352 research outputs found

    ϕ\phi- meson Production at RHIC energies using the PHENIX Detector

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    Light vector mesons are among the most informative probes to understand the strongly coupled Quark Gluon Plasma created at RHIC. The suppression of light mesons at high transverse momentum, compared to expectations from scaled p+pp+p results, reflects the properties of the strongly interacting matter formed. The ϕ\phi-meson is one of the probes whose systematic measurement in p+pp+p, d+Aud+Au and Au+AuAu+Au collisions can provide useful information about initial and final state effects on particle production. The mass, width and branching ratio of the ϕ\phi-meson decay in the di-kaon and di-electron decay channels could be modified in \au collisions due to the restoration of chiral symmetry in the QGP. The PHENIX experiment at RHIC has measured ϕ\phi-meson production in various systems ranging form p+pp+p, d+Aud+Au to Au+AuAu+Au collisions via both its di-electron and di-kaon decay modes. A summary of PHENIX results on invariant spectra, nuclear modification factor and elliptic flow of the ϕ\phi-meson are presented here

    New faunistic data on Dolichopodidae (Diptera) from Turkey

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    Faunistic data is given for 83 species of Dolichopodidae from Turkey. The following genera are recorded for the first time in Turkey: Achalcus Loew, 1857, Cyrturella Collin, 1952, and Trigonocera Becker, 1902; 21 species are recorded for the first time in Turkey: Achalcus flavicollis (Meigen, 1824), Aphrosylus venator Loew, 1857, Asyndetus separatus (Becker, 1902), Chrysotus larachensis Grichanov, Nourti et Kettani, 2020, Cyrturella albosetosa (Strobl, 1909), Hydrophorus bipunctatus (Lehmann, 1822), Lamprochromus bifasciatus (Macquart, 1827), Lamprochromus kowarzi Negrobov et Tshalaja, 1988, Medetera petrophiloides Parent, 1925, M. signaticornis Loew, 1957, Orthoceratium sabulosum (Becker, 1907), Rhaphium antennatum (Carlier, 1835), Sciapus bellus (Loew, 1873), S. euchromus (Loew, 1857), S. longulus (Fallén, 1823), S. tenuinervis (Loew, 1857), Syntormon triangulipes Becker, 1902, Teuchophorus calcaratus (Macquart, 1828), Thinophilus quadrimaculatus Becker, 1902, Trigonocera rivosa Becker, 1902, Xanthochlorus silaceus Chandler et Negrobov, 2008

    Measurement of light mesons at RHIC by the PHENIX experiment

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    The PHENIX experiment at RHIC has measured a variety of light neutral mesons (π0\pi^{0}, KS0_{S}^{0}, η\eta, ω\omega, η\eta^{\prime}, ϕ\phi) via multi-particle decay channels over a wide range of transverse momentum. A review of the recent results on the production rates of light mesons in p+p and their nuclear modification factors in d+Au, Cu+Cu and Au+Au collisions at different energies is presented.Comment: 5 pages, 4 figures, talk given at Hard Probes 2008 conference in La Toja, Spain. submitted to EPJ

    Construction and Expected Performance of the Hadron Blind Detector for the PHENIX Experiment at RHIC

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    A new Hadron Blind Detector (HBD) for electron identification in high density hadron environment has been installed in the PHENIX detector at RHIC in the fall of 2006. The HBD will identify low momentum electron-positron pairs to reduce the combinatorial background in the e+ee^{+}e^{-} mass spectrum, mainly in the low-mass region below 1 GeV/c2^{2}. The HBD is a windowless proximity-focusing Cherenkov detector with a radiator length of 50 cm, a CsI photocathode and three layers of Gas Electron Multipliers (GEM). The HBD uses pure CF4_{4} as a radiator and a detector gas. Construction details and the expected performance of the detector are described.Comment: QM2006 proceedings, 4 pages 3 figure

