest for classical novae to a precision of a few keV as an essential first step toward constraining their thermonuclear reaction rates. Method: $^{35}$Ar excited states were populated by the $^{36}$Ar($d,t$)$^{35}$Ar reaction at $E$(d)=22~MeV and reaction products were momentum analyzed by a high resolution quadrupole-dipole-dipole-dipole (Q3D) magnetic spectrograph. Results: Seventeen new $^{35}$Ar levels have been detected at a statistically significant level in the region $E_x\\approx$~5.9-6.7~MeV ($E_r$ \\textless~800~ k...

  7. For the Men at the Front 

    E-Print Network [OSTI]

    Dykes, John Bacchus, 1823-1876 [composer; Oxenham, John, 1852-1941 [author

    2012-03-05

    &~3 A. Pp~ovc~ as to s'~v3. o ~~'~ co-. &ie~zb by: , . c~:ver. Janus~ 1968 U9. 8i". 66 ti~ 5X' ~ JOE g ~ 3GP'8 f QZ Gl~~~QBMQ XQ& QX'884 ill 446 Qi1~& 0 f 66t Q~~ikL'Bg GIVE f QX' MiS iilV$1GGMC GBQ9. $'583MQ LB 16CG'53. Bg GD(l 'OFCCGZ. 'Mg... ~ . ' ~ ' 1 Od iv C j2 L P l Tj', XU~)22Q3UC'j~lC7'2 'i'PAT T. jE CL X1XCS QI'LY The ls22ottiest pzohle2229 i22 philoooohy QG22 'be ezpzesse~l sic2X2ly2 Why Goes acn Got as 228 doeGI XG hc "- free G:. Got lii 8 q Qz is -19 the Xlal'222 of 922 io...

  8. Heavy Truck Engine Program

    SciTech Connect (OSTI)

    Nelson, Christopher

    2009-01-08

    The Heavy Duty Truck Engine Program at Cummins embodied three significant development phases. All phases of work strove to demonstrate a high level of diesel engine efficiency in the face of increasingly stringent emission requirements. Concurrently, aftertreatment system development and refinement was pursued in support of these efficiency demonstrations. The program's first phase focused on the demonstration in-vehicle of a high level of heavy duty diesel engine efficiency (45% Brake Thermal Efficiency) at a typical cruise condition while achieving composite emissions results which met the 2004 U.S. EPA legislated standards. With a combination of engine combustion calibration tuning and the development and application of Urea-based SCR and particulate aftertreatment, these demonstrations were successfully performed by Q4 of 2002. The second phase of the program directed efforts towards an in-vehicle demonstration of an engine system capable of meeting 2007 U.S. EPA legislated emissions requirements while achieving 45% Brake Thermal Efficiency at cruise conditions. Through further combustion optimization, the refinement of Cummins Cooled EGR architecture, the application of a high pressure common rail fuel system and the incorporation of optimized engine parasitics, Cummins Inc. successfully demonstrated these deliverables in Q2 of 2004. The program's final phase set a stretch goal of demonstrating 50% Brake Thermal Efficiency from a heavy duty diesel engine system capable of meeting 2010 U.S. EPA legislated emissions requirements. Cummins chose to pursue this goal through further combustion development and refinement of the Cooled EGR system architecture and also applied a Rankine cycle Waste Heat Recovery technique to convert otherwise wasted thermal energy to useful power. The engine and heat recovery system was demonstrated to achieve 50% Brake Thermal Efficiency while operating at a torque peak condition in second quarter, 2006. The 50% efficient engine system was capable of meeting 2010 emissions requirements through the application of NOx and particulate matter reduction techniques proven earlier in the program.

  9. High performance charge breeder for HIE-ISOLDE and TSR@ISOLDE applications

    SciTech Connect (OSTI)

    Shornikov, Andrey Mertzig, Robert C.; Wenander, Fredrik J. C.; Beebe, Edward N.; Pikin, Alexander

    2015-01-09

    We report on the development of the HEC{sup 2} (High Energy Compression and Current) charge breeder, a possible high performance successor to REXEBIS at ISOLDE. The new breeder would match the performance of the HIE-ISOLDE linac upgrade and make full use of the possible installation of a storage ring at ISOLDE (the TSR@ISOLDE initiative [1]). Dictated by ion beam acceptance and capacity requirements, the breeder features a 2–3.5 A electron beam. In many cases very high charge states, including bare ions up to Z=70 and Li/Na-like up to Z=92 could be requested for experiments in the storage ring, therefore, electron beam energies up to 150 keV are required. The electron-beam current density needed for producing ions with such high charge states at an injection rate into TSR of 0.5–1 Hz is between 10 and 20 kA/cm{sup 2}, which agrees with the current density needed to produce A/q<4.5 ions for the HIE-ISOLDE linac with a maximum repetition rate of 100 Hz. The first operation of a prototype electron gun with a pulsed electron beam of 1.5 A and 30 keV was demonstrated in a joint experiment with BNL [2]. In addition, we report on further development aiming to achieve CW operation of an electron beam having a geometrical transverse ion-acceptance matching the injection of 1{sup +} ions (11.5 ?m), and an emittance/energy spread of the extracted ion beam matching the downstream mass separator and RFQ (0.08 ?m normalized / ± 1%)

