2014, Vol.17, No.4, pp.377-380
In 1936, Weisskopf [K. Dan. Vidensk. Selsk. Mat. Fys. Medd. XIV (1936)] showed that for vanishing electric or magnetic fields the strong-field behavior of the one-loop Euler–Heisenberg effective Lagrangian of quantum electrodynamics (QED) is logarithmic. This result can be generalized for different limits of the Lorentz invariants. The logarithmic dependence can be interpreted as a lowest-order manifestation of an anomalous power behavior of the effective Lagrangian of QED.
Key words:
QED, effective action, Euler–Heisenberg, strong fields
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