| Sample search results for: 12-group gamma cross-sections |
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| 1 | Magnetic field mapping of the Belle solenoid N. Tan a M. Akatsu b A. Bozek c;2 K. Fujimoto b J. Haba c;1 | ||
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Summary: ,800 mm length @ 4:5 ffi K 3,910 mm Conductor cross section 3 2 33mm 2 winding pitch 3.3 mm Electrical No... (m) SCALE QCSR \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma... \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma ... |
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Source: BELLE Collaboration |
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Collection: Physics |
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| 2 | Fermilab-Pub-01/057-E Search for First-Generation Scalar and Vector Leptoquarks | ||
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Summary: pair-production cross section as a function of mass and of #12;, the branching fraction to a charged... channels are #12; 2 , 2#12;(1 #12;), and (1 #12;) 2 , respec- tively. The cross section for p#22;p ! LQ LQ... of the pair-production cross section of scalar ... |
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Source: Fermi National Accelerator Laboratory, DØ Experiment |
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Collection: Physics |
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| 3 | The Upgraded D Detector D Collaboration | ||
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Summary: environment. The length 11 #12; Fig. 2. Crosssectional view of the new central tracking system in the x - z... then assembled into a disk/barrel central module or one of the threedisk 18 #12; Fig. 8. Cross section |
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Source: Fermi National Accelerator Laboratory, DØ Experiment |
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Collection: Physics |
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| 4 | 1995 PARTIAL UPDATE TO THE REVIEW OF PARTICLE PROPERTIES* or J=/(3097) | ||
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Summary: the integrated cross section into channel I in the e + e \Gamma annihilation. \Gamma \Gamma hadrons \Delta \Theta... \Gamma (1 \Gamma \Gamma ) J=/(1S) MASS J=/(1S) MASS J=/(1S) MASS J=/(1S) MASS VALUE (MeV) EVTS DOCUMENT... + ... |
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Source: Fermilab, E835 Experiment Charmonium |
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Collection: Physics |
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| 5 | Evaluating the Impact of Advanced Memory Systems on CompilerParallelized Codes | ||
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Summary: .0 0.5 1.0 1.5 2.0 \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma... \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma... ... |
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Source: Martonosi, Margaret - Department of Electrical Engineering, Princeton University |
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Collection: Computer Technologies and Information Sciences |
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| 6 | Memory Referencing Behavior in CompilerParallelized Applications | ||
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Summary: affects the performance 5 #12; 0.0 0.5 1.0 1.5 2.0 \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma... \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma... ... |
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Source: Martonosi, Margaret - Department of Electrical Engineering, Princeton University; Tseng, Chau-Wen - Department of Computer Science, University of Maryland at College Park |
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Collection: Computer Technologies and Information Sciences |
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| 7 | Evaluating the Impact of Advanced Memory Systems on CompilerParallelized Codes | ||
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Summary: .0 0.5 1.0 1.5 2.0 \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma... \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma... ... |
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Source: Tseng, Chau-Wen - Department of Computer Science, University of Maryland at College Park |
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Collection: Computer Technologies and Information Sciences |
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| 8 | Categories, Allegories and Circuit Design Carolyn Brown | ||
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Summary: of the picture constructors. 1 A picture is either ffl the picture C: A ! B of a cell C \Lambda \Gamma \Gamma... \Gamma \Gamma \Gamma \Gamma \Gamma \Gamma \Gamma \Gamma ... |
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Source: Hutton, Graham - School of Computer Science, University of Nottingham |
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Collection: Computer Technologies and Information Sciences |
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| 9 | 1995 PARTIAL UPDATE TO THE REVIEW OF PARTICLE PROPERTIES* \Gamma \Gamma | ||
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Summary: from the integrated cross section into channel I in the e + e \Gamma annihilation. We list only data... 1995 PARTIAL UPDATE TO THE REVIEW OF PARTICLE PROPERTIES* \Gamma \Gamma fl fl \Delta /\Gamma total... \Gamma 2 /\Gamma ... |
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Source: Fermilab, E835 Experiment Charmonium |
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Collection: Physics |
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| 10 | Parity Violating Asymmetries: Definitions (tentative !) | ||
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Summary: a b + oe \Gamma a b ) unpolarized cross section : oe 0 0 = 1 4 ( oe \Gamma\Gamma + oe ++ + oe... a ) a 0 b 0 (a 0 = 1 2 (a a + a \Gamma a )) Then, we have an ``experimental'' cross section : oe a 0... ... |
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Source: Ohta, Shigemi - Theory Group, Institute of Particle and Nuclear Studies, High Energy Accelerator Research Organization (KEK) |
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Collection: Physics |
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| 11 | \Gamma\Gamma \Gamma\Gamma | ||
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Summary: 60 50 40 30 20 10 0 \Gamma\Gamma \Gamma\Gamma \Gamma\Gamma \Gamma\Gamma \Gamma\Gamma \Gamma\Gamma... \Gamma\Gamma \Gamma\Gamma \Gamma\Gamma \Gamma\Gamma ... |
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Source: Laske, Gabi - Institute of Geophysics and Planetary Physics, Scripps Institution of Oceanography |
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Collection: Geosciences |
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| 12 | Vol. 30 (1999) ACTA PHYSICA POLONICA B No 7 REVIEW ON NEUTRINO OSCILLATIONS | ||
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Summary: recoilless elastic scattering of hadrons against the heavy nuclei in the emul- sion (white-kinks). The cross-section... 800 ¯m VERTEX PLATE measured track segment ø \Gamma ø NON ZERO IMPACT PARAMETER SB ¯ \Gamma tracker... predictions ¯ ZERO IMPACT PARAMETER SB ¯ \Gamma tracker predictions Fig. ... |
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Source: Magiera, Andrzej - Instytut Fizyki, Uniwersytet Jagiellonski |
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Collection: Physics |
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| 13 | Characterizing the Memory Behavior of CompilerParallelized Applications | ||
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Summary: ) have significant inter 9 #12; \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma... \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma... ... |
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Source: Tseng, Chau-Wen - Department of Computer Science, University of Maryland at College Park |