  10. Measurements on the 3He+?System at ANKE

    E-Print Network [OSTI]

    A. Khoukaz

    2010-11-03

    The differential and total cross-sections for the dp \\to 3He \\eta reaction have been measured in a high precision high statistics COSY-ANKE experiment near threshold using a continuous beam energy ramp up to an excess energy Q of 11.3 MeV with essentially 100% acceptance. The kinematics allowed the mean value of Q to be determined to about 9 keV. Evidence is found for the effects of higher partial waves for Q > 4 MeV. The very rapid rise of the total cross-section to its maximum value within 0.5 MeV of threshold implies a very large \\eta 3He scattering length and hence the presence of a quasi-bound state extremely close to threshold. In addition, differential and total cross-sections have been measured at excess energies of 19.5, 39.4, and 59.4 MeV over the full angular range. While at 19.5 MeV the results can be described in terms of s- and p-wave production, by 59.4 MeV higher partial waves are required. Including the 19.5 MeV point together with the near-threshold data in a global s- and p-wave fit gives a poorer overall description of the data though the position of the pole in the \\eta 3He scattering amplitude, corresponding to the quasi-bound or virtual state, is hardly changed.

  11. Progress in preparing scenarios for operation of the International Thermonuclear Experimental Reactor

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

    Sips, A. C. C.; European Commission, Brussels; Giruzzi, G.; Ide, S.; Kessel, C.; Luce, T. C.; Snipes, J. A.; Stober, J. K.

    2015-02-01

    The development of operating scenarios is one of the key issues in the research for ITER which aims to achieve a fusion gain (Q) of ~10, while producing 500MW of fusion power for ?300 s. The ITER Research plan proposes a success oriented schedule starting in hydrogen and helium, to be followed by a nuclear operation phase with a rapid development towards Q ~ 10 in deuterium/tritium. The Integrated Operation Scenarios Topical Group of the International Tokamak Physics Activity initiates joint activities among worldwide institutions and experiments to prepare ITER operation. Plasma formation studies report robust plasma breakdown in devicesmore »with metal walls over a wide range of conditions, while other experiments use an inclined EC launch angle at plasma formation to mimic the conditions in ITER. Simulations of the plasma burn-through predict that at least 4MW of Electron Cyclotron heating (EC) assist would be required in ITER. For H-modes at q??~ 3, many experiments have demonstrated operation with scaled parameters for the ITER baseline scenario at ne/nGW ~ 0.85. Most experiments, however, obtain stable discharges at H??(y,2) ~ 1.0 only for bN = 2.0–2.2. For the rampup in ITER, early X-point formation is recommended, allowing auxiliary heating to reduce the flux consumption. A range of plasma inductance (li(3)) can be obtained from 0.65 to 1.0, with the lowest values obtained in H-mode operation. For the rampdown, the plasma should stay diverted maintaining H-mode together with a reduction of the elongation from 1.85 to 1.4. Simulations show that the proposed rampup and rampdown schemes developed since 2007 are compatible with the present ITER design for the poloidal field coils. At 13–15 MA and densities down to ne/nGW ~ 0.5, long pulse operation (>1000 s) in ITER is possible at Q ~ 5, useful to provide neutron fluence for Test Blanket Module assessments. ITER scenario preparation in hydrogen and helium requires high input power (>50 MW). H-mode operation in helium may be possible at input powers above 35MW at a toroidal field of 2.65T, for studying H-modes and ELM mitigation. In hydrogen, H-mode operation is expected to be marginal, even at 2.65T with 60MW of input power. Simulation code benchmark studies using hybrid and steady state scenario parameters have proved to be a very challenging and lengthy task of testing suites of codes, consisting of tens of sophisticated modules. Nevertheless, the general basis of the modelling appears sound, with substantial consistency among codes developed by different groups. For a hybrid scenario at 12 MA, the code simulations give a range for Q = 6.5–8.3, using 30MW neutral beam injection and 20MW ICRH. For non-inductive operation at 7–9 MA, the simulation results show more variation. At high edge pedestal pressure (Tped ~ 7 keV), the codes predict Q = 3.3–3.8 using 33MW NB, 20MW EC, and 20MW ion cyclotron to demonstrate the feasibility of steady-state operation with the day-1 heating systems in ITER. Simulations using a lower edge pedestal temperature (~3 keV) but improved core confinement obtain Q = 5–6.5, when ECCD is concentrated at mid-radius and ~ 20MW off-axis current drive (ECCD or LHCD) is added. Several issues remain to be studied, including plasmas with dominant electron heating, mitigation of transient heat loads integrated in scenario demonstrations and (burn) control simulations in ITER scenarios.« less

