Abstract
Anomalous hydrodynamics is a low-energy effective theory that captures effects of quantum anomalies. We develop a numerical code of ideal anomalous hydrodynamics and apply it to dynamics of heavy-ion collisions, where anomalous transports are expected to occur. We discuss implications of the simulations for possible experimental observations of anomalous transport effects. From analyses of the charge-dependent elliptic flow parameters (v2±) as a function of the net charge asymmetry A±, we find that the linear dependence of Δv2±≡v2−−v2+ on the net charge asymmetry A± can come from a mechanism unrelated to anomalous transport effects. Instead, we find that a finite intercept Δv2±(A±=0) can come from anomalous effects.
Highlights
Anomalous hydrodynamics is a low-energy effective theory that captures effects of quantum anomalies
Introduction.— Macroscopic transport phenomena induced by the triangle anomalies have recently attracted much attention. One such example is the chiral magnetic(separation) effect (CME/CSE), which states that a dissipationless vector(axial) current is generated along a magnetic field [1,2,3,4]
The quark-gluon plasma (QGP) is experimentally produced in heavy-ion collisions at Relativistic Heavy Ion Collider (RHIC) in BNL, and Large Hadron Collider (LHC) in CERN
Summary
Anomalous hydrodynamics is a low-energy effective theory that captures effects of quantum anomalies. Since two charged nuclei collide at very high energy, extremely strong magnetic fields are created in off-central collisions, along which vector and axial currents flow due to CME/CSE [1,2,3,4]. It brings a charge quadrupole deformation in the QGP, which could be used as an experimental signal of anomalous transport effects [21, 22].
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