78 research outputs found

    System Size and Energy Dependence of Jet-Induced Hadron Pair Correlation Shapes in Cu+Cu and Au+Au Collisions at sqrt(s_NN) = 200 and 62.4 GeV

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    We present azimuthal angle correlations of intermediate transverse momentum (1-4 GeV/c) hadrons from {dijets} in Cu+Cu and Au+Au collisions at sqrt(s_NN) = 62.4 and 200 GeV. The away-side dijet induced azimuthal correlation is broadened, non-Gaussian, and peaked away from \Delta\phi=\pi in central and semi-central collisions in all the systems. The broadening and peak location are found to depend upon the number of participants in the collision, but not on the collision energy or beam nuclei. These results are consistent with sound or shock wave models, but pose challenges to Cherenkov gluon radiation models.Comment: 464 authors from 60 institutions, 6 pages, 3 figures, 2 tables. Submitted to Physical Review Letters. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.htm

    Improved Measurement of Double Helicity Asymmetry in Inclusive Midrapidity pi^0 Production for Polarized p+p Collisions at sqrt(s)=200 GeV

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    We present an improved measurement of the double helicity asymmetry for pi^0 production in polarized proton-proton scattering at sqrt(s) = 200 GeV employing the PHENIX detector at the Relativistic Heavy Ion Collider (RHIC). The improvements to our previous measurement come from two main factors: Inclusion of a new data set from the 2004 RHIC run with higher beam polarizations than the earlier run and a recalibration of the beam polarization measurements, which resulted in reduced uncertainties and increased beam polarizations. The results are compared to a Next to Leading Order (NLO) perturbative Quantum Chromodynamics (pQCD) calculation with a range of polarized gluon distributions.Comment: 389 authors, 4 pages, 2 tables, 1 figure. Submitted to Phys. Rev. D, Rapid Communications. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.htm

    Elliptic Flow of Identified Hadrons in Au+Au Collisions at sqrt(s_NN) = 200 GeV

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    The anisotropy parameter v_2, the second harmonic of the azimuthal particles distribution, has been measured with the PHENIX detector in Au+Au collisions at sqrt(s_NN) = 200 GeV for identified and inclusive charged particles at central rapidities (|eta| < 0.35) with respect to the reaction plane defined at high rapidities (|eta| = 3-4). The v_2 for all particles reaches a maximum at mid-centrality, and increases with p_T up to 2 GeV/c and then saturates or decreases slightly. Our results depart from hydrodynamically predicted behavior above 2 GeV/c. A quark coalescence model is also investigated.Comment: 325 authors, 6 pages text, RevTeX, 3 figures, 0 tables. This version accepted for publication in Phys. Rev. Lett. after minor changes in response to referee suggestions. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are publicly available at http://www.phenix.bnl.gov/papers.htm

    Photoproduction of J/psi and of high mass e+e- in ultra-peripheral Au+Au collisions at sqrt(s_NN) = 200 GeV

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    We present the first measurement of photoproduction of J/psi and of two-photon production of high-mass e+e- pairs in electromagnetic (or ultra-peripheral) nucleus-nucleus interactions, using Au+Au data at sqrt(s_NN) = 200 GeV. The events are tagged with forward neutrons emitted following Coulomb excitation of one or both Au^{star} nuclei. The event sample consists of 28 events with m_{e+e-} > 2 GeV/c^2 with zero like-sign background. The measured cross sections at midrapidity of d\sigma / dy (J/psi + Xn, y=0) = 76 +/- 33 (stat) +/- 11 (syst) micro b and d^2\sigma/dm dy (e^+e^- + Xn, y=0) = 86 +/- 23 (stat) +/- 16 (syst) micro b/(GeV/c^2) for m_{e+e-} \in [2.0,2.8] GeV/c^2 are consistent with various theoretical predictions.Comment: 345 authors from 52 institutions, 20 pages, 4 figures, 3 tables. Submitted to Physics Letters B. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.htm

    Scaling properties of azimuthal anisotropy in Au+Au and Cu+Cu collisions at sqrt(s_NN) = 200 GeV

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    Detailed differential measurements of the elliptic flow for particles produced in Au+Au and Cu+Cu collisions at sqrt(s_NN) = 200 GeV are presented. Predictions from perfect fluid hydrodynamics for the scaling of the elliptic flow coefficient v_2 with eccentricity, system size and transverse energy are tested and validated. For transverse kinetic energies KE_T ~ m_T-m up to ~1 GeV, scaling compatible with the hydrodynamic expansion of a thermalized fluid is observed for all produced particles. For large values of KE_T, the mesons and baryons scale separately. A universal scaling for the flow of both mesons and baryons is observed for the full transverse kinetic energy range of the data when quark number scaling is employed. In both cases the scaling is more pronounced in terms of KE_T rather than transverse momentum.Comment: 422 authors from 58 institutions, 6 pages, 3 figures. Submitted to Physical Review Letters. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.htm

