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The vacuum persistence probability, Pvac(t), for a system of charged fermions in a fixed, external, and spatially homogeneous electric field, was derived long ago by Schwinger; w≡-log[Pvac(t)]/Vt has often been identified as the rate at which fermion-antifermion pairs are produced per unit volume due to the electric field. In this paper, we separately compute exact expressions for both w and for the rate of fermion-antifermion pair production per unit volume, Γ, and show that they differ. While w is given by the standard Schwinger mechanism result of w=(qE)²4π³∑ₙ₌₁^∞1n²exp(-nπm²qE), the pair production rate, Γ, is just the first term of that series. Our calculation is done for a system with periodic boundary conditions in the A₀=0 gauge but the result should hold for any consistent set of boundary conditions. We discuss, the physical reason why the rates w and Γ differ.
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Cohen et al. (2008) studied this question.
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