Search results for "Cross Section"

showing 10 items of 3111 documents

"Table 3" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

PI+ P --> P PHI PI+6.198Integrated Cross SectionExclusiveCross SectionSIGPion-Proton Scattering
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"Table 9" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

PI+ P --> P PHI PI+6.198Integrated Cross SectionExclusivePI+ P --> P OMEGA PI+Cross SectionSIGPion-Proton Scattering
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"Table 7" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

PI+ P --> P PHI PI+6.198Integrated Cross SectionExclusivePI+ P --> P OMEGA PI+Cross SectionSIGPion-Proton Scattering
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"Table 1" of "First observation of strong OZI rule violation in pi N interactions."

1996

No description provided.

PI+ P --> P PHI PI+6.198Integrated Cross SectionExclusivePI+ P --> P OMEGA PI+Cross SectionSIGPion-Proton Scattering
researchProduct

"Table 25" of "Measurements of Forward Proton Production with Incident Protons and Charged Pions on Nuclear Targets at the CERN Proton Synchroton"

2010

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

PI- AL --> P XInclusive0.501.00Nuclear TheoryD2SIG/DP/DOMEGAPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentDouble Differential Cross Section
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"Table 28" of "Measurements of Forward Proton Production with Incident Protons and Charged Pions on Nuclear Targets at the CERN Proton Synchroton"

2010

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

PI- AL --> P XInclusive0.501.00Nuclear TheoryD2SIG/DP/DOMEGAPhysics::Accelerator PhysicsNuclear ExperimentDouble Differential Cross Section
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"Table 27" of "Measurements of Forward Proton Production with Incident Protons and Charged Pions on Nuclear Targets at the CERN Proton Synchroton"

2010

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

PI- AL --> P XInclusive0.501.00Nuclear TheoryD2SIG/DP/DOMEGAPhysics::Atomic and Molecular ClustersPhysics::Accelerator PhysicsNuclear ExperimentDouble Differential Cross Section
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"Table 26" of "Measurements of Forward Proton Production with Incident Protons and Charged Pions on Nuclear Targets at the CERN Proton Synchroton"

2010

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

PI- AL --> P XInclusive0.501.00Nuclear TheoryD2SIG/DP/DOMEGAPhysics::Atomic and Molecular ClustersPhysics::Accelerator PhysicsNuclear ExperimentDouble Differential Cross Section
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"Table 2" of "Production properties of D0, D+, D*+ and D(s)+ in 230-GeV/c pi- and K- Cu interactions"

1992

Data fitted with the form d2sig/dxdpt**2 alpha ((1-x)**N)* EXP(-B*PT**2) using combined maximum likelihood fit to the invariant mass spectrum and the x and pt**2 distributions. The values for N and B are given here. Additional systematic errors are 10 pct for N and 3 pct for B.

PI- CU --> D*(2010)+ XPI- CU --> D/S- XStrange productionPI- CU --> D*(2010)- XPI- CU --> D/S+ XDSIG/DXLPI- CU --> D+ XPI- CU --> DBAR0 XInclusiveSingle Differential Cross SectionPI- NUCLEUS --> CHARM XPI- NUCLEUS --> CHARMBAR XCharm productionPI- CU --> D- XPI- CU --> D0 XDSIG/DPT**22.300E+022.300E+02Transverse Momentum Dependence
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"Table 1" of "Production properties of D0, D+, D*+ and D(s)+ in 230-GeV/c pi- and K- Cu interactions"

1992

Data fitted with the form d2sig/dxdpt**2 alpha ((1-x)**N)* EXP(-B*PT**2) using combined maximum likelihood fit to the invariant mass spectrum and the x and pt**2 distributions. The values for N and B are given here. Additional systematic errors are 10 pct for N and 3 pct for B.

PI- CU --> D*(2010)+ XPI- CU --> D/S- XStrange productionPI- CU --> D*(2010)- XPI- CU --> D/S+ XDSIG/DXLPI- CU --> D+ XPI- CU --> DBAR0 XInclusiveSingle Differential Cross SectionPI- NUCLEUS --> CHARM XPI- NUCLEUS --> CHARMBAR XCharm productionPI- CU --> D- XPI- CU --> D0 XDSIG/DPT**22.300E+022.300E+02Transverse Momentum Dependence
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