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The Chiral Magnetic Effect (0808.3382v1)

Published 25 Aug 2008 in hep-ph and hep-th

Abstract: Topological charge changing transitions can induce chirality in the quark-gluon plasma by the axial anomaly. We study the equilibrium response of the quark-gluon plasma in such a situation to an external magnetic field. To mimic the effect of the topological charge changing transitions we will introduce a chiral chemical potential. We will show that an electromagnetic current is generated along the magnetic field. This is the Chiral Magnetic Effect. We compute the magnitude of this current as a function of magnetic field, chirality, temperature, and baryon chemical potential.

Citations (1,409)

Summary

  • The paper demonstrates that topological transitions in the quark-gluon plasma induce chirality and an electromagnetic current using QCD principles.
  • It employs four distinct approaches, including energy balance and Dirac equation solutions, to phenomenologically compute the induced current.
  • The study offers predictive insights for heavy-ion collision experiments and proposes applications such as a 'chiral battery' in material science.

An Analysis of the Chiral Magnetic Effect

The paper "The Chiral Magnetic Effect" by Fukushima, Kharzeev, and Warringa provides a detailed exploration of a significant phenomenon in quantum chromodynamics (QCD) termed the Chiral Magnetic Effect (CME). The crucial premise here revolves around how topological charge-changing transitions, driven by the axial anomaly in the quark-gluon plasma (QGP), generate chirality and subsequently lead to an electromagnetic current parallel to an external magnetic field.

At the outset, the paper introduces the concept of the quark-gluon plasma, drawing connections to the early universe just after the Big Bang, an era where this state of matter was dominant. The contemporary paper of QGP is facilitated by heavy-ion collisions as conducted at RHIC and other facilities like LHC, FAIR, and NICA.

QCD predicts that in the QGP phase, topologically non-trivial gluon configurations, characterized by a winding number, play a significant role. This winding number remains invariant under smooth deformations, thereby showing its topological nature. At elevated temperatures pertinent to QGP, transitions between these configurations are no longer suppressed — they occur as sphalerons. These transitions induce a chirality, i.e., changing left-handed into right-handed quarks or vice versa, owing to the axial anomaly.

The theoretical underpinnings of the CME are centered around introducing an external magnetic field to a system bereft of parity and CP violation. The paper portrays how a chiral chemical potential introduced in this environment leads to the generation of an electromagnetic current parallel to the magnetic field, quantified for its magnitude concerning factors including chirality and temperature. This insight is crucial as it extends the discussion to potential applications such as in heavy-ion collisions, where observing charge separation driven by the CME could provide direct evidence of these topological effects in QCD.

The paper details the methodology and theoretical models used to compute this current using four distinct approaches. These approaches include an energy balance argument, solving the Dirac equation, using a derivative expansion of the effective action, and studying the thermodynamic potential. Each approach underscores the robustness of the CME, noting its independence from parameters such as mass and temperature, a consequence of the interplay between the QCD and electromagnetic anomalies.

Of particular interest are the numerical results presented, exemplifying how the induced current varies with external parameters, and supportive analytical approximations that foster a deeper understanding of the CME in different regimes of the QGP. Additionally, adapting this analysis to a multi-flavor QCD system further articulates its relevance in experimental settings like heavy-ion collisions, offering observable predictions of charge separation.

Finally, the authors propose hypothetical applications, such as a "chiral battery," drawing parallels between theoretical predictions and practical implementations. This underlines the broader relevance of the CME beyond theoretical physics, suggesting novel technological applications through material science featuring charged quasiparticles.

In conclusion, the paper on the Chiral Magnetic Effect provides an insightful and comprehensive analysis of how topological phases in QCD can induce macroscopic electromagnetic phenomena, with profound implications for both theoretical physics and potential practical applications. Future developments in this area could lead to enhanced understanding and observation of QCD topological features, offering novel insights into high-energy physics as well as innovative technological advancements.