  12. Engineering of a novel Ca{sup 2+}-regulated kinesin molecular motor using a calmodulin dimer linker

    SciTech Connect (OSTI)

    Shishido, Hideki; Maruta, Shinsaku

    2012-06-29

    Highlights: Black-Right-Pointing-Pointer Engineered kinesin-M13 and calmodulin involving single cysteine were prepared. Black-Right-Pointing-Pointer CaM mutant was cross-linked to dimer by bifunctional thiol reactive reagent. Black-Right-Pointing-Pointer Kinesin-M13 was dimerized via CaM dimer in the presence of calcium. Black-Right-Pointing-Pointer Function of the engineered kinesin was regulated by a Ca{sup 2+}-calmodulin dimer linker. -- Abstract: The kinesin-microtubule system holds great promise as a molecular shuttle device within biochips. However, one current barrier is that such shuttles do not have 'on-off' control of their movement. Here we report the development of a novel molecular motor powered by an accelerator and brake system, using a kinesin monomer and a calmodulin (CaM) dimer. The kinesin monomer, K355, was fused with a CaM target peptide (M13 peptide) at the C-terminal part of the neck region (K355-M13). We also prepared CaM dimers using CaM mutants (Q3C), (R86C), or (A147C) and crosslinkers that react with cysteine residues. Following induction of K355-M13 dimerization with CaM dimers, we measured K355-M13 motility and found that it can be reversibly regulated in a Ca{sup 2+}-dependent manner. We also found that velocities of K355-M13 varied depending on the type and crosslink position of the CaM dimer used; crosslink length also had a moderate effect on motility. These results suggest Ca{sup 2+}-dependent dimerization of K355-M13 could be used as a novel molecular shuttle, equipped with an accelerator and brake system, for biochip applications.

  13. Discovery of $^{34g,m}$Cl$(p,?)^{35}$Ar resonances activated at classical nova temperatures

    E-Print Network [OSTI]

    C. Fry; C. Wrede; S. Bishop; B. A. Brown; A. A. Chen; T. Faestermann; R. Hertenberger; A. Parikh; D. Pérez-Loureiro; H. -F. Wirth; A. García; R. Ortez

    2015-10-14

    Background: The thermonuclear $^{34g,m}$Cl($p,\\gamma$)$^{35}$Ar reaction rates are unknown due to a lack of experimental nuclear physics data. Uncertainties in these rates translate to uncertainties in $^{34}$S production in models of classical novae on oxygen-neon white dwarfs. $^{34}$S abundances have the potential to aid in the classification of presolar grains. Purpose: Determine resonance energies for the $^{34g,m}$Cl($p,\\gamma$)$^{35}$Ar reactions within the region of astrophyical interest for classical novae to a precision of a few keV as an essential first step toward constraining their thermonuclear reaction rates. Method: $^{35}$Ar excited states were populated by the $^{36}$Ar($d,t$)$^{35}$Ar reaction at $E$(d)=22~MeV and reaction products were momentum analyzed by a high resolution quadrupole-dipole-dipole-dipole (Q3D) magnetic spectrograph. Results: Seventeen new $^{35}$Ar levels have been detected at a statistically significant level in the region $E_x\\approx$~5.9-6.7~MeV ($E_r$ \\textless~800~ keV) and their excitation energies have been determined to typical uncertainties of 3~keV. The uncertainties for five previously known levels have also been reduced substantially. The measured level density was compared to those calculated using the WBMB Hamiltonian within the $sd-pf$ model space. Conclusions: Most of the resonances in the region of astrophyical interest have likely been discovered and their energies have been determined, but the resonance strengths are still unknown, and experimentally constraining the $^{34g,m}$Cl($p,\\gamma$)$^{35}$Ar reaction rates will require further experiments.

