Department of Physics, University of Connecticut, Storrs Connecticut 06269, USA.
Phys Rev Lett. 2010 Jun 11;104(23):232301. doi: 10.1103/PhysRevLett.104.232301. Epub 2010 Jun 7.
We argue that the presence of a very strong magnetic field in the chirally broken phase induces inhomogeneous expectation values, of a spiral nature along the magnetic field axis, for the currents of charge and chirality, when there is finite baryon density or an imbalance between left and right chiralities. This "chiral magnetic spiral" is a gapless excitation transporting the currents of (i) charge (at finite chirality), and (ii) chirality (at finite baryon density) along the direction of the magnetic field. In both cases it also induces in the transverse directions oscillating currents of charge and chirality. In heavy ion collisions, the chiral magnetic spiral possibly provides contributions both to the out-of-plane and the in-plane dynamical charge fluctuations recently observed at BNL RHIC.
我们认为,在手征破缺相中存在很强的磁场时,在有限重子密度或左右手性之间存在不平衡时,电荷和手性的电流会沿着磁场轴产生螺旋性质的不均匀期望值。这种“手征磁场螺旋”是一种无间隙激发,它沿着磁场的方向传输(i)电荷(在有限手性时)和(ii)手性(在有限重子密度时)的电流。在这两种情况下,它也会在横向方向上产生电荷和手性的振荡电流。在重离子碰撞中,手征磁场螺旋可能对最近在 BNL RHIC 观测到的平面外和平面内动态电荷涨落都有贡献。