Search results for "200"

showing 10 items of 5058 documents

"Figure 2c" of "Measurement of Transverse Single-Spin Asymmetries for J/psi Production in Polarized p+p Collisions at sqrt(s) = 200 GeV"

2023

Transverse single-spin asymmetry of $J/\psi$ mesons plotted against $J/\psi$ transverse momentum. Systematic uncertainties $\delta$$A^f_N$ Type B and $\delta$$A^P_N$ Type B are due to the geometric scale factor and the polarization, respectively.

ppg103transverse momentum$p$ $p$ --> $J/\psi$200.0
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"Figure 3" of "Nuclear modification of psi^prime, chi_c and J/psi production in d+Au collisions at sqrt(s_NN) = 200 GeV"

2023

The $\psi^{\prime}$ nuclear modification factor, $R_{dAu}$, as a function of $N_{coll}$. Also included is the previously measured $J/\psi$ $R_{dAu}$ as a function of $N_{coll}$.

ppg151nuclear modification$\psi^\prime$ suppressionmidrapidity200.0$d$ Au --> CHARGED X
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"Figure 2" of "Nuclear modification of psi^prime, chi_c and J/psi production in d+Au collisions at sqrt(s_NN) = 200 GeV"

2023

The $\psi^{\prime}$, $\chi_c$, and $J/\psi$ $R_{dAu}$ for minimum bias centrality integrated $d$+Au collisions as a function of the quarkonia binding energy, where $J/\psi$ $R_{dAu}$ has been corrected for the effects of $\psi^{\prime}$ and $\chi_c$ feed-down.

ppg151nuclear modification$\psi^\prime$ suppressionmidrapidity200.0$d$ Au --> CHARGED X
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"Figure 4" of "Nuclear modification of psi^prime, chi_c and J/psi production in d+Au collisions at sqrt(s_NN) = 200 GeV"

2023

The $\psi^{\prime}$ nuclear modification factor, $R_{dAu}$, as a function of proper time in nucleus. Also included is the previously measured $J/\psi$ $R_{dAu}$ as a function of $N_{coll}$.

ppg151nuclear modification$\psi^\prime$ suppressionmidrapidity200.0$d$ Au --> CHARGED X
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"Figure 2" of "Measurement of long-range angular correlation and quadrupole anisotropy of pions and (anti)protons in central $d+$Au collisions at $\s…

2023

$c_2$ ($p_T$) for track lower-tower pairs from 0-5% $d$+Au collisions and $c_2$ ($p_T$) for pairs in minimum bias $p$+$p$ collisions times the dilution factor.

ppg161long-range angular correlation$p$ $p$ --> CHARGED Xazimuthal angular correlationsquadrupole anisotropy200.0$d$ Au --> CHARGED X
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"Figure 4b" of "Measurement of long-range angular correlation and quadrupole anisotropy of pions and (anti)protons in central $d+$Au collisions at $\…

2023

Measured $v_2$ ($p_T$) for identified pions, each charged combined, 0-5% central $d$+Au collisions at RHIC.

ppg161long-range angular correlationazimuthal angular correlationsquadrupole anisotropy200.0$d$ Au --> CHARGED X
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"Figure 3" of "Measurement of long-range angular correlation and quadrupole anisotropy of pions and (anti)protons in central $d+$Au collisions at $\s…

2023

Measured $v_2$ for midrapidity charged tracks in 0-5% central $d$+Au at $\sqrt{s_{NN}}$ = 200 GeV using the event plane method.

ppg161long-range angular correlationazimuthal angular correlationsquadrupole anisotropy200.0$d$ Au --> CHARGED X
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"Figure 1a" of "Measurements of mass-dependent azimuthal anisotropy in central $p+$Au, $d+$Au, and $^3$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ G…

2023

Transverse momentum dependence of $v_2$ for identified pions and protons within $|\eta|$ < 0.35 in 0-5% central $^3$He+Au collisions.

ppg207$p$ Au --> CHARGED Xmidrapidityazimuthal anisotropy$^3$He Au --> CHARGED Xtransverse momentum200.0
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"Table 2" of "Measurements of mass-dependent azimuthal anisotropy in central $p+$Au, $d+$Au, and $^3$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

2023

Values of $v_2$($p_T$) for kaons in central 0-5% $p$+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

ppg207$p$ Au --> CHARGED Xmidrapidityazimuthal anisotropytransverse momentum200.0
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"Table 3" of "Measurements of mass-dependent azimuthal anisotropy in central $p+$Au, $d+$Au, and $^3$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV"

2023

Values of $v_2$($p_T$) for kaons in central 0-5% $^3$He+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

ppg207midrapidityazimuthal anisotropy$^3$He Au --> CHARGED Xtransverse momentum200.0
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