  14. Hubble space telescope investigation of main-belt comet 133P/Elst-Pizarro

    SciTech Connect (OSTI)

    Jewitt, David; Ishiguro, Masateru; Weaver, Harold; Agarwal, Jessica; Mutchler, Max; Larson, Steven

    2014-05-01

    We report new observations of the prototype main-belt comet (active asteroid) 133P/Elst-Pizarro taken at high angular resolution using the Hubble Space Telescope. The object has three main components: (1) a point-like nucleus; (2) a long, narrow antisolar dust tail; and (3) a short, sunward anti-tail. There is no resolved coma. The nucleus has a mean absolute magnitude H{sub V} = 15.70 ± 0.10 and a light curve range ?V = 0.42 mag, the latter corresponding to projected dimensions 3.6 × 5.4 km (axis ratio 1.5:1) at the previously measured geometric albedo of 0.05 ± 0.02. We explored a range of continuous and impulsive emission models to simultaneously fit the measured surface brightness profile, width, and position angle of the antisolar tail. Preferred fits invoke protracted emission, over a period of 150 days or less, of dust grains following a differential power-law size distribution with index 3.25 ?q ? 3.5 and with a wide range of sizes. Ultra-low surface brightness dust projected in the sunward direction is a remnant from emission activity occurring in previous orbits, and consists of the largest (?cm-sized) particles. Ejection velocities of one-micron-sized particles are comparable to the ?1.8 m s{sup –1} gravitational escape speed of the nucleus, while larger particles are released at speeds less than the gravitational escape velocity. The observations are consistent with, but do not prove, a hybrid hypothesis in which mass loss is driven by gas drag from the sublimation of near-surface water ice, but escape is aided by centripetal acceleration from the rotation of the elongated nucleus. No plausible alternative hypothesis has been identified.

  15. Evidence for heterogeneity in facioscapulohumeral muscular dystrophy (FSHD)

    SciTech Connect (OSTI)

    Gilbert, J.R.; Stajich, J.M.; Wall, S.; Carter, S.C.; Qiu, H.; Vance, J.M.; Stewart, C.S.; Speer, M.C.; Pufky, J.; Yamaoka, L.H.; Rozear, M.; Roses, A.D.; Pericak-Vance, M.A. (Duke Univ. Medical Center, Durham, NC (United States)); Samson, F.; Fardeau, M. (INSERM, Paris (France))

    1993-08-01

    Facioscapulohumeral muscular dystrophy (FSHD) is a slowly progressive primary disease of muscle which is usually inherited as an autosomal dominant disorder. FSHD has been localized to the long arm of chromosome 4, specifically to the 4q3.5-qter region. Initially published linkage studies showed no evidence for heterogeneity in FSHD. In the present study the authors have examined individuals in seven FSHD families. Two-point lod scores show significant evidence for linkage for D4S163 (lod score 3.04 at recombination fraction .21) and D4S139 (lod score 3.84 at recombination fraction .20). D4S171 also gave a positive score (lod score 2.56 at recombination fraction .24). Significant evidence for heterogeneity was found for each of the three markers. Multipoint linkage analysis in this region resulted in a peak multipoint lod score of 6.47. The multipoint analysis supported the two-point studies with odds of 20:1 showing linkage and heterogeneity over linkage and homogeneity. Five of the seven families gave a posterior probability of >95% of being of the linked type, while two families appeared unlinked to this region of 4q (P<.01%). Individuals in the two unlinked families met the clinical criteria for the diagnosis of FSHD, including facial weakness, clavicular flattening, scapula winging, proximal muscle weakness, and myopathic changes on muscle biopsies without inflammatory or mitochondrial pathology. This study demonstrates genetic heterogeneity in FSHD and has important implications for both genetic counseling and the elucidation of the etiology of FSHD. 19 refs., 3 figs., 2 tabs.

  16. High Resolution Infrared Spectra of the v2, v3, v4 and 2v3 Bands of 32S16O3

    SciTech Connect (OSTI)

    Maki, Arthur G.; Blake, Thomas A.; Sams, Robert L.; Vulpanovici, Nicolae; Barber, Jeffrey B.; Chrysostom, Engelene; Masiello, Tony; Nibler, Joseph W.; Weber, Alfons

    2001-09-14

    New measurements are reported for the infrared spectrum of sulfur trioxide, 32S16O3, with resolutions ranging from 0.0015 cm-1 to 0.0025 cm-1. New rovibrational constants have been measured for the fundamentals v2, v3, and v4, and the overtone band 2v3. Comparisons are made with the earlier high resolution measurements on SO3 and the high correlation among some of the constants related to the Coriolis coupling of the v2 and v4 levels is duscussed in order to understand the areas of disagreement with the arlier work. Splittings of some of the levels are observed and hte splitting constant for K = 3 of the ground state is determined for the first time. Other observed splittings include the K = 1 levels of 2v3 (I = 2), the K = 2 levels of the v3 and v4 states and the K = 3 levels of v2. This analysis shows that there are level corssings between the I = 0 and I = 2 states of 2v3 that allow one to determine the separation of the sub-band centers for those two states even thoug the I = o state is a dark state. This is a generalized phenomenon that should be found for many other molecules with the same symmetry. The I-type resonance constant that couples the I = 0 and 2 states is roughly the same as q3 which causes the splitting of the I = 1 levels of the v3 fundamental.

