Search results for "Proton Scattering"

showing 10 items of 3238 documents

"Table 6" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

PI- P --> P OMEGA PI-Integrated Cross SectionExclusiveCross Section4.839SIGPion-Proton Scattering
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"Table 2" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

PI- P --> P OMEGA PI-PI- P --> P PHI PI-Integrated Cross SectionExclusiveCross Section4.839SIGPion-Proton Scattering
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"Table 10" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

PI- P --> P OMEGA PI-PI- P --> P PHI PI-Integrated Cross SectionExclusiveCross Section4.839SIGPion-Proton Scattering
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"Table 8" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

PI- P --> P OMEGA PI-PI- P --> P PHI PI-Integrated Cross SectionExclusiveCross Section4.839SIGPion-Proton Scattering
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"Table 4" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

PI- P --> P PHI PI-Integrated Cross SectionExclusiveCross Section4.839SIGPion-Proton Scattering
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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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"Table 9" of "Inclusive double-helicity asymmetries in neutral pion and eta meson production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=200$ GeV"

2014

The best fit value of the gluon polarization where the uncertainty is that at a chi-squared value of 9 when considering only statistical experimental uncertainties.

POLInclusiveP P --> PI0 XProton-Proton ScatteringPolarizationHigh Energy Physics::Phenomenology200.0
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"Table 1" of "Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=…

2015

Transverse polarization POL of LAMBDA and LAMBDABAR hyperons averaged over PT and XF.

POLInclusiveProton-Proton ScatteringStrange productionPolarization7000.0P P --> LAMBDA X
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"Table 4" of "Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions…

2018

Expected allowed ranges for 8 dimensional aQGC, no cutoff).

Photon-Photon ScatteringP P --> H --> WW (exclusive)8000.0W Pair ProductionProton-Proton ScatteringAstrophysics::High Energy Astrophysical PhenomenaP P --> gamma gamma --> WWExclusiveCross SectionSIGDiffraction
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