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Pion, kaon, proton and anti-proton transverse momentum distributions from p+p and d+Au collisions at $\sqrt{s_{NN}} = 200$ GeV

STAR Collaboration

Abstract

Identified mid-rapidity particle spectra of $π^{\pm}$, $K^{\pm}$, and $p(\bar{p})$ from 200 GeV p+p and d+Au collisions are reported. A time-of-flight detector based on multi-gap resistive plate chamber technology is used for particle identification. The particle-species dependence of the Cronin effect is observed to be significantly smaller than that at lower energies. The ratio of the nuclear modification factor ($R_{dAu}$) between protons $(p+\bar{p})$ and charged hadrons ($h$) in the transverse momentum range $1.2<{p_{T}}<3.0$ GeV/c is measured to be $1.19\pm0.05$(stat)$\pm0.03$(syst) in minimum-bias collisions and shows little centrality dependence. The yield ratio of $(p+\bar{p})/h$ in minimum-bias d+Au collisions is found to be a factor of 2 lower than that in Au+Au collisions, indicating that the Cronin effect alone is not enough to account for the relative baryon enhancement observed in heavy ion collisions at RHIC.

Pion, kaon, proton and anti-proton transverse momentum distributions from p+p and d+Au collisions at $\sqrt{s_{NN}} = 200$ GeV

Abstract

Identified mid-rapidity particle spectra of , , and from 200 GeV p+p and d+Au collisions are reported. A time-of-flight detector based on multi-gap resistive plate chamber technology is used for particle identification. The particle-species dependence of the Cronin effect is observed to be significantly smaller than that at lower energies. The ratio of the nuclear modification factor () between protons and charged hadrons () in the transverse momentum range GeV/c is measured to be (stat)(syst) in minimum-bias collisions and shows little centrality dependence. The yield ratio of in minimum-bias d+Au collisions is found to be a factor of 2 lower than that in Au+Au collisions, indicating that the Cronin effect alone is not enough to account for the relative baryon enhancement observed in heavy ion collisions at RHIC.

Paper Structure

This paper contains 1 equation, 4 figures, 1 table.

Figures (4)

  • Figure 1: $1/\beta$ vs. momentum for $\pi^{\pm}$, $K^{\pm}$, and $p(\bar{p})$ from 200 GeV d+Au collisions. Separations between pions and kaons, kaons and protons are achieved up to $p_{T}\simeq1.6$ and $3.0$ GeV/c, respectively. The insert shows $m^{2}=p^{2}(1/\beta^{2}-1)$ for $1.2<p_{T}<1.4$ GeV/c. Clear separation of pions, kaons and protons is seen.
  • Figure 2: The invariant yields of $\pi^{+}$ (filled circles), $K^{+}$ (open squares), $p$ (filled triangles) and their anti-particles as a function of $p_{T}$ from d+Au and NSD p+p events at 200 GeV. The rapidity range was $-0.5<y<0.0$ with the direction of the outgoing Au ions as negative rapidity. Errors are statistical.
  • Figure 3: The identified particle $R_{dAu}$ for minimum-bias and top 20% d+Au collisions. The filled triangles are for $p+\bar{p}$, the filled circles are for $\pi^{+}+\pi^{-}$ and the open squares are for $K^{+}+K^{-}$. Dashed lines are $R_{dAu}$ of inclusive charged hadrons from stardau. The open triangles and open circles are $R_{CP}$ of $p+\bar{p}$ and $\pi^{0}$ in Au+Au collisions measured by PHENIX phenixpid. Errors are statistical. The gray band represents the normalization uncertainty of 16%.
  • Figure 4: Minimum-bias ratios of protons ($p+\bar{p}$) over inclusive charged hadrons ($h$) at $-0.5\!<\!\eta\!<\!0.0$ from $\sqrt{s_{_{NN}}} =200$ GeV p+p (open diamonds), d+Au (filled triangles) and $\sqrt{s_{_{NN}}} =130$ GeV Au+Au phenixpid (asterisks) collisions. Results of $\mathrm{p+\bar{p}}$ collisions at $\sqrt{s_{_{NN}}} = 1.8$ TeV e735 are shown as solid stars. Dashed lines are results of $p/h^{+}$ ratios from $\sqrt{s_{_{NN}}} = 23.8$ GeV p+p (short-dashed lines) and p+W (dot-dashed) collisions cronincronin1979. Errors are statistical.