  17. High-pressure behavior and thermoelastic properties of niobium studied by in situ x-ray diffraction

    SciTech Connect (OSTI)

    Zou, Yongtao E-mail: yongtaozou6@gmail.com; Li, Baosheng; Qi, Xintong; Wang, Xuebing; Chen, Ting; Li, Xuefei; Welch, David

    2014-07-07

    In situ synchrotron energy dispersive x-ray diffraction (XRD) experiments on Nb have been conducted at pressures up to 6.4 GPa and temperatures up to 1073 K. From the pressure-volume-temperature measurements, thermoelastic parameters were derived for the first time for Nb based on the thermal pressure (?P{sub th}) equation of state (EOS), modified high-T Birch-Murnaghan EOS, and Mie-Grüneisen-Debye EOS. With the pressure derivative of the bulk modulus K{sub T}{sup ´} fixed at 4.0, we obtained the ambient isothermal bulk modulus K{sub T0}=174(5) GPa, the temperature derivative of bulk modulus at constant pressure (?K{sub T}/?T){sub P}=-0.060(8) GPa K?¹ and at constant volume (?K{sub T}/?T){sub V}=-0.046(8) GPa K?¹, the volumetric thermal expansivity ?{sub T}(T)=2.3(3)×10??+0.3(2)×10??T (K?¹), as well as the pressure dependence of thermal expansion (??/?P){sub T}=(?2.0±0.4)×10?? K?¹ GPa?¹. Fitting the present data to the Mie-Grüneisen-Debye EOS with Debye temperature ??=276.6 K gives ??=1.27(8) and K{sub T0}=171(3) GPa at a fixed value of q=3.0. The ambient isothermal bulk modulus and Grüneisen parameter derived from this work are comparable to previously reported values from both experimental and theoretical studies. An in situ high-resolution, angle dispersive XRD study on Nb did not indicate any anomalous behavior related to pressure-induced electronic topological transitions at ~5 GPa as has been reported previously.

  18. XCOM intrinsic dimensionality for low-Z elements at diagnostic energies

    SciTech Connect (OSTI)

    Bornefalk, Hans [Department of Physics, Royal Institute of Technology, SE-106 91 Stockholm (Sweden)

    2012-02-15

    Purpose: To determine the intrinsic dimensionality of linear attenuation coefficients (LACs) from XCOM for elements with low atomic number (Z = 1-20) at diagnostic x-ray energies (25-120 keV). H{sub 0}{sup q}, the hypothesis that the space of LACs is spanned by q bases, is tested for various q-values. Methods: Principal component analysis is first applied and the LACs are projected onto the first q principal component bases. The residuals of the model values vs XCOM data are determined for all energies and atomic numbers. Heteroscedasticity invalidates the prerequisite of i.i.d. errors necessary for bootstrapping residuals. Instead wild bootstrap is applied, which, by not mixing residuals, allows the effect of the non-i.i.d residuals to be reflected in the result. Credible regions for the eigenvalues of the correlation matrix for the bootstrapped LAC data are determined. If subsequent credible regions for the eigenvalues overlap, the corresponding principal component is not considered to represent true data structure but noise. If this happens for eigenvalues l and l + 1, for any l{<=}q, H{sub 0}{sup q} is rejected. Results: The largest value of q for which H{sub 0}{sup q} is nonrejectable at the 5%-level is q = 4. This indicates that the statistically significant intrinsic dimensionality of low-Z XCOM data at diagnostic energies is four. Conclusions: The method presented allows determination of the statistically significant dimensionality of any noisy linear subspace. Knowledge of such significant dimensionality is of interest for any method making assumptions on intrinsic dimensionality and evaluating results on noisy reference data. For LACs, knowledge of the low-Z dimensionality might be relevant when parametrization schemes are tuned to XCOM data. For x-ray imaging techniques based on the basis decomposition method (Alvarez and Macovski, Phys. Med. Biol. 21, 733-744, 1976), an underlying dimensionality of two is commonly assigned to the LAC of human tissue at diagnostic energies. The finding of a higher statistically significant dimensionality thus raises the question whether a higher assumed model dimensionality (now feasible with the advent of multibin x-ray systems) might also be practically relevant, i.e., if better tissue characterization results can be obtained.

