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Chiral Magnetic Effect and the Heisenberg–Euler Lagrangian


In our letter we establish coupling of the effective Heisenberg–Euler Lagrangian on the order of 1/m4 and the Chiral Magnetic Effect known for a massless particles. We consider a generalization of the effective Heisenberg–Euler Lagrangian from QED to QCD and then calculate the induced vector current. Further, considering the vector current, we establish a method to connect the perturbative result with the Chiral Magnetic Effect. We formulate the rule of transit from perturbation to nonperturbation (formula (5)) and obtain the well-known result for a massless particles.

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Correspondence to D. A. Shohonov.

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Teryaev, O.V., Shohonov, D.A. Chiral Magnetic Effect and the Heisenberg–Euler Lagrangian. Phys. Part. Nuclei Lett. 19, 317–319 (2022).

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