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This dependence appears in Eq. (16) from γ which depends on R due to the conductivity tensor (18).
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This dependence appears in Eq. from γ which depends on R due to the conductivity tensor.
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The multiplier 2 appears as a result of different choices of the expressions for the EM wave field: in work 15, we set it as E0 exp [i (ωt-kr)]; but, here at Γ→0, we have E0 cos (ω0 t- k0 r) according to formula (1). The another multiplier π/2 results from the fact that we deal here with the Gaussian like, rather than rectangular pulse.
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The multiplier 2 appears as a result of different choices of the expressions for the EM wave field: in work 15, we set it as E0 exp [i (ωt-kr)]; but, here at Γ→0, we have E0 cos (ω0 t- k0 r) according to formula. The another multiplier π/2 results from the fact that we deal here with the Gaussian like, rather than rectangular pulse.
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