  19. After runaway: The trans-Hill stage of planetesimal growth

    SciTech Connect (OSTI)

    Lithwick, Yoram [Department of Physics and Astronomy, Northwestern University, Evanston, IL 60208, USA and Center for Interdisciplinary Exploration and Research in Astrophysics (CIERA), Evanston, IL 60208 (United States)

    2014-01-01

    When planetesimals begin to grow by coagulation, they first enter an epoch of runaway, during which the biggest bodies grow faster than all the others. The questions of how runaway ends and what comes next have not been answered satisfactorily. We show that runaway is followed by a new stage—the 'trans-Hill stage'—that commences when the bodies that dominate viscous stirring ('big bodies') become trans-Hill, i.e., when their Hill velocity matches the random speed of the small bodies they accrete. Subsequently, the small bodies' random speed grows in lockstep with the big bodies' sizes, such that the system remains in the trans-Hill state. Trans-Hill growth is crucial for determining the efficiency of growing big bodies, as well as their growth timescale and size spectrum. Trans-Hill growth has two sub-stages. In the earlier one, which occurs while the stirring bodies remain sufficiently small, the evolution is collisionless, i.e., collisional cooling among all bodies is irrelevant. The efficiency of forming big bodies in this collisionless sub-stage is very low, ?10? << 1, where ? ? 0.005(a/AU){sup –1} is the ratio between the physical size of a body and its Hill radius. Furthermore, the size spectrum is flat (equal mass per size decade, i.e., q = 4). This collisionless trans-Hill solution explains results from previous coagulation simulations for both the Kuiper Belt and the asteroid belt. The second trans-Hill sub-stage commences once the stirring bodies grow big enough (>?{sup –1} × the size of the accreted small bodies). After that time, collisional cooling among small bodies controls the evolution. The efficiency of forming big bodies rises and the size spectrum becomes more top heavy. Trans-Hill growth can terminate in one of two ways, depending on the sizes of the small bodies. First, mutual accretion of big bodies can become significant and conglomeration proceeds until half of the total mass is converted into big bodies. This mode of growth may explain the observed size distributions of small bodies in the solar system and is explored in our subsequent work. Second, if the big bodies' orbits become separated by their Hill radius, oligarchy commences. This mode likely precedes the formation of fully fledged planets.

  20. Advanced, Low/Zero Emission Boiler Design and Operation

    SciTech Connect (OSTI)

    Babcock/Wilcox; Illinois State Geological; Worley Parsons; Parsons Infrastructure/Technology Group

    2007-06-30

    In partnership with the U.S. Department of Energy's National Energy Technology Laboratory, B&W and Air Liquide are developing and optimizing the oxy-combustion process for retrofitting existing boilers as well as new plants. The main objectives of the project is to: (1) demonstrate the feasibility of the oxy-combustion technology with flue gas recycle in a 5-million Btu/hr coal-fired pilot boiler, (2) measure its performances in terms of emissions and boiler efficiency while selecting the right oxygen injection and flue gas recycle strategies, and (3) perform technical and economic feasibility studies for application of the technology in demonstration and commercial scale boilers. This document summarizes the work performed during the period of performance of the project (Oct 2002 to June 2007). Detailed technical results are reported in corresponding topical reports that are attached as an appendix to this report. Task 1 (Site Preparation) has been completed in 2003. The experimental pilot-scale O{sub 2}/CO{sub 2} combustion tests of Task 2 (experimental test performance) has been completed in Q2 2004. Process simulation and cost assessment of Task 3 (Techno-Economic Study) has been completed in Q1 2005. The topical report on Task 3 has been finalized and submitted to DOE in Q3 2005. The calculations of Task 4 (Retrofit Recommendation and Preliminary Design of a New Generation Boiler) has been completed in 2004. In Task 6 (engineering study on retrofit applications), the engineering study on 25MW{sub e} unit has been completed in Q2, 2008 along with the corresponding cost assessment. In Task 7 (evaluation of new oxy-fuel power plants concepts), based on the design basis document prepared in 2005, the design and cost estimate of the Air Separation Units, the boiler islands and the CO{sub 2} compression and trains have been completed, for both super and ultra-supercritical case study. Final report of Task-7 is published by DOE in Oct 2007.

  1. Intergovernmental Advanced Stationary PEM Fuel Cell System Demonstration Final Report

    SciTech Connect (OSTI)

