Search results for "Physics::Accelerator Physics"
showing 10 items of 1235 documents
"Table 4" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"
2009
Differential cross section for PI+ production with a C target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 14" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"
2009
Differential cross section for PI- production with a C target in the angular range 1.15 to 1.35 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 13" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"
2009
Differential cross section for PI- production with a C target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 48" 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 proton beam and Copper 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.
"Table 45" 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 proton beam and Copper 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.
"Table 47" 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 proton beam and Copper 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.
"Table 46" 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 proton beam and Copper 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.
"Table 22" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"
2009
Differential cross section for PI+ production with a TA target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 31" of "Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets"
2009
Differential cross section for PI- production with a TA target in the angular range 0.95 to 1.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 23" of "Centrality dependence of Pi, K, p production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV"
2018
pT-differential invariant yield of proton and antiproton for centrality 10-20%.