Search results for "Dependence"
showing 10 items of 2462 documents
"Table 2" of "Multiplicity dependence of charged pion, kaon, and (anti)proton production at large transverse momentum in p-Pb collisions at $\mathbf{…
2016
pT-differential invariant yield of charged pions in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV, measured for NSD events. The first uncertainty is statistical, the second one is the total systematic uncertainty, while the third one is the uncorrelated systematic uncertainty which is multiplicity dependent.
"Table 50" 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 PB 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 51" 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 PB target in the angular range 1.35 to 1.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 46" 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 PB target in the angular range 0.35 to 0.55 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 47" 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 PB target in the angular range 0.55 to 0.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 48" 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 PB target in the angular range 0.75 to 0.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 54" 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 PB target in the angular range 1.95 to 2.15 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 53" 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 PB target in the angular range 1.75 to 1.95 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 52" 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 PB target in the angular range 1.55 to 1.75 radians.. The errors are the square root of the diagonal elements of the covariant matrix.
"Table 49" 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 PB 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.