21,994 research outputs found

    Chiral magnetic effect search in p+Au, d+Au and Au+Au collisions at RHIC

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    Metastable domains of fluctuating topological charges can change the chirality of quarks and induce local parity violation in quantum chromodynamics. This can lead to observable charge separation along the direction of the strong magnetic field produced by spectator protons in relativistic heavy-ion collisions, a phenomenon called the chiral magnetic effect (CME). A major background source for CME measurements using the charge-dependent azimuthal correlator (Δγ\Delta\gamma) is the intrinsic particle correlations (such as resonance decays) coupled with the azimuthal elliptical anisotropy (v2v_{2}). In heavy-ion collisions, the magnetic field direction and event plane angle are correlated, thus the CME and the v2v_{2}-induced background are entangled. In this report, we present two studies from STAR to shed further lights on the background issue. (1) The Δγ\Delta\gamma should be all background in small system p+Au and d+Au collisions, because the event plane angles are dominated by geometry fluctuations uncorrelated to the magnetic field direction. However, significant Δγ\Delta\gamma is observed, comparable to the peripheral Au+Au data, suggesting a background dominance in the latter, and likely also in the mid-central Au+Au collisions where the multiplicity and v2v_{2} scaled correlator is similar. (2) A new approach is devised to study Δγ\Delta\gamma as a function of the particle pair invariant mass (minvm_{inv}) to identify the resonance backgrounds and hence to extract the possible CME signal. Signal is consistent with zero within uncertainties at high minvm_{inv}. Signal at low minvm_{inv}, extracted from a two-component model assuming smooth mass dependence, is consistent with zero within uncertainties.Comment: ISMD 2017 conference proceeding contributio

    Continuous Cluster Expansion for Field Theories

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    A new version of the cluster expansion is proposed without breaking the translation and rotation invariance. As an application of this technique, we construct the connected Schwinger functions of the regularized Ï•4\phi^4 theory in a continuous way
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