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Collection: Computer Technologies and Information Sciences |
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| 14 | Characterizing the Memory Behavior of CompilerParallelized Applications | ||
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Summary: ; \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma... \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma... ... |
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Source: Martonosi, Margaret - Department of Electrical Engineering, Princeton University |
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Collection: Computer Technologies and Information Sciences |
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| 15 | Integrated Optical Circulator based on Radiatively Coupled Magnetooptic Waveguides | ||
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Summary: coupled waveguides. Cross sections perpendicular to the direction of propagation z are shown. Guiding... , magnetooptic isolator, magnetooptic circulator #12; \Gamma \Gamma \Gamma \Gamma \Gamma \Gamma ... |
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Source: Hammer, Manfred - Department of Applied Mathematics, Universiteit Twente |
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Collection: Mathematics |
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| 16 | Review of Rare and Forbidden Decays Department of Physics, The Ohio State University, Columbus, OH 43210, U.S.A. | ||
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Summary: may be resolved soon with a higher precision measurement of the ß + ß \Gamma j cross section expected... vector current. The predictions for the rate [6,7] estimated using the measured cross section for e + e... decays, this includes new results on the chiral anomaly decay ø ... |
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Source: Gan, K. K. - Department of Physics, Ohio State University |
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Collection: Physics |
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| 17 | restrictive conjunction | ||
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Summary: and LEP2 with ALEPH and L3 looking at production of ßß and KK final states, measuring total cross section... National Laboratory Upton, NY The CLEO experiment at the e + e \Gamma collider CESR has obtained evidence... , 95% of 4ß solid angle coverage. (oe E=E)% = 0:35=E 0:75 + 1:9 \Gamma 0:1E. ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 18 | New Results on Rare Decays Department of Physics, The Ohio State University, Columbus, OH 43210, U.S.A. | ||
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Summary: fractions are also related to the cross section for e + e \Gamma ! 6ß by the ConservedVectorCurrent (CVC... to the e + e \Gamma crosssection or any axialvector contribution to the ø de cay through an j... frac tion to be small from CVC due to the relatively small measured ... |
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Source: Gan, K. K. - Department of Physics, Ohio State University |
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Collection: Physics |
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| 19 | GROUP EXTENSION HOMOMORPHISM MATRICES A. M. DuPr' e | ||
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Summary: (y \Gamma1 ; y) \Gamma1 \Lambda oe(y \Gamma1 ; y) y = (t ffi s 0 )(y) : #12; GROUP EXTENSION HOMOMORPHISM... of functions, and recover f from this matrix. We also investigate the dependence of the matrix on the crosssections... ; y 2 ))s(y 1 y 2 ) : Proof. Apply t ... |
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Source: DuPre, Art - Department of Mathematics and Computer Science, Rutgers University at Newark |
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Collection: Mathematics |
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| 20 | hepex/9910070 New experimental data for the decays OE ! + \Gamma and | ||
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Summary: ! ¯ + ¯ \Gamma and OE ! ß + ß \Gamma give interference patterns in the energy dependences of the cross sections... of the interference amplitude, m OE ; \Gamma OE -- mass and width of OE meson. Nonresonant cross section was taken... 1000 ... |
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Source: Budker Institute of Nuclear Physics, Spherical Neutral Detector Group |
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Collection: Fission and Nuclear Technologies |
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| 21 | Belle Prerpint 20043 KEK Preprint 2003119 | ||
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Summary: (\Lambda)\Gamma crosssections T. Uglov, 10 K. Abe, 6 K. Abe, 37 T. Abe, 6 H. Aihara, 39 M. Akatsu, 18 Y... threshold. The cross sections for e + e \Gamma ! D \Lambda+ T D \Lambda\Gamma L and e + e \Gamma ! D + D... 0:03 \Sigma 0:06 pb, ... |
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Source: BELLE Collaboration |
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Collection: Physics |
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| 22 | Proseminar/Seminar Quantum Computing | ||
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Summary: Proseminar/Seminar Quantum Computing \Gamma \Gamma \Gamma @ @ @ @ @ @ \Gamma \Gamma \Gamma \Gamma... \Gamma \Gamma \Gamma \Gamma \Gamma ... |
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Source: Grassl, Markus - Institut für Algorithmen und Kognitive Systeme, Universität Karlsruhe |
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Collection: Computer Technologies and Information Sciences |
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| 23 | Quantenalgorithmen \Gamma \Gamma @ | ||
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Summary: Seminar Quantenalgorithmen \Gamma \Gamma \Gamma @ @ @ @ @ @ \Gamma \Gamma \Gamma \Gamma \Gamma... \Gamma \Gamma \Gamma \Gamma ... |
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Source: Grassl, Markus - Institut für Algorithmen und Kognitive Systeme, Universität Karlsruhe |
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Collection: Computer Technologies and Information Sciences |
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| 24 | Userlevel Checkpointing for LinuxThreads Programs \Lambda William R. Dieter and James E. Lumpp, Jr. | ||
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Summary: Checkpoint Thread time Running outside signal handler Running in signal handler Blocked \Gamma\Gamma\Gamma\Gamma... \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma \Gamma\Gamma\Gamma\Gamma\Gamma... \Gamma\Gamma\Gamma\Gamma\Gamma ... |
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Source: Dieter, William R. - Department of Electrical and Computer Engineering, University of Kentucky |
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Collection: Engineering |
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| 25 | CLNS 01/1762 Understanding B Meson Branching Fractions | ||
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Summary: [1], and the measurement of the electromagnetic production cross section, e + e \Gamma ! \Upsilon(1S) and e + e \Gamma... ! \Upsilon(2S), in 1978 at the DORIS storage ring of DESY[2]. From the magnitude of these crosssections... This is a discussion of the main branching fractions of B ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 26 | Top quark : Discovery and What's New ffl Last year's D results | ||
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Summary: -- New optimized cuts #12; Top Cross Section: ffl Luminosity of ß 100 pb \Gamma1 ffl Cuts optimized... to minimize cross section error ffl Seven channels considered in analysis: -- Di--lepton + 2 jets (e¯; ee... Background of 13:4 \Sigma 3:0 Expected Signal of 21:2 \Sigma 3:8 (180 GeV ... |
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Source: Gerber, Cecilia E. - Department of Physics, University of Illinois at Chicago |
