Search results for "nucleus nucleus"
showing 10 items of 80 documents
"Table 2" of "Evidence for collective expansion in light-particle emission following Au+Au collisions at 100, 150 and 250 A��MeV"
2015
No description provided.
"Table 3" of "Evidence for collective expansion in light-particle emission following Au+Au collisions at 100, 150 and 250 A��MeV"
2015
No description provided.
"Table 5" of "Evidence for collective expansion in light-particle emission following Au+Au collisions at 100, 150 and 250 A��MeV"
2015
No description provided.
"Table 4" of "Evidence for collective expansion in light-particle emission following Au+Au collisions at 100, 150 and 250 A��MeV"
2015
No description provided.
"Table 6" of "Evidence for collective expansion in light-particle emission following Au+Au collisions at 100, 150 and 250 A��MeV"
2015
No description provided.
"Figure 3.1" of "Measurements of Higher-Order Flow Harmonics in Au+Au Collisions at sqrt(s_NN) = 200 GeV"
2020
Charged hadron azimuthal anisotropy $v_4$ vs centrality in Au+Au collisions at 200 GeV. The corresponding Npart value to each centrality is shown in Fig.3.2.
"Figure 3.2" of "Measurements of Higher-Order Flow Harmonics in Au+Au Collisions at sqrt(s_NN) = 200 GeV"
2020
Npart in each centrality bin in Au+Au collisions at 200 GeV.
"Table 4" of "Transverse momentum of J / psi produced in oxygen uranium collisions at 200-GeV per nucleon."
1996
D(SIG)/D(PT) is parameterized as PT*exp(-SLOPE*PT**CONST).
"Table 3" of "Transverse momentum of J / psi produced in oxygen uranium collisions at 200-GeV per nucleon."
1996
D(SIG)/D(PT) is parameterized as PT*exp(-SLOPE*PT**CONST).
"Table 1" of "Transverse momentum of J / psi produced in oxygen uranium collisions at 200-GeV per nucleon."
1996
Two parametrization of the D(SIG)/D(PT) are used: first is : PT*exp(-SLOPE*PT**CONST(C=PT)) and second is : PT*exp(-2*MT/CONST(C=MT)).