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Production of particle-antiparticle pairs by a high-energy probe photon propagating through a high-intensity laser field is considered in the nonperturbative interaction regime.
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We note that an onset of nonperturbative signatures has been seen in SLAC ; see also H. R. Reiss, Eur. Phys. J. D 55
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The rate enhancement reported in Kampfer has a different nature as it results from the broad frequency spectrum of a short laser pulse and applies to the perturbative regime
Cited in the paper.
The spin degree of freedom of the electron shall not be accounted for in our calculation. This simplification, which renders the physical content of the equations more transparent, is enabled by the fact that the production rates for scalar and fermion pairs coincide, apart from an overall numerical prefactor of order 0.1; see Eq. (35) in Selym
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For comparison we note that a production rate of 2.5 × 10 − 15 m 2.5\times 10^{-15}m ( 3.9 × 10 − 13 m 3.9\times 10^{-13}m ) would result in Fig. 1
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In the case of commensurate laser frequencies (e.g., when ω 1 \omega_{1} is a harmonic of ω 2 \omega_{2} ) interference terms can arise in the square of the S S matrix; see Fofanov or S. Augustin and C. Müller, Phys. Rev. A 88
2013
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Intense extreme-ultraviolet photon pulses can be generated through harmonic emission from laser-irradiated plasma surfaces; see, e.g., C. Rödel et al
2013
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W. P. Leemans et al
2013
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