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Collection: Physics |
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| 27 | JavaCard Program Veri cation Bart Jacobs | ||
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Summary: Mag., 2001. To appear. \Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma... ... |
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Source: Jacobs, Bart - Institute for Computing and Information Sciences, Radboud Universiteit Nijmegen |
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Collection: Computer Technologies and Information Sciences |
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| 28 | CLNS 03/1837 Primer on Onium Widths | ||
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Summary: . Note that in eq. 5 the units of cross section \Theta energy are taken to be MeV \Gamma1 rather than cm... M ) 2 +\Gamma 2 =4 , thereby distorting slightly the shape of the resonant cross section. However... radiation cross ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 29 | Generalized Eigenfunction Expansion Near Resonances Roger Waxler | ||
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Summary: that scattering cross sections have the expected BreitWigner peaks near the resonances. 1 #12; Introduction 1... parameter. The BreitWigner peaks refer to peaks in the scattering cross sections again of the form const... cross sections jff(k)j 2 and jfi(k)j 2 ... |
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Source: Mathematical Physics Preprint Archive |
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Collection: Mathematics |
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| 30 | hepph/0012257 High energy photonneutrino elastic scattering | ||
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Summary: in the forward direction to the total cross section for the process fl !W + e \Gamma as \Gamma 1 s ImA (` = 0... powers of m 2 e =m 2 W . The spin aver aged cross section (oe + + oe \Gamma )=2 agrees with the result... Im A++ (` = 0)=s ... |
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Source: Repko, Wayne - Department of Physics and Astronomy, Michigan State University |
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Collection: Physics |
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| 31 | Particle Physics Detectors, Decay Widths, and Cross Sections | ||
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Summary: Particle Physics Detectors, Decay Widths, and Cross Sections Problem Set 2 Due:Thursday, Feb. 11... '', then the cross section would have the form of the ``BreitWigner''. Problem 5 In PRL 74, 4376... it as necessary for these problems. Consider the decay K 0 (1270) ! K \Lambda+ (892)ß ... |
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Source: Johnson, Randy - Physics Department, University of Cincinnati |
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Collection: Physics |
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| 32 | hepex/9910057 NEW DATA FROM SND DETECTOR IN NOVOSIBIRSK | ||
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Summary: patterns in the cross sections of e + e \Gamma ! !ß and e + e \Gamma ! ß + ß \Gamma processes. The Born... 1 \Gamma Z m OE \Gamma OE D OE (E) fi fi fi fi 2 ; where oe 0 (E) is nonresonant cross section, ... |
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Source: Budker Institute of Nuclear Physics, Spherical Neutral Detector Group |
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Collection: Fission and Nuclear Technologies |
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| 33 | THE GAP BETWEEN COMPLEX STRUCTURED SINGULAR VALUE AND ITS UPPER BOUND IS | ||
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Summary: ] and is defined as follows ¯(A) : = i inffk\Deltak : \Delta is diagonal, I \Gamma M \Delta is not invertibleg j... \Gamma1 = i inffk\Deltak : \Delta is diagonal, I \Gamma \DeltaM is not invertibleg j \Gamma1 Here... \Deltak : I \Gamma G\Delta is not invertibleg (let us remind the reader ... |
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Source: Treil, Sergei - Department of Mathematics, Brown University |
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Collection: Mathematics |
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| 34 | EPJ manuscript No. (will be inserted by the editor) | ||
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Summary: on a reanalysis of the measured cross section for e + e \Gamma ! ß + ß \Gamma , with a more proper treatment... on the measured cross section for e + e \Gamma ! 4ß. More precise measurements of the branching ratio and cross... B(ø ... |
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Source: Gan, K. K. - Department of Physics, Ohio State University |
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Collection: Physics |
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| 35 | Undercompressive Shocks for a System of Hyperbolic Conservation Laws with Cubic Nonlinearity | ||
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Summary: , with viscosity and capillarity terms in cluded, are: u t \Gamma v x = 0 v t \Gamma oe(u) x = fflv xx \Gamma ffl... 2 Au xxx : (1.1) In this system, u = u(x; t) represents the longitudinal strain at time t at a cross... section of a rod located at position x, and v = v(x; t) is the ... |
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Source: North Carolina State University, Center for Research in Scientific Computation |
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Collection: Computer Technologies and Information Sciences |
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| 36 | Flow from a Tank Consider water flowing from a tank with water through a hole in its bottom. Denote | ||
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Summary: at time t, A(h) the crosssectional area of the tank at height h and a the cross sectional area... )dt. So the volume of water that has left the tank in this time interval h(t) h(t + dt) volume A \Gamma h... (t) \Delta [h(t) \Gamma h(t + dt)] volume a v(t) dt is essentially A ... |
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Source: Feldman, Joel - Department of Mathematics, University of British Columbia |
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Collection: Mathematics |
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| 37 | Global pathfollowing of homoclinic orbits in twoparameter flows | ||
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Summary: for both t ! +1 and t ! \Gamma1, (1.2) A \Sigma := lim t!\Sigma1 h(t), A+ 6= A \Gamma . The limits... are equilibria of (1.1), by invariance of !limit sets. If A+ = A \Gamma , then h(t) is called a homoclinic orbit... \Gamma ) `` W s (A+ ). See, for example, [Chow & Hale] (1982), [Arnol'd] (1992), ... |
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Source: Fiedler, Bernold - Fachbereich Mathematik und Informatik & Institut für Mathematik, Freie Universität Berlin |
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Collection: Mathematics |
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| 38 | Inhaltsverzeichnis 1 Einleitung 5 | ||
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Summary: .1) ! plus(\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma\Gamma... ... |
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Source: Siekmann, Jörg H. - Deutsche Forschungszentrum für Künstliche Intelligenz |
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Collection: Computer Technologies and Information Sciences |
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| 39 | MSUHEP70723 hepph/9707448 | ||
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Summary: to the Higgs production cross section via the gluon fusion mechanism. #12; 1 Introduction The Higgs Boson H... available. Moreover, these amplitudes are necessary for a full NNLO calculation of the cross section... of the total crosssection in this limit. Acknowledgements We would like ... |
