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Transverse-momentum dependence of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>J</mml:mi><mml:mo>/</mml:mo><mml:mi>ψ</mml:mi></mml:mrow></mml:math>nuclear modification in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>d</mml:mi></mml:math>+Au collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msqrt><mml:msub><mml:mi>s</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mi>…
We present measured $J/\ensuremath{\psi}$ production rates in $d+\text{Au}$ collisions at $\sqrt{{s}_{{}_{NN}}}=200$ GeV over broad ranges of transverse momentum (${p}_{T}=0$--14 GeV/$c$) and rapidity ($\ensuremath{-}2.2<y<2.2$). We construct the nuclear-modification factor ${R}_{d\mathrm{Au}}$ for these kinematics and as a function of collision centrality (related to impact parameter for the $d+\mathrm{Au}$ collision). We find that …