    Rich Chartrand

    2011-08-31

    A program to complete the design, construction and demonstration of a PEMFC system fuelled by Ethanol, LPG or NG for telecom applications was initiated in October 2007. Early in the program the economics for Ethanol were shown to be unfeasible and permission was given by DOE to focus on LPG only. The design and construction of a prototype unit was completed in Jun 2009 using commercially available PEM FC stack from Ballard Power Systems. During the course of testing, the high pressure drop of the stack was shown to be problematic in terms of control and stability of the reformer. Also, due to the power requirements for air compression the overall efficiency of the system was shown to be lower than a similar system using internally developed low pressure drop FC stack. In Q3 2009, the decision was made to change to the Plug power stack and a second prototype was built and tested. Overall net efficiency was shown to be 31.5% at 3 kW output. Total output of the system is 6 kW. Using the new stack hardware, material cost reduction of 63% was achieved over the previous Alpha design. During a November 2009 review meeting Plug Power proposed and was granted permission, to demonstrate the new, commercial version of Plug Power's telecom system at CERL. As this product was also being tested as part of a DOE Topic 7A program, this part of the program was transferred to the Topic 7A program. In Q32008, the scope of work of this program was expanded to include a National Grid demonstration project of a micro-CHP system using hightemperature PEM technology. The Gensys Blue system was cleared for unattended operation, grid connection, and power generation in Aug 2009 at Union College in NY state. The system continues to operate providing power and heat to Beuth House. The system is being continually evaluated and improvements to hardware and controls will be implemented as more is learned about the system's operation. The program is instrumental in improving the efficiency and reducing costs of PEMFC based power systems using LPG fuel and continues to makes steps towards meeting DOE's targets. Plug Power would like to thank DOE for their support of this program.

  2. Rapidly re-computable EEG (electroencephalography) forward models for realistic head shapes

    SciTech Connect (OSTI)

    Ermer, J. J.; Mosher, J. C.; Baillet, S.; Leahy, R. M.

    2001-01-01

    Solution of the EEG source localization (inverse) problem utilizing model-based methods typically requires a significant number of forward model evaluations. For subspace based inverse methods like MUSIC [6], the total number of forward model evaluations can often approach an order of 10{sup 3} or 10{sup 4}. Techniques based on least-squares minimization may require significantly more evaluations. The observed set of measurements over an M-sensor array is often expressed as a linear forward spatio-temporal model of the form: F = GQ + N (1) where the observed forward field F (M-sensors x N-time samples) can be expressed in terms of the forward model G, a set of dipole moment(s) Q (3xP-dipoles x N-time samples) and additive noise N. Because of their simplicity, ease of computation, and relatively good accuracy, multi-layer spherical models [7] (or fast approximations described in [1], [7]) have traditionally been the 'forward model of choice' for approximating the human head. However, approximation of the human head via a spherical model does have several key drawbacks. By its very shape, the use of a spherical model distorts the true distribution of passive currents in the skull cavity. Spherical models also require that the sensor positions be projected onto the fitted sphere (Fig. 1), resulting in a distortion of the true sensor-dipole spatial geometry (and ultimately the computed surface potential). The use of a single 'best-fitted' sphere has the added drawback of incomplete coverage of the inner skull region, often ignoring areas such as the frontal cortex. In practice, this problem is typically countered by fitting additional sphere(s) to those region(s) not covered by the primary sphere. The use of these additional spheres results in added complication to the forward model. Using high-resolution spatial information obtained via X-ray CT or MR imaging, a realistic head model can be formed by tessellating the head into a set of contiguous regions (typically the scalp, outer skull, and inner skull surfaces). Since accurate in vivo determination of internal conductivities is currently not currently possible, the head is typically assumed to consist of a set of contiguous isotropic regions, each with constant conductivity.

  3. Materials for Advanced Ultrasupercritical Steam Turbines Task 4: Cast Superalloy Development

    SciTech Connect (OSTI)