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Source: Schmidt, Carl - Department of Physics and Astronomy, Michigan State University |
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Collection: Physics |
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| 40 | pCROSSSECTION BODIES R. J. GARDNER AND A. A. GIANNOPOULOS | ||
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Summary: , its crosssection body CK has a radial function in any direction u 2 S n\Gamma1 equal to the maximal... body in E n , its crosssection body CK has a radial function in any direction u 2 S n\Gamma1 equal... be a convex body in E n . We define the pcrosssection body C p K of K for ... |
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Source: Giannopoulos, Apostolos - Department of Mathematics, University of Athens |
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Collection: Mathematics |
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| 41 | arXiv:hepex/0010077 RECENT RESULTS FROM SND DETECTOR AT VEPP2M | ||
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Summary: . In the energy range 2E 0 = 1:0 \Xi 1:4 GeV the cross sections of the processes e + e \Gamma ! !ß 0 and e + e... + e \Gamma ! ß 0 ß 0 fl cross section is shown in Fig. 4. The fit of the cross section included ae; ae... ... |
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Source: Budker Institute of Nuclear Physics, Spherical Neutral Detector Group |
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Collection: Fission and Nuclear Technologies |
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| 42 | Technische Universitat ChemnitzZwickau Sonderforschungsbereich 393 | ||
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Summary: of the cross section of an electronic motor the magnetic field computation must be calculated in. The following... (e) air gap ¯ r = 1 Figure 7: The fourthcross section of the electronic motor containing 4 materials... By means of Maxwell's laws the magnetic field problem defined on motor's ... |
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Source: Chemnitz, Technische Universität - Fakultaet fuer Mathematik, Numerische Simulation auf massiv parallelen Rechnern |
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Collection: Computer Technologies and Information Sciences |
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| 43 | Energy Conduction Band Shallow Traps | ||
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Summary: = free carrier density J = current density E = electrostatic field SD = photoexcitation crosssection... for donors ST = photoexcitation crosssection for shallow traps fl D ; fl T = recombination rate for donor... . The equations governing the aformentioned process are @N i D @t = SD I(ND \Gamma N i D ) ... |
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Source: Gander, Martin J. - Section de Mathématiques, Université de Genève |
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Collection: Mathematics |
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| 44 | LU TP 99--39 December 10, 1999 | ||
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Summary: 4 treats the crosssection of e + e \Gamma ! e + e \Gamma PS, where PS is ß 0 , j or j 0 , and how... : Diagram contributing to the cross section for e + e \Gamma ! PS e + e \Gamma . 16 #12; e + 2 (p e + 2 ) e... ; ffl 4 ) Figure 11: Second ... |
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Source: Lunds Universitet, - Computational Biology and Biological Physics Group |
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Collection: Physics ; Biology and Medicine |
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| 45 | Atomic Data for Astrophysics. II. New Analytic Fits for Photoionization Cross Sections of Atoms and Ions | ||
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Summary: the threshold) cross section maximum, and \Gamma 1 = y 1 E 0 is an `energy width' of this maximum. Similarly, (x... the energy position of the cross section minimum (dip), and \Gamma 2 = y w E 0 can be treated as the `dip... energy width'. The fit parameter P ... |
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Source: Verner, Dima - Department of Physics and Astronomy, University of Kentucky |
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Collection: Physics |
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| 46 | ENTROPY DISSIPATION AND LONGRANGE INTERACTIONS R. ALEXANDRE, L. DESVILLETTES, C. VILLANI, AND B.WENNBERG | ||
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Summary: , and collision crosssections that satisfy B(v \Gamma v \Lambda ; oe) \Phi(jv \Gamma v \Lambda j)b(k \Delta oe... of the Boltzmann collision operator with a crosssection given by (7) seems to be the requirement Z S N \Gamma1 b... dissipation functional D(g; f) = ... |
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Source: Ecole Normale Supérieure de Cachan, Centre de mathématiques et de leurs applications |
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Collection: Mathematics |
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| 47 | \Gamma ! K + K \Gamma \Gamma at CLEO III Feng Liu a \Lambda | ||
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Summary: includes the uncertain ties from the ø pair cross section (1%), the inte grated luminosity (2%) and MC... 1 ø \Gamma ! K + K \Gamma ß \Gamma ø at CLEO III Feng Liu a \Lambda a On behalf of the CLEO... Collaboration SMU Group, Wilson Lab, Cornell University, Ithaca, NY 14853, ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 48 | CLNS 05/1939 Measurement of oe(e + e \Gamma ! /(3770) ! hadrons) at E cm = 3773 MeV | ||
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Summary: ! /(3770) ! D ¯ D cross section at the same energy is found to be (\Gamma0:01 \Sigma 0:08 +0:41 \Gamma0... :30 ) nb. With the observed total cross section, we extract \Gamma ee (/(3770)) = (0:204 \Sigma 0:003 +0... section ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 49 | LU TP 9529 Ratios of strange antibaryons to baryons | ||
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Summary: and the limited knowledge of the relevant cross sections. Recently the NA36 collaboration has published... . There are 195 inelastic reactions involved altogether. The cross section of ßß ! K ¯ K is taken to be 2.0 mb... as usual [11]. The isospin averaged parametrization of Ref.12 is adopted for the ... |
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Source: Lunds Universitet, - Computational Biology and Biological Physics Group |
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Collection: Physics ; Biology and Medicine |
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| 50 | Charm Meson Hadroproduction Mithat Kaya | ||
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Summary: Particle effect : The leading particle has a larger differential crosssection than non leading one. D... 2. The E781(SELEX) Apparatus 3. Charm Selection Criteria 4. D s Mass Distribution from \Sigma \Gamma... t distributions ffl Differential production asymmetries for \Sigma \Gamma beam 6. Summary and Conclusions Mithat |
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Source: Fermi National Accelerator Laboratory - SELEX (Segmented Large X baryon Spectrometer) |
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Collection: Physics |
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| 51 | GROUP EXTENSION ENDOMORPHISM COORDINATES A. M. DuPr' e | ||
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Summary: a short exact sequence 1 ! N i \Gamma! G j \Gamma! H ! 1 of groups, together with a crosssection s : H... ! H : Then #12; GROUP EXTENSION ENDOMORPHISM COORDINATES 3 Theorem 1.1. The f ij satisfy the following... . #12; GROUP EXTENSION ... |
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Source: DuPre, Art - Department of Mathematics and Computer Science, Rutgers University at Newark |
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Collection: Mathematics |
