204 research outputs found

    Improved Measurement of the Longitudinal Spin Transfer to Λ and Λ¯ Hyperons in Polarized Proton-Proton Collisions at √\u3cem\u3es\u3c/em\u3e = 200 GeV

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    The longitudinal spin transfer DLL to Λ and Λ¯ hyperons produced in high-energy polarized proton-proton collisions is expected to be sensitive to the helicity distribution functions of strange quarks and antiquarks of the proton, and to longitudinally polarized fragmentation functions. We report an improved measurement of DLL from data obtained at a center-of-mass energy of √s = 200  GeV with the STAR detector at RHIC. The data have an approximately twelve times larger figure of merit than prior results and cover |η| \u3c 1.2 in pseudorapidity with transverse momenta pT up to 6  GeV/c. In the forward scattering hemisphere at largest pT, the longitudinal spin transfer is found to be DLL = −0.036 ± 0.048(stat) ± 0.013(sys) for Λ hyperons and DLL = 0.032 ± 0.043(stat) ± 0.013(sys) for Λ¯ antihyperons. The dependences on η and pT are presented and compared with model evaluations

    \u3cem\u3eJ/ψ\u3c/em\u3e Production Cross Section and Its Dependence on Charged-Particle Multiplicity in \u3cem\u3ep\u3c/em\u3e +\u3cem\u3e p\u3c/em\u3e Collisions at √\u3cem\u3es\u3c/em\u3e=200 GeV

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    We present a measurement of inclusive J/ψ production at mid-rapidity (|y| \u3c 1) in p+p collisions at a center-of-mass energy of √s=200 GeV with the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The differential production cross section for J/ψ as a function of transverse momentum (pT) for 0 \u3c pT \u3c 14 GeV/c and the total cross section are reported and compared to calculations from the color evaporation model and the non-relativistic Quantum Chromodynamics model. The dependence of J/ψ relative yields in three pT intervals on charged-particle multiplicity at mid-rapidity is measured for the first time in p+p collisions at √s=200 GeV and compared with that measured at √s=7 TeV, PYTHIA8 and EPOS3 Monte Carlo generators, and the Percolation model prediction

    Low-\u3cem\u3ep\u3csub\u3eT\u3c/sub\u3e\u3c/em\u3e \u3cem\u3ee\u3c/em\u3e\u3csup\u3e+\u3c/sup\u3e \u3cem\u3ee\u3c/em\u3e\u3csup\u3e-\u3c/sup\u3e Pair Production in Au + Au Collisions at √\u3cem\u3es\u3c/em\u3e\u3csub\u3eNN\u3c/sub\u3e\u3c/em\u3e = 193 GeV and U + U Collisions at √\u3cem\u3es\u3c/em\u3e\u3csub\u3eNN\u3c/sub\u3e\u3c/em\u3e = 193 GeV at STAR

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    We report first measurements of e+e− pair production in the mass region 0.4 \u3c Mee \u3c 2.6  GeV/c2 at low transverse momentum (pT \u3c 0.15  GeV/c) in noncentral Au+Au collisions at √sNN = 200  GeV and U+U collisions at √sNN = 193  GeV. Significant enhancement factors, expressed as ratios of data over known hadronic contributions, are observed in the 40%–80% centrality of these collisions. The excess yields peak distinctly at low pT with a width (√⟨p2T⟩) between 40 and 60  MeV/c. The absolute cross section of the excess depends weakly on centrality, while those from a theoretical model calculation incorporating an in-medium broadened ρ spectral function and radiation from a quark gluon plasma or hadronic cocktail contributions increase dramatically with an increasing number of participant nucleons. Model calculations of photon-photon interactions generated by the initial projectile and target nuclei describe the observed excess yields but fail to reproduce the p2T distributions

    Beam Energy Dependence of Rapidity-Even Dipolar Flow in Au + Au Collisions

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    New measurements of directed flow for charged hadrons, characterized by the Fourier coefficient v1, are presented for transverse momenta pT, and centrality intervals in Au+Au collisions recorded by the STAR experiment for the center-of-mass energy range √sNN=7.7–200 GeV. The measurements underscore the importance of momentum conservation, and the characteristic dependencies on √sNN, centrality and pT are consistent with the expectations of geometric fluctuations generated in the initial stages of the collision, acting in concert with a hydrodynamic-like expansion. The centrality and pT dependencies of v1even, as well as an observed similarity between its excitation function and that for v3, could serve as constraints for initial-state models. The v1even excitation function could also provide an important supplement to the flow measurements employed for precision extraction of the temperature dependence of the specific shear viscosity

    The Proton-Ω Correlation Function in Au + Au Collisions at √s\u3csub\u3eNN\u3c/sub\u3e = 200 GeV

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    We present the first measurement of the proton–Ω correlation function in heavy-ion collisions for the central (0–40%) and peripheral (40–80%) Au + Au collisions at √sNN = 200 GeV by the STAR experiment at the Relativistic Heavy-Ion Collider (RHIC). Predictions for the ratio of peripheral collisions to central collisions for the proton–Ω correlation function are sensitive to the presence of a nucleon–Ω bound state. These predictions are based on the proton–Ω interaction extracted from (2+1)-flavor lattice QCD calculations at the physical point. The measured ratio of the proton–Ω correlation function between the peripheral (small system) and central (large system) collisions is less than unity for relative momentum smaller than 40 MeV/c. Comparison of our measured correlation ratio with theoretical calculation slightly favors a proton–Ω bound system with a binding energy of ∼ 27 MeV
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