    Thangirala, Mani

    2015-09-30

    The Steam Turbine critical stationary structural components are high integrity Large Shell and Valve Casing heavy section Castings, containing high temperature steam under high pressures. Hence to support the development of advanced materials technology for use in an AUSC steam turbine capable of operating with steam conditions of 760°C (1400°F) and 35 Mpa (5000 psia), Casting alloy selection and evaluation of mechanical, metallurgical properties and castability with robust manufacturing methods are mandated. Alloy down select from Phase 1 based on producability criteria and creep rupture properties tested by NETL-Albany and ORNL directed the consortium to investigate cast properties of Haynes 282 and Haynes 263. The goals of Task 4 in Phase 2 are to understand a broader range of mechanical properties, the impact of manufacturing variables on those properties. Scale up the size of heats to production levels to facilitate the understanding of the impact of heat and component weight, on metallurgical and mechanical behavior. GE Power & Water Materials and Processes Engineering for the Phase 2, Task 4.0 Castings work, systematically designed and executed casting material property evaluation, multiple test programs. Starting from 15 lbs. cylinder castings to world’s first 17,000 lbs. poured weight, heavy section large steam turbine partial valve Haynes 282 super alloy casting. This has demonstrated scalability of the material for steam Turbine applications. Activities under Task 4.0, Investigated and characterized various mechanical properties of Cast Haynes 282 and Cast Nimonic 263. The development stages involved were: 1) Small Cast Evaluation: 4 inch diam. Haynes 282 and Nimonic 263 Cylinders. This provided effects of liquidus super heat range and first baseline mechanical data on cast versions of conventional vacuum re-melted and forged Ni based super alloys. 2) Step block castings of 300 lbs. and 600 lbs. Haynes 282 from 2 foundry heats were evaluated which demonstrated the importance of proper heat treat cycles for Homogenization, and Solutionizing parameters selection and implementation. 3) Step blocks casting of Nimonic 263: Carried out casting solidification simulation analysis, NDT inspection methods evaluation, detailed test matrix for Chemical, Tensile, LCF, stress rupture, CVN impact, hardness and J1C Fracture toughness section sensitivity data and were reported. 4) Centrifugal Casting of Haynes 282, weighing 1400 lbs. with hybrid mold (half Graphite and half Chromite sand) mold assembly was cast using compressor casing production tooling. This test provided Mold cooling rates influence on centrifugally cast microstructure and mechanical properties. Graphite mold section out performs sand mold across all temperatures for 0.2% YS; %Elongation, %RA, UTS at 1400°F. Both Stress-LMP and conditional Fracture toughness plots data were in the scatter band of the wrought alloy. 5) Fundamental Studies on Cooling rates and SDAS test program. Evaluated the influence of 6 mold materials Silica, Chromite, Alumina, Silica with Indirect Chills, Zircon and Graphite on casting solidification cooling rates. Actual Casting cooling rates through Liquidus to Solidus phase transition were measured with 3 different locations based thermocouples placed in each mold. Compared with solidification simulation cooling rates and measurement of SDAS, microstructure features were reported. The test results provided engineered casting potential methods, applicable for heavy section Haynes 282 castings for optimal properties, with foundry process methods and tools. 6) Large casting of Haynes 282 Drawings and Engineering FEM models and supplemental requirements with applicable specifications were provided to suppliers for the steam turbine proto type feature valve casing casting. Molding, melting and casting pouring completed per approved Manufacturing Process Plan during 2014 Q4. The partial valve casing was successfully cast after casting methods were validated with solidification simulation analysis and the casting met NDT inspection and a

  4. The pMSSM10 after LHC run 1

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

    de Vries, K. J.; Cavanaugh, R.

    2015-09-15

    We present a frequentist analysis of the parameter space of the pMSSM10, in which the following ten soft SUSY-breaking parameters are specified independently at the mean scalar top mass scale MSUSY ? $\\sqrt{m$\\tilde{t}$1m$\\tilde{t}$2}$ : the gaugino masses M1,2,3 , the first-and second-generation squark masses m$\\tilde{q}$1 = m$\\tilde{q}$2 , the third-generation squark mass m$\\tilde{q}$3, a common slepton mass m$\\tilde{?}$ and a common trilinear mixing parameter A , as well as the Higgs mixing parameter ? , the pseudoscalar Higgs mass MA and tan? , the ratio of the two Higgs vacuum expectation values. We use the MultiNest sampling algorithm with ?more »1.2 ×109 points to sample the pMSSM10 parameter space. A dedicated study shows that the sensitivities to strongly interacting sparticle masses of ATLAS and CMS searches for jets, leptons + E-slashT signals depend only weakly on many of the other pMSSM10 parameters. With the aid of the Atom and Scorpion codes, we also implement the LHC searches for electroweakly interacting sparticles and light stops, so as to confront the pMSSM10 parameter space with all relevant SUSY searches. In addition, our analysis includes Higgs mass and rate measurements using the HiggsSignals code, SUSY Higgs exclusion bounds, the measurements of BR(Bs??+?-) by LHCb and CMS, other B -physics observables, electroweak precision observables, the cold dark matter density and the XENON100 and LUX searches for spin-independent dark matter scattering, assuming that the cold dark matter is mainly provided by the lightest neutralino ?-tilde10 . We show that the pMSSM10 is able to provide a supersymmetric interpretation of (g-2)? , unlike the CMSSM, NUHM1 and NUHM2. As a result, we find (omitting Higgs rates) that the minimum ?2=20.5 with 18 degrees of freedom (d.o.f.) in the pMSSM10, corresponding to a ?2 probability of 30.8 %, to be compared with ?2/d.o.f.=32.8/24(31.1/23)(30.3/22) in the CMSSM (NUHM1) (NUHM2). We display the one-dimensional likelihood functions for sparticle masses, and we show that they may be significantly lighter in the pMSSM10 than in the other models, e.g., the gluino may be as light as ? 1250 GeV at the 68 % CL, and squarks, stops, electroweak gauginos and sleptons may be much lighter than in the CMSSM, NUHM1 and NUHM2. We discuss the discovery potential of future LHC runs, e+e- colliders and direct detection experiments.« less