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| 52 | RADIATIVE WIDTH OF THE a 2 MESON. The SELEX Collaboration 1 | ||
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Summary: measurement of the (ß + ß \Gamma ß \Gamma ) coherent cross section using SELEX data. Figure 2: The radiative... it pos sible to explore the features of the Primakoff reaction. The differential cross section... section for the reaction (1) in ... |
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Source: Fermi National Accelerator Laboratory - SELEX (Segmented Large X baryon Spectrometer) |
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Collection: Physics |
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| 53 | arXiv:hepex/0009036 Processes e + e \Gamma ! K + K \Gamma , K S KL and + \Gamma 0 at the OE(1020) | ||
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Summary: The cross sections of the processes e + e \Gamma ! K + K \Gamma , e + e \Gamma ! KSKL and e + e \Gamma ! ß... \Gamma ! ß + ß \Gamma ß 0 reaction cross section. I. INTRODUCTION The ... |
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Source: Budker Institute of Nuclear Physics, Spherical Neutral Detector Group |
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Collection: Fission and Nuclear Technologies |
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| 54 | ON A SEMICONDUCTOR MODEL INCLUDING RECOMBINATION VIA DISTRIBUTED TRAPS* | ||
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Summary: . The given functions oe n = oe n (E) and oe(E; E 0 ) are scattering cross sections, M = M(E) = exp ` \Gamma E... \Gamma Ev kT \Delta , the scattering cross sections oe n and oe by ¯nUT =L 2 and ¯nUT =(L 2 ~ C) exp... and the cross ... |
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Source: Schmeiser, Christian - Fakultät für Mathematik, Universität Wien |
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Collection: Mathematics |
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| 55 | CALCULATIONS OF NUCLEAR REACTIONS OF ASTROPHYSICAL INTEREST INVOLVING UNSTABLE NUCLEI | ||
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Summary: if the half--lives are of the order of 1 s or longer, the cross sections of nuclear reactions can be measured... ) in calculating cross sections at the border and far--off the region of stability. #12; 2 Direct capture... .g. 8) for neutron capture by neutron--rich nuclei). The Direct Capture (DC) ... |
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Source: Rauscher, Thomas - Institut für Physik, Universität Basel |
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Collection: Physics |
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| 56 | estimates for the spatially homogeneous Boltzmann equation | ||
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Summary: on the regularity property of the gain term of the collision operator. 2. When the cross section is not a product... ) : they hold only in fact for the symmetrized cross section B sym defined above). Recalling that v 0 = v + v... kernel 5 #12; Proposition 2.1. Let B be a cross ... |
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Source: Ecole Normale Supérieure de Cachan, Centre de mathématiques et de leurs applications |
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Collection: Mathematics |
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| 57 | JOURNAL DE PHYSIQUE Colloque C6, suppl&mentau no 11-12, Tome 32, Novembre-Dkcembre 1971, page C6-265 HEAVY ION REACTION CHANNELS DETERMINED | ||
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Summary: . activation analysis to the determination of cross sections. From its decay curve and energy, the 634keV gamma... were observed, only one was used to extract the cross section. This gamma ray is given in Column 4... transition occurs) used to obtain the ... |
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Source: Ecole Polytechnique, Centre de mathématiques |
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Collection: Mathematics |
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| 58 | NEW RESULTS FROM CLEOII ON HADRONIC DECAYS OF THE TAU LEPTON | ||
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Summary: vector states, production of nonstrange vector states can be related to low energy e + e \Gamma crosssections... :6 GeV, with a ¸ 0:91 nb cross section. Since the turnon of CLEOII in late 1989, CESR has delivered... ß \Gamma ß 0 decay width to the isovector contribution to ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 59 | EUROPEAN ORGANISATION FOR NUCLEAR RESEARCH CERNPPE/96098 | ||
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Summary: The differential crosssections for e + e \Gamma ! e + e \Gamma , e + e \Gamma ! ¯ + ¯ \Gamma and e + e \Gamma ! ø... + ø \Gamma , and the total crosssection for e + e \Gamma ! q¯q at ... |
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Source: OPAL Experiment at Large Electron Positron Collider (LEP), CERN |
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Collection: Plasma Physics and Fusion |
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| 60 | Arch Beam Models: Finite Element Analysis and Superconvergence | ||
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Summary: and moment inertia of the cross section A and I, respectively, and shear correction factor k. It is easy... Fundation grant CCR8820279. 1 #12; arch is described by the rotation of the crosssection... to see that A=I = O(t \Gamma2 ). For simplicity we assume that the arch is clamped at both ends. We use |
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Source: Zhang, Zhimin - Department of Mathematics, Wayne State University |
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Collection: Mathematics |
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| 61 | David Cinabro Wayne State University | ||
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Summary: , Belle, BES. Take advantage of the enhanced cross sections at threshold and the clean- liness of e + e... ELC UKQCD Stech ISGW BBD WSB LMMS r 2 r V 24 #12; Protons Colliders Cross section huge, but tough... + B \Gamma production at the \Upsilon (4S). We have attempted to bring older ... |
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Source: Cinabro, David - Department of Physics and Astronomy, Wayne State University |
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Collection: Physics |
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| 62 | THEORETICAL NEUTRONCAPTURE CROSS SECTIONS FOR RPROCESS NUCLEOSYNTHESIS IN THE 48 CA REGION | ||
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Summary: ) . With this level information we updated the theoretical cross sections of the eveneven isotopes of 40\Gamma44 S... THEORETICAL NEUTRONCAPTURE CROSS SECTIONS FOR RPROCESS NUCLEOSYNTHESIS IN THE 48 CA REGION T... Abstract: We calculate neutron capture cross ... |
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Source: Rauscher, Thomas - Institut für Physik, Universität Basel |
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Collection: Physics |
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| 63 | JOURNAL OF LIGHTWAVE TECHNOLOGY 15(6) 983{989 (1997) 1 Analysis of power-dependent switching between | ||
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Summary: with the same value #31; of the nonlinear coeÆcient . The variation of the refractive index in the cross-section... directional coupler," J. Opt. Soc. Amer. A 9, 2258-2264 (1992) #12; Figure 1 \Gamma \Gamma \Gamma \Gamma... \Gamma \Gamma ... |
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Source: Hammer, Manfred - Department of Applied Mathematics, Universiteit Twente |
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Collection: Mathematics |
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| 64 | A Note on the Hybridmixed C 0 Curved Beam Zhimin Zhang \Lambda | ||