    Correlated Production of p and p^bar in Au+Au Collisions at sqrt(s_NN) = 200 GeV

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    Correlations between p and pbar's at transverse momenta typical of enhanced baryon production in Au+Au collisions are reported. The PHENIX experiment measures same and opposite sign baryon pairs in Au+Au collisions at sqrt(s_NN) = 200 GeV. Correlated production of p and p^bar with the trigger particle from the range 2.5 < p_T < 4.0 GeV/c and the associated particle with 1.8 < p_T < 2.5 GeV/c is observed to be nearly independent of the centrality of the collisions. Same sign pairs show no correlation at any centrality. The conditional yield of mesons triggered by baryons (and anti-baryons) and mesons in the same pT range rises with increasing centrality, except for the most central collisions, where baryons show a significantly smaller number of associated mesons. These data are consistent with a picture in which hard scattered partons produce correlated p and p^bar in the p_T region of the baryon excess.Comment: 420 authors from 58 institutions, 21 pages,5 figures. Submitted to Physics Letters B. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.htm

    The Physics of the B Factories

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    Triangle Singularity as the Origin of the a1(1420)

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    International audienceThe COMPASS Collaboration experiment recently discovered a new isovector resonancelike signal with axial-vector quantum numbers, the a1(1420), decaying to f0(980)π. With a mass too close to and a width smaller than the axial-vector ground state a1(1260), it was immediately interpreted as a new light exotic meson, similar to the X, Y, Z states in the hidden-charm sector. We show that a resonancelike signal fully matching the experimental data is produced by the decay of the a1(1260) resonance into K*(→Kπ)K¯ and subsequent rescattering through a triangle singularity into the coupled f0(980)π channel. The amplitude for this process is calculated using a new approach based on dispersion relations. The triangle-singularity model is fitted to the partial-wave data of the COMPASS experiment. Despite having fewer parameters, this fit shows a slightly better quality than the one using a resonance hypothesis and thus eliminates the need for an additional resonance in order to describe the data. We thereby demonstrate for the first time in the light-meson sector that a resonancelike structure in the experimental data can be described by rescattering through a triangle singularity, providing evidence for a genuine three-body effect

