Search results for "160.0"
showing 10 items of 140 documents
"Table 10" of "Experimental investigation of transverse spin asymmetries in muon-p SIDIS processes: Sivers asymmetries"
2013
The Sivers asymmetry, from the 2010 data set, for negative hadrons as a function of PT for x > 0.032. Also shown are the mean values of other variables plus the correlation with the Collins data measurments.
"Table 2" of "Experimental investigation of transverse spin asymmetries in muon-p SIDIS processes: Sivers asymmetries"
2013
The Sivers asymmetry, from the 2010 data set, for negative hadrons as a function of X for full range. Also shown are the mean values of other variables plus the correlation with the Collins data measurments.
"Table 6" of "Experimental investigation of transverse spin asymmetries in muon-p SIDIS processes: Sivers asymmetries"
2013
The Sivers asymmetry, from the 2010 data set, for negative hadrons as a function of Z for full range. Also shown are the mean values of other variables plus the correlation with the Collins data measurments.
"Table 4" of "Experimental investigation of transverse spin asymmetries in muon-p SIDIS processes: Sivers asymmetries"
2013
The Sivers asymmetry, from the 2010 data set, for negative hadrons as a function of PT for full range. Also shown are the mean values of other variables plus the correlation with the Collins data measurments.
"Table 3" of "Search for collectivity with azimuthal J/$\psi$-hadron correlations in high multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 …
2017
$v_2^{J/\psi}${2,sub} in bins of $p_T^{J/\psi}$ for p-Pb collisions in proton-going direction at $\sqrt{s_{NN}}$ = 8.16 TeV. The quoted global systematic uncertainties correspond to the combined statistical and systematic uncertainties of the measured $v_2^{tracklet}$ coefficient. The results are obtained by subtracting associated per-trigger yields in low-multiplicity (40-100% V0M) collisions from the yields in high-multiplicity (0-20% V0M) collisions.
"Table 4" of "Search for collectivity with azimuthal J/$\psi$-hadron correlations in high multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 …
2017
$v_2^{J/\psi}${2,sub} in bins of $p_T^{J/\psi}$ for p-Pb collisions in Pb-going direction at $\sqrt{s_{NN}}$ = 8.16 TeV. The quoted global systematic uncertainties correspond to the combined statistical and systematic uncertainties of the measured $v_2^{tracklet}$ coefficient. The results are obtained by subtracting associated per-trigger yields in low-multiplicity (40-100% V0M) collisions from the yields in high-multiplicity (0-20% V0M) collisions.
"Table 10" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"
2020
$\Upsilon$(1S) $R_{\rm pPb}$ as a function of $p_{\rm T}$ at backward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
"Table 11" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"
2020
$\Upsilon$(1S) $R_{\rm pPb}$ as a function of $p_{\rm T}$ at forward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
"Table 9" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"
2020
$\Upsilon$(1S) $R_{\rm pPb}$ as a function of $y_{\rm {cms}}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.
"Table 1" of "Inclusive $\Upsilon$ production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV"
2020
$\Upsilon$(1S) differential cross section as a function of $y_{\rm cms}$, in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, while the second is the systematic.