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Summary: correction factor, A and I are area and moment of inertia of the crosssection, respectively. In this case... mixed formulation Consider a circular arch element c having a singlysymmetric (with respect to yaxis) cross... section of thickness t, radius R and length l as shown in Fig.1. HellingerReissner functional is \Pi ... |
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Source: Zhang, Zhimin - Department of Mathematics, Wayne State University |
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Collection: Mathematics |
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| 65 | LU TP 9413 hepph/9410244 | ||
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Summary: . The phasespace limits are \Gamma1 x B ! x 1 ! \Gamma1; (24) 1 + x 1 ! x 2 ! 1: (25) 5 #12; The crosssection... and one throughout the physical phasespace. The crosssection is then doe = C F ff s 2ß d\Gamma 2 xB xp f... s z p (1 \Gamma z p )Q 2 n x 2 p (x 2 ... |
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Source: Lunds Universitet, - Computational Biology and Biological Physics Group |
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Collection: Physics ; Biology and Medicine |
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| 66 | D Run delivered recorded Run 1A 23 pb \Gamma1 15 pb \Gamma1 | ||
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Summary: V \Delta(E)=E = 7% #12; Tests of QCD ffl Jets -- Inclusive Jet Cross Section -- Dijet Mass Spectrum... and Angular Distribution -- Rapidity Gaps ffl Photons ffl W + Jet #12; Inclusive Jet Cross Section jjj ! 0... 400 450 Good agreement with NLO QCD for 35 ! E T ! 470 GeV #12; Inclusive Jet ... |
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Source: Gerber, Cecilia E. - Department of Physics, University of Illinois at Chicago |
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Collection: Physics |
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| 67 | Nuclear cross sections for gamma ray deexcitation line production by secondary neutrons | ||
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Summary: Nuclear cross sections for gamma ray deexcitation line production by secondary neutrons... sections from a few to >200 MeV. Using these cross sections, we also demonstrate the sensitivity of gamma... : Murphy, R. J., B. Kozlovsky, and G. H. ... |
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Source: Share, Gerald - Department of Astronomy, University of Maryland at College Park |
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Collection: Physics |
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| 68 | DIFFRACTION SCATTERING AT HIGH ENERGIES (outlook from 1980s) 1 | ||
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Summary: (t = 0) (from the Coulomb interference region), and the total cross section oe tot ß \Gamma p from... ; Fig. 2. Differential cross sections of ß \Gamma p elastic scattering at 250 GeV/c. Solid curve... s--1970s, the study of the hadronic total ... |
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Source: Titov, Anatoly - Laboratory of Molecular Beams, Petersburg Nuclear Physics Institute |
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Collection: Physics |
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| 69 | PARTICLE DATA GROUP NOTES PDG--93--04 19 October 1993 | ||
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Summary: max =2m e (maximum kinetic energy transfer) The form factor multiplies the cross section given... \Gamma Q 2 \Delta = m 2 ae m 2 ae +Q 2 ; where m ae = 0:77 GeV : Calculation: s = m 2 ß +m 2 e + 2m e E ß... (lab) Q 2 max = s \Gamma 2 \Gamma m 2 ß +m 2 e \Delta + ... |
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Source: Lawrence Berkeley National Laboratory, Computational Research Division, Distributed Systems Department, Data Intensive Distributed Computing Group |
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Collection: Computer Technologies and Information Sciences |
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| 70 | EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH CERNPPE/97110 | ||
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Summary: of the coupling of a meson to two photons, \Gamma flfl , and the Q 2 dependence of the formation cross section... 3 leads to a proportionality relation between the measured cross section and the twophoton width \Gamma... reduces nonresonant ß + ß ... |
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Source: CERN - European Organization for Nuclear Research, L3 High Energy Physics Experiment |
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Collection: Physics |
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| 71 | Measurement of the F 2 structure function in deep inelastic e + p scattering using 1994 data | ||
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Summary: . `Minimum bias' photoproduction events were simulated using PYTHIA [24] with cross sections according... of the kinematic region covered by the experiment. At Q 2 ! 35 GeV 2 the range in x now spans 6:3 \Delta 10 \Gamma5... below 10 \Gamma2 . Extensions of these measurements to low Q 2 have shown that this ... |
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Source: DESY, Deutsches Elektronen-Synchrotron in Hamburg |
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Collection: Physics |
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| 72 | Absolute cross sections for electronimpact single ionization of Ne q+ (q = 2,46) ions | ||
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Summary: ) for the four ions discussed in this paper, but his results overestimate the peak cross sections by 30 \Gamma 50... the cross section by 10 \Gamma 15% near the peak, but agrees well with the measurements near threshold... Absolute cross ... |
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Source: Controlled Fusion Atomic Data Center (CFADC) |
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Collection: Plasma Physics and Fusion |
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| 73 | CLNS 03/1838 Onium Line Shape Fitting | ||
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Summary: the resonance, measuring the cross section for hadronic final states. The dependence of the observed cross... of higher order virtual radiative processes on the overall scale of the cross section (see ref. [2]) G ffi... it to the observed cross ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 74 | Group Classification and Representations of Invariant Solutions | ||
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Summary: by the full Boltzmann kinetic equation with arbitrary differential cross section and by the EGD... ) is a differential scattering cross section, dw denotes an volume element of R 3 v , dn is a surface element of unit... . For arbitrary cross section oe there is the ... |
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Source: Meleshko, Sergey V. - School of Mathematics, Suranaree University of Technology |
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Collection: Mathematics |
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| 75 | CLNS 06/1952 Charmonium Decays of Y (4260), /(4160), and /(4040) | ||
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Summary: (4260) ! K + K \Gamma J=/ (3:7oe). We measure e + e \Gamma crosssections at p s = 4:26 GeV as oe(ß + ß... :8 \Gamma0:7 eV. It is located quite unexpectedly at a local minimum of the hadronic crosssection. Since... in opencharm crosssection and a hypothesized ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 76 | arXiv:hepph/0004225 Nonextensive statistical mechanics and particle spectra | ||
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Summary: for differential cross sections that are in very good agreement with e + e \Gamma annihilation experiments. 1... . The differential cross section oe \Gamma1 doe=dp T is expected to be proportional to w(p T ). 5 Large p... cross ... |