    A Hadron Blind Detector for the PHENIX Experiment

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    A novel Hadron Blind Detector (HBD) has been developed for an upgrade of the PHENIX experiment at RHIC. The HBD will allow a precise measurement of electron-positron pairs from the decay of the light vector mesons and the low-mass pair continuum in heavy-ion collisions. The detector consists of a 50 cm long radiator filled with pure CF4 and directly coupled in a windowless configuration to a triple Gas Electron Multiplier (GEM) detector with a CsI photocathode evaporated on the top face of the first GEM foil.Comment: 4 pages, 3 figures, Quark Matter 2005 conference proceeding

    Design, Construction, Operation and Performance of a Hadron Blind Detector for the PHENIX Experiment

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    A Hadron Blind Detector (HBD) has been developed, constructed and successfully operated within the PHENIX detector at RHIC. The HBD is a Cherenkov detector operated with pure CF4. It has a 50 cm long radiator directly coupled in a window- less configuration to a readout element consisting of a triple GEM stack, with a CsI photocathode evaporated on the top surface of the top GEM and pad readout at the bottom of the stack. This paper gives a comprehensive account of the construction, operation and in-beam performance of the detector.Comment: 51 pages, 39 Figures, submitted to Nuclear Instruments and Method

    Quadrupole Anisotropy in Dihadron Azimuthal Correlations in Central dd++Au Collisions at sNN\sqrt{s_{_{NN}}}=200 GeV

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    The PHENIX collaboration at the Relativistic Heavy Ion Collider (RHIC) reports measurements of azimuthal dihadron correlations near midrapidity in dd++Au collisions at sNN\sqrt{s_{_{NN}}}=200 GeV. These measurements complement recent analyses by experiments at the Large Hadron Collider (LHC) involving central pp++Pb collisions at sNN\sqrt{s_{_{NN}}}=5.02 TeV, which have indicated strong anisotropic long-range correlations in angular distributions of hadron pairs. The origin of these anisotropies is currently unknown. Various competing explanations include parton saturation and hydrodynamic flow. We observe qualitatively similar, but larger, anisotropies in dd++Au collisions compared to those seen in pp++Pb collisions at the LHC. The larger extracted v2v_2 values in dd++Au collisions at RHIC are consistent with expectations from hydrodynamic calculations owing to the larger expected initial-state eccentricity compared with that from pp++Pb collisions. When both are divided by an estimate of the initial-state eccentricity the scaled anisotropies follow a common trend with multiplicity that may extend to heavy ion data at RHIC and the LHC, where the anisotropies are widely thought to arise from hydrodynamic flow.Comment: 375 authors, 7 pages, 5 figures. Published in Phys. Rev. Lett. v2 has minor changes to text and figures in response to PRL referee suggestions. 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

    Charged hadron multiplicity fluctuations in Au+Au and Cu+Cu collisions from sqrt(s_NN) = 22.5 to 200 GeV

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    A comprehensive survey of event-by-event fluctuations of charged hadron multiplicity in relativistic heavy ions is presented. The survey covers Au+Au collisions at sqrt(s_NN) = 62.4 and 200 GeV, and Cu+Cu collisions sqrt(s_NN) = 22.5, 62.4, and 200 GeV. Fluctuations are measured as a function of collision centrality, transverse momentum range, and charge sign. After correcting for non-dynamical fluctuations due to fluctuations in the collision geometry within a centrality bin, the remaining dynamical fluctuations expressed as the variance normalized by the mean tend to decrease with increasing centrality. The dynamical fluctuations are consistent with or below the expectation from a superposition of participant nucleon-nucleon collisions based upon p+p data, indicating that this dataset does not exhibit evidence of critical behavior in terms of the compressibility of the system. An analysis of Negative Binomial Distribution fits to the multiplicity distributions demonstrates that the heavy ion data exhibit weak clustering properties.Comment: 464 authors from 60 institutions, 17 pages, 12 figures, 1 table. Submitted to Physical Review C. 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
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