    Spin density matrix elements in exclusive ρ0\rho ^0 meson muoproduction

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    We report on a measurement of Spin Density Matrix Elements (SDMEs) in hard exclusive ρ0\rho ^0 meson muoproduction at COMPASS using 160~GeV/cc polarised μ+ \mu ^{+} and μ \mu ^{-} beams impinging on a liquid hydrogen target. The measurement covers the kinematic range 5.0~GeV/c2c^2 <W<< W < 17.0~GeV/c2c^2, 1.0 (GeV/cc)2^2 <Q2<< Q^2 < 10.0 (GeV/cc)2^2 and 0.01 (GeV/cc)2^2 <pT2<< p_{\rm{T}}^2 < 0.5 (GeV/cc)2^2. Here, WW denotes the mass of the final hadronic system, Q2Q^2 the virtuality of the exchanged photon, and pTp_{\rm{T}} the transverse momentum of the ρ0\rho ^0 meson with respect to the virtual-photon direction. The measured non-zero SDMEs for the transitions of transversely polarised virtual photons to longitudinally polarised vector mesons (γTVL\gamma^*_T \to V^{ }_L) indicate a violation of ss-channel helicity conservation. Additionally, we observe a dominant contribution of natural-parity-exchange transitions and a very small contribution of unnatural-parity-exchange transitions, which is compatible with zero within experimental uncertainties. The results provide important input for modelling Generalised Parton Distributions (GPDs). In particular, they may allow one to evaluate in a model-dependent way the role of parton helicity-flip GPDs in exclusive ρ0\rho ^0 production.We report on a measurement of Spin Density Matrix Elements (SDMEs) in hard exclusive ρ0\rho ^0 meson muoproduction at COMPASS using 160 GeV/c polarised μ+ \mu ^{+} and μ \mu ^{-} beams impinging on a liquid hydrogen target. The measurement covers the kinematic range 5.0 GeV/c2<W<c^2< W< 17.0 GeV/c2c^2, 1.0 (GeV/c)2<Q2<^2< Q^2< 10.0 (GeV/c)2^2 and 0.01 (GeV/c)2<pT2<^2< p_{\textrm{T}}^2< 0.5 (GeV/c)2^2. Here, W denotes the mass of the final hadronic system, Q2Q^2 the virtuality of the exchanged photon, and pTp_{\textrm{T}} the transverse momentum of the ρ0\rho ^0 meson with respect to the virtual-photon direction. The measured non-zero SDMEs for the transitions of transversely polarised virtual photons to longitudinally polarised vector mesons (γTVL\gamma ^*_T \rightarrow V^{ }_L) indicate a violation of s-channel helicity conservation. Additionally, we observe a dominant contribution of natural-parity-exchange transitions and a very small contribution of unnatural-parity-exchange transitions, which is compatible with zero within experimental uncertainties. The results provide important input for modelling Generalised Parton Distributions (GPDs). In particular, they may allow one to evaluate in a model-dependent way the role of parton helicity-flip GPDs in exclusive ρ0\rho ^0 production.We report on a measurement of Spin Density Matrix Elements (SDMEs) in hard exclusive ρ0\rho ^0 meson muoproduction at COMPASS using 160~GeV/cc polarised μ+ \mu ^{+} and μ \mu ^{-} beams impinging on a liquid hydrogen target. The measurement covers the kinematic range 5.0~GeV/c2c^2<W<< W < 17.0~GeV/c2c^2, 1.0 (GeV/cc)2^2<Q2<< Q^2 < 10.0 (GeV/cc)2^2 and 0.01 (GeV/cc)2^2<pT2<< p_{\rm{T}}^2 < 0.5 (GeV/cc)2^2. Here, WW denotes the mass of the final hadronic system, Q2Q^2 the virtuality of the exchanged photon, and pTp_{\rm{T}} the transverse momentum of the ρ0\rho ^0 meson with respect to the virtual-photon direction. The measured non-zero SDMEs for the transitions of transversely polarised virtual photons to longitudinally polarised vector mesons (γTVL\gamma^*_T \to V^{ }_L) indicate a violation of ss-channel helicity conservation. Additionally, we observe a dominant contribution of natural-parity-exchange transitions and a very small contribution of unnatural-parity-exchange transitions, which is compatible with zero within experimental uncertainties. The results provide important input for modelling Generalised Parton Distributions (GPDs). In particular, they may allow one to evaluate in a model-dependent way the role of parton helicity-flip GPDs in exclusive ρ0\rho ^0 production

    Measurement of the cross section for hard exclusive π0\pi^0 leptoproduction

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    We report on a measurement of hard exclusive π0\pi^0 muoproduction on the proton by COMPASS using 160 GeV/cc polarised μ+\mu^+ and μ\mu^- beams of the CERN SPS impinging on a liquid hydrogen target. From the average of the measured μ+\mu^+ and μ\mu^- cross sections, the virtual-photon proton cross section is determined as a function of the squared four-momentum transfer between initial and final proton in the range 0.08(GeV/c)2<t<0.64(GeV/c)20.08\,(\text{GeV/}c)^2 < |t| < 0.64\,(\text{GeV/}c)^2. The average kinematics of the measurement are Q2=2.0  (GeV/c)2\langle Q^2 \rangle =2.0\; {(\text{GeV}/c)^2}, ν=12.8  GeV\langle \nu \rangle = 12.8\; {\text{GeV}}, xBj=0.093\langle x_{Bj} \rangle = 0.093 and t=0.256  (GeV/c)2\langle -t \rangle = 0.256\; {(\text{GeV}/c)^2} . Fitting the azimuthal dependence reveals a combined contribution by transversely and longitudinally polarised photons of (8.1 ± 0.9stat 1.0+ 1.1sys)nb/(GeV/c)2(8.1 \ \pm \ 0.9_{\text{stat}}{}_{- \ 1.0}^{+ \ 1.1}\big\rvert_{\text{sys}})\,{\text{nb}}/{(\text{GeV}/c)^{2}}, as well as transverse-transverse and longitudinal-transverse interference contributions of (6.0±1.3stat 0.7+ 0.7sys)nb/(GeV/c)2(-6.0 \pm 1.3_{\text{stat}}{}_{- \ 0.7}^{+ \ 0.7}\big\rvert_{\text{sys}})\,{\text{nb}}/{(\text{GeV}/c)^{2}} and (1.4±0.5stat 0.2+ 0.3sys)nb/(GeV/c)2(1.4 \pm 0.5_{\text{stat}}{}_{- \ 0.2}^{+ \ 0.3}\big\rvert_{\text{sys}})\,{\text{nb}}/{(\text{GeV}/c)^{2}}, respectively. Our results provide important input for modelling Generalised Parton Distributions. In the context of the phenomenological Goloskokov-Kroll model, the statistically significant transverse-transverse interference contribution constitutes clear experimental evidence for the chiral-odd GPD ET\overline{E}_T
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