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Source: Beck, Christian - School of Mathematical Sciences, Queen Mary, University of London |
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Collection: Mathematics |
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| 77 | EUROPEAN LABORATORY FOR PARTICLE PHYSICS CERNPPE/97116 | ||
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Summary: for an integrated luminosity of 10.36 pb \Gamma1 . The W + W \Gamma production crosssection is measured to be oe WW... direct reconstruction and from the W + W \Gamma production cross sections measured at p s ¸ 161 and p... of approximately 30--40 MeV. The mass ... |
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Source: OPAL Experiment at Large Electron Positron Collider (LEP), CERN |
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Collection: Plasma Physics and Fusion |
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| 78 | DESY 93139 SCIPP 93/35 | ||
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Summary: corrected cross section to the largey Born cross section, K = doe(minijet) dyd¯y OE doe(large \Gamma y) dyd... rapidities we approach the Born cross section (4) with f(y; p 1? ; p 2? ) ! ffi(p 2 1? \Gamma p 2 2? )ffi... , ... |
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Source: Schmidt, Carl - Department of Physics and Astronomy, Michigan State University |
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Collection: Physics |
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| 79 | CLNS 04/1899 Study of Decays to FourHadron Final States with Kaons | ||
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Summary: similarly. These include the uncertainty in integrated luminosity (2%), øpair crosssection (1%), charged... at the Cornell Elec tron Storage Ring (CESR) using (7:56 \Sigma 0:15) fb \Gamma1 of data collected near... the \Upsilon(4S) resonance. We present the first statistically significant measurements of B(ø \Gamma ! K |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 80 | Diffusion Approximation of Radiative Transfer Problems with Guillaume Bal \Lambda Leonid Ryzhik y | ||
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Summary: be also taken into account. The differential scattering cross section oe(x; k; k 0 ) is explicitly given... keep the same notation for the scattering cross section after the change of variables: oe(x; ¯; ¯ 0... distance between two successive collisions, becomes small. We denote it by ''. The scattering ... |
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Source: Ryzhik, Lenya - Department of Mathematics, University of Chicago |
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Collection: Mathematics |
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| 81 | astroph/9509083 Astrophysical Journal Supplement Series, in press | ||
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Summary: & Dalgarno 1962) from the photoionization cross sections known in early seventies; for many species... , extrapolations of the cross sections #12; -- 2 -- along isoelectronic sequences were necessary due to lack... photoionization cross sections from the ground ... |
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Source: Verner, Dima - Department of Physics and Astronomy, University of Kentucky |
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Collection: Physics |
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| 82 | ENERGY CALIBRATION OF THE SUDBURY NEUTRINO OBSERVATORY USING MONOENERGETIC GAMMARAY SOURCES | ||
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Summary: Cross Section . . . . . . . . . . . . 53 3.3.2 A Survey of the Astrophysical S... many input parameters and functions: solar age, solar luminosity, nuclear cross sections, initial... the nuclear cross sections and the elemental abundances within their ranges of ... |
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Source: Waltham, Chris - Department of Physics and Astronomy, University of British Columbia |
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Collection: Physics |
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| 83 | Interesting Interesting | ||
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Summary: 5 10 15 20 25 ¡(4S) Dataset: ffl 3.3 M B ¯ B ffl 4.8 M c¯ c ffl 3.9 M ø + ø \Gamma \Gamma \Gamma\Gamma... E j EB \Gamma Ebeam ß 0 ffl Beamconstrained mass: =) Use Ebeam to calculate mass, instead of EB . ffl... tried to separate !ß + from !K + ffl ! ! ß + ß \Gamma ß 0 ffl ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 84 | I. DEFINITIONS AND GENERAL FORMULAS Here are the basic formulas. My apologies in advance that I don't guarantee the overall | ||
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Summary: the Golden Rule formula W = 2ß X f jhf jvjiij 2 ffi(E f \Gamma E i ) The differental scattering cross section... . Differential cross section: doe d\Omega = jf j 2 (1) Relation between scattering amplitude and phase shifts: f... 0 i = V 0 k; k 0 ! \Lambda = 0 otherwise Let us first ... |
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Source: Bertsch George F. - Department of Physics, University of Washington at Seattle |
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Collection: Physics |
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| 85 | Search for the pentaquark via the cs ! K \Lambda0 K \Gamma p decay | ||
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Summary: for the ratio of cross section times branching fraction of this de cay relative to that for the decay D \Gamma... momentum (x F ) peaks near zero. Estimated pen taquark production cross sections range between 10 \Gamma4... \Gamma K + ß ... |
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Source: Fermi National Accelerator Laboratory - Experiment E791 |
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Collection: Physics |
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| 86 | Particle Physics Detectors, Decay Widths, and Cross Sections | ||
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Summary: Particle Physics Detectors, Decay Widths, and Cross Sections Problem Set 2 Due: Tuesday, Feb. 8... . Show that if the matrix element was proportional to this ``propagator'', then the cross section would... for these problems. Consider the decay K 0 (1270) ! K \Lambda+ (892)ß \Gamma ! K 0 ... |
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Source: Johnson, Randy - Physics Department, University of Cincinnati |
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Collection: Physics |
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| 87 | Pointwise Semiclassical Asymptotics for Total Cross Sections in Nbody Problems | ||
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Summary: Pointwise Semiclassical Asymptotics for Total Cross Sections in Nbody Problems Didier ROBERT... direction, of total cross sections with initial twocluster channels in Nbody problems. 1 INTRODUCTION... The total scattering cross section is a physically important ... |
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Source: Wang, Xue Ping - Laboratoire de Mathématiques Jean Leray, Univeristé de Nantes |
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Collection: Mathematics ; Physics |
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| 88 | Physics with the Initial State Radiation Events at Bfactory Experiments X. C. Lou a , T. L. Benninger a and W. M. Dunwoodie b | ||
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Summary: and the e + e \Gamma !¯¯ cross section, oe ¯¯ (s 0 ). #12; 2 A narrow resonance with mass MR has a spin... averaged BreitWigner production cross section oe(s 0 ) = F 3ß s 0 \Gamma ee \Gamma 0 ( p s 0 \Gamma MR ) 2... ... |
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Source: Lou, XinChou - Department of Physics, University of Texas at Dallas |
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Collection: Physics |
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| 89 | Coincidence CT cross-section (based on MCNP model) of a canister containing | ||
