Search results for "RHO0"

showing 6 items of 26 documents

"Table 6" of "Exclusive rho0 and phi muoproduction at large q**2"

1995

No description provided.

MUON NUCLEUS --> CA MUON RHO0GAMMA* NUCLEON --> RHO0 NUCLEONPhotoproductionIntegrated Cross SectionExclusiveMUON CA --> MUON RHO0 CACross SectionSIGMuon production19.393
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"Table 1" of "Phi, rho, and omega production in p U, O U and S U reactions at 200-GeV per nucleon"

1996

The cross sections are parametrized as A**POWER.

O U --> RHO0 XP NUCLEUS --> MU+ MU- XPOWERS U --> MU- MU+ XInclusiveO U --> PHI XCharged CurrentNUCLEUS NUCLEUS --> OMEGA XNUCLEUS NUCLEUS --> RHO0 XO U --> MU- MU+ XNUCLEUS NUCLEUS --> PHI XS U --> PHI XP U --> MU- MU+ XDi-Muon ProductionP U --> PHI XP U --> OMEGA XP NUCLEUS --> RHO0 XDeep Inelastic ScatteringO U --> OMEGA XS U --> RHO0 XMuon productionP U --> RHO0 XP NUCLEUS --> OMEGA XS U --> OMEGA XNUCLEUS NUCLEUS --> MU+ MU- XP NUCLEUS --> PHI X
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"Decay Phase-Space Volume of Partial Waves" of "Light isovector resonances in $\pi^- p \to \pi^-\pi^-\pi^+ p$ at 190 GeV/${\it c}$"

2018

Decay phase-space volume $I_{aa}$ for the 14 selected partial waves as a function of $m_{3\pi}$, normalized such that $I_{aa}(m_{3\pi} = 2.5~\text{GeV}/c^2) = 1$. The wave index $a$ represents the quantum numbers that uniquely define the partial wave. The quantum numbers are given by the shorthand notation $J^{PC} M^\varepsilon [$isobar$] \pi L$. We use this notation to label the decay phase-space volume in the column headers. The labels are identical to the ones used in the column headers of the table of the transition amplitudes. $I_{aa}$ is calculated using Monte Carlo integration techniques for fixed $m_{3\pi}$ values, which are given in the first column, in the range from 0.5 to 2.5 Ge…

PI- P --> PI2(2005)- PLight-Meson SpectroscopyIsobar ModelPI- P --> PI- F2(1270) PAmplitude AnalysisPI- P --> PI1(1600)- PDiffractivePI- P --> A1(1420)- PPI- P --> A1(1260)- PPI- P --> A2(1320)- PPI- P --> A1(1640)- PPI- P --> A4(2040)- PPI- P --> PI- RHO0 PPI- P --> PI- F0(980) PPI- P --> PI- PI- PI+ PPI- P --> PI2(1670)- PPI- P --> A2(1700)- PExclusivePI- P --> PI(1800)- PPI- P --> PI2(1880)- PPion-Proton Scattering
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"Transition Amplitudes" of "Light isovector resonances in $\pi^- p \to \pi^-\pi^-\pi^+ p$ at 190 GeV/${\it c}$"

2018

Real and imaginary parts of the normalized transition amplitudes $\mathcal{T}_a$ of the 14 selected partial waves in the 1100 $(m_{3\pi}, t')$ cells (see Eq. (12) in the paper). The wave index $a$ represents the quantum numbers that uniquely define the partial wave. The quantum numbers are given by the shorthand notation $J^{PC} M^\varepsilon [$isobar$] \pi L$. We use this notation to label the transition amplitudes in the column headers. The $m_{3\pi}$ values that are given in the first column correspond to the bin centers. Each of the 100 $m_{3\pi}$ bins is 20 MeV/$c^2$ wide. Since the 11 $t'$ bins are non-equidistant, the lower and upper bounds of each $t'$ bin are given in the column he…

PI- P --> PI2(2005)- PLight-Meson SpectroscopyIsobar ModelPI- P --> PI- F2(1270) PAmplitude AnalysisPI- P --> PI1(1600)- PDiffractivePartial-Wave AmplitudePI- P --> A1(1420)- PPI- P --> A1(1260)- PPI- P --> A2(1320)- PPI- P --> A1(1640)- PPI- P --> A4(2040)- PPI- P --> PI- RHO0 PPI- P --> PI- F0(980) PPI- P --> PI- PI- PI+ PPI- P --> PI2(1670)- PPI- P --> A2(1700)- PExclusive19.0PI- P --> PI(1800)- PPI- P --> PI2(1880)- PPion-Proton ScatteringAMP
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Measurement of inclusive production of light meson resonances in hadronic decays of the Z0

1993

A study of inclusive production of the meson resonances ρ0, K*0 (892), f{hook}0 (975) and f{hook}2 (1270) in hadronic decays of the Z0 is presented. The measured mean meson multiplicity per hadronic event is 0.83 ± 0.14 for the ρ0 0.64 ± 0.24 for the K*0 (892), 0.10 ± 0.04 for the f{hook}0 (975) in the momentum range p > 0.05pbeam (xp > 0.05) and 0.11 ± 0.05 for the f{hook}2 (1270) for xp > 0.1. These values and the corresponding differential cross sections ( 1 σhadr) dσ dxp for the vector mesons are in good agreement with the predictions of the JETSET 7.3 PS and HERWIG 5.4 models. The f{hook}2 (1270) production is overestimated by HERWIG but its xp-shape is correctly reproduced. T…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonLUND MONTE-CARLO010308 nuclear & particles physicsElectron–positron annihilationHadronE+E-ANNIHILATION01 natural sciencesJET FRAGMENTATIONK+P INTERACTIONSPHYSICSNuclear physicsGEV/C0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]RHO0Física nuclearMultiplicity (chemistry)010306 general physicsParticle Physics - ExperimentLUND MONTE-CARLO; E+E-ANNIHILATION; K+P INTERACTIONS; JET FRAGMENTATION; PHYSICS; GEV/C; RHO0Physics Letters B
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"Table 1" of "Search for exclusive charmless B meson decays with the DELPHI detector at LEP"

1995

Two body decay modes. Upper limits at 90% CL. In computing of limits the fractions of B/(d,u)(0,-) and B/S0 mesons were assumed to be 0.39 and 0.12 respectively. Limits are given for the weighted average of the decay rates of the two neutral B mesons.

SIG/SIGStrange productionB0 --> K+ PI-B- --> K- RHO0B/S --> K+ K-B- --> K*BAR(892)0 PI-Integrated Cross SectionB0 --> P PBARCross SectionB/S --> K+ A1(1270)-B0 --> K+ K-B/S --> K+ PI-B0 --> K+ A1(1270)-B- --> PHI K-E+ E- ScatteringE+ E- --> ZExclusiveHigh Energy Physics::ExperimentB0 --> PI+ PI-B- --> RHO0 PI-
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