Table 1
Figure 1a
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Invariant mass distributions of electron pairs in the region $|y_{ee}| < 0.5$, p+p.
https://www.hepdata.net/record/data/982159yaml https://www.hepdata.net/record/data/982159/csvcsvFigure 1a
10.17182/hepdata.102940.v1/t1
Invariant mass distributions of electron pairs in the region $|y_{ee}| < 0.5$, p+p.
https://www.hepdata.net/record/data/982159yaml https://www.hepdata.net/record/data/982159/csvcsvFigure 1b
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Invariant mass distributions of electron pairs in the region $|y_{ee}| < 0.5$, d+Au.
https://www.hepdata.net/record/data/982160yaml https://www.hepdata.net/record/data/982160/csvcsvFigure 2a
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(a) $B_{ee} \times d\sigma/dy$ vs. $y$ for p+p collisions and for d+Au collisions (scaled down by 103).
https://www.hepdata.net/record/data/982161yaml https://www.hepdata.net/record/data/982161/csvcsvFigure 2b
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$R_{dAu}$ vs. $y$.
https://www.hepdata.net/record/data/982162yaml https://www.hepdata.net/record/data/982162/csvcsvFigure 3a
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Comparison of our d+Au measurements to the pA measurements from E772. Ratio of $\Upsilon$ production in pA to pp scaled...
https://www.hepdata.net/record/data/982163yaml https://www.hepdata.net/record/data/982163/csvcsvFigure 3b
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Comparison of our d+Au measurements to the pA measurements from E772. Exponent $\alpha$ as a function of $x_{F}$.
https://www.hepdata.net/record/data/982164yaml https://www.hepdata.net/record/data/982164/csvcsvFigure 4a
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Invariant mass distributions of electron pairs in the region $|y_{ee}| < 1.0$ for the centrality selections $30-60\%$.
https://www.hepdata.net/record/data/982165yaml https://www.hepdata.net/record/data/982165/csvcsvFigure 4b
10.17182/hepdata.102940.v1/t8
Invariant mass distributions of electron pairs in the region $|y_{ee}| < 1.0$ for the centrality selections $10-30\%$.
https://www.hepdata.net/record/data/982166yaml https://www.hepdata.net/record/data/982166/csvcsvFigure 4c
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Invariant mass distributions of electron pairs in the region $|y_{ee}| < 1.0$ for the centrality selections $0-10\%$.
https://www.hepdata.net/record/data/982167yaml https://www.hepdata.net/record/data/982167/csvcsvFigure 5a
10.17182/hepdata.102940.v1/t10
Nuclear modification factor for $\Upsilon$(1S+2S+3S), in $|y| < 1.0$ in d+Au and Au+Au collisions as a function of $N_{part}$.
https://www.hepdata.net/record/data/982168yaml https://www.hepdata.net/record/data/982168/csvcsvFigure 5b
10.17182/hepdata.102940.v1/t11
Nuclear modification factor for $\Upsilon$(1S+2S+3S), in $|y| < 0.5$, in d+Au and Au+Au collisions as a function of $N_{part}$.
https://www.hepdata.net/record/data/982169yaml https://www.hepdata.net/record/data/982169/csvcsvFigure 5c
10.17182/hepdata.102940.v1/t12
Nuclear modification factor for $\Upsilon$(1S) in $|y| < 1.0$, in d+Au and Au+Au collisions as a function of $N_{part}$.
https://www.hepdata.net/record/data/982170yaml https://www.hepdata.net/record/data/982170/csvcsv10.17182/hepdata.102940.v1/t13
Nuclear modification factor for $\Upsilon$(1S) in $|y| < 0.5$, in d+Au and Au+Au collisions as a function of $N_{part}$.
https://www.hepdata.net/record/data/982171yaml https://www.hepdata.net/record/data/982171/csvcsvFigure 6
10.17182/hepdata.102940.v1/t14
Nuclear modification factor of quarkonium states as a function of binding energy as measured by STAR.
https://www.hepdata.net/record/data/982172yaml https://www.hepdata.net/record/data/982172/csvcsvLoading Data...
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