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Summary: Coincidence CT cross-section (based on MCNP model) of a canister containing Uranium cylinder... and a poly rod. Confocal coded aperture gamma camera with 103 104 improved collection efficiency over... equivalent pinhole camera. Fourier camera demonstrator for terrestrial gamma imaging applications. Imaging |
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Source: Oak Ridge National Laboratory, Engineering Science and Technology Division, Image Science and Machine Vision Group |
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Collection: Engineering |
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| 90 | CLNS 05/1923 TimeIndependent Measurements of D 0 D 0 Mixing and Relative | ||
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Summary: , the relationship between the observed f N C \Gamma , which is used to obtain the D 0 D 0 cross section... of the luminosity or D 0 D 0 production cross section) [46], us 7 #12; TABLE III: D 0 D 0 DT branching fractions... to quantum correlations in the Codd and Ceven D 0 D 0 pairs ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 91 | Volume 12, No. 1 (2003), pp. 95--115 Allerton Press, Inc. M A TH E M A TIC A L M E TH O D S O F STA TISTIC S | ||
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Summary: cross sections (x i ; \Delta) ae S carry out n=m(n) sequential observations to recover f(x i ). (For... to justify this!) The choice of the observation points in each crosssection is governed by the sequential... of the crosssections (x k ; \Delta) ae S, using n=m(n) observations. This is followed by ... |
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Source: Levit, Boris - Department of Mathematics and Statistics, Queen's University (Kingston) |
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Collection: Mathematics |
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| 92 | EUROPEAN LABORATORY FOR PARTICLE PHYSICS CERNEP/98108 | ||
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Summary: Collaboration Abstract Crosssections for hadronic, bb and lepton pair final states in e + e \Gamma collisions... with at least one W decaying hadronically. All crosssections except those for e + e \Gamma have been corrected... . Values for bb production are given in the text. ... |
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Source: OPAL Experiment at Large Electron Positron Collider (LEP), CERN |
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Collection: Plasma Physics and Fusion |
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| 93 | PHYSICS RESULTS FROM SELEX G.D.Alkhazov, N.K.Terentyev, A.A.Vorobyov | ||
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Summary: beams, the \Lambda + c lifetime, the total cross sections for interaction of ß \Gamma ; \Sigma \Gamma... collaboration has measured the total cross sections oe tot (ß \Gamma Be), oe tot (ß \Gamma C), oe tot (ß ... |
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Source: Titov, Anatoly - Laboratory of Molecular Beams, Petersburg Nuclear Physics Institute |
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Collection: Physics |
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| 94 | Ann. Probab. 22 (1994), 180--194. DOMINATION BETWEEN TREES AND APPLICATION TO | ||
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Summary: , the notation D=(x 1 ; : : : ; x k ) is used for the crosssection of D given by f(x k+1 ; : : : ; x n ) 2 IR n... time. For a tree in which each vertex at distance n \Gamma 1 from the root has f(n) offspring, f... nondecreasing, an explosion occurs with exponentially distributed passage times if and only if P f(n) \Gamma1 |
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Source: Peres, Yuval - Department of Statistics, University of California at Berkeley |
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Collection: Mathematics |
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| 95 | DOMINATION BETWEEN TREES AND APPLICATION TO AN EXPLOSION PROBLEM | ||
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Summary: , the notation D=(x 1 ; : : : ; x k ) is used for the crosssection of D given by f(x k+1 ; : : : ; x n ) 2 IR n... . For a tree in which each vertex at distance n \Gamma 1 from the root has f(n) offspring, f nondecreasing... , an explosion occurs with exponentially distributed passage times if and only if P f(n) \Gamma1 ! 1. ... |
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Source: Pemantle, Robin - Department of Mathematics, University of Pennsylvania |
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Collection: Mathematics |
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| 96 | CLNS 97/1497 Study of the Decay \Gamma ! 2 \Gamma + 3 0 | ||
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Summary: and to the cross section for e + e \Gamma ! 6ß by the Conserved VectorCurrent (CVC) hypothesis. The decay can... component of the hadronic weak vector current so any I = 0 contribution to the e + e \Gamma crosssection... ! Luminosity 1 1 Crosssection 1 1 ø ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 97 | CLNS 97/1497 CLEO CONF 9704 | ||
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Summary: ß + ß 0 ø and ø \Gamma ! ß \Gamma 5ß 0 ø by isospin symmetry and to the cross section for e + e... vector current so any I = 0 contribution to the e + e \Gamma crosssection or any axial... . Summary of systematic errors (%). Mode 2ß ... |
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Source: Cornell University, Floyd R. Newman Laboratory of Nuclear Studies (LNS) |
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Collection: Physics |
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| 98 | Gauge Theories & Particle Physics Physics 539 Spring Semester 1997 Chris Quigg | ||
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Summary: \Gamma is formed as an schannel resonance. 24. (a) Compute the cross section for the reaction e + e... ? (c) Write the cross section for the reaction e + e \Gamma ! all in the form oe(e + e \Gamma ! H) = 4ß\Gamma... number ... |
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Source: Quigg, Chris - Theoretical Physics, Fermi National Accelerator Laboratory |
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Collection: Physics |
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| 99 | Easy to use software package for comprehensive modeling of nucleEasy to use software package for comprehensive modeling of nuclear reactions using variousar reactions using various theoretical formalisms. Consists of a number of FORTRAN codes, itheoretica | ||
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Summary: for inelastic scattering · Particle and gamma-spectra · Cross sections for discrete gamma transitions... and calculated excitation functions, angular distributions and double differential cross sections · GUI assisted... and reaction cross ... |
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Source: Brookhaven National Laboratory, Environmental Chemistry Division, Department of Applied Science |
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Collection: Environmental Sciences and Ecology |
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| 100 | SELFSIMILAR FLUID DYNAMIC LIMITS FOR THE BROADWELL SYSTEM | ||
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Summary: is the cross section for binary collisions. #12; 2 For flows which are independent of y; z and for which f 3... by the system of partial differ ential equations @f 1 @t + c @f 1 @x = oe(f 3 f 4 + f 5 f 6 \Gamma 2f 1 f 2... ) ; @f 2 @t \Gamma c @f 2 @x = oe(f 3 f 4 + f 5 f 6 \Gamma 2f 1 ... |
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Source: Tzavaras, Athanasios E. - Department of Applied Mathematics, University of Crete |
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Collection: Mathematics |
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