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This might be justified in view of the bonding (gerade) symmetry of the ground state of the H2, HD, and D2 molecules, and for the intensity regime below 2× 1014 W/cm2, considered in the present calculations.
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33644701012
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note
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We noted two misprints in Eqs. (96) and (98) of Ref., Sec. 6.4, which should read bn = (2 α′ λ) -2n ∑ m=0 ν/2 (α′/α) 2m m! (ν-2m) ! (n-m) ! [ν′ -2 (n-m)] !, I (s,p) = 2π exp (- p2 2) ∑ k=0 s/2 s! (s-2k) !k! 2k (ip) s-2k. For the ion χ ν′ ′ (x′) depends on different parameters x′ =R- Re′, and α′, which turns the integral over the internuclear coordinate R into an expression similar to those treated in quantum chemical calculations with Gaussian type orbitals. We found, however, that it is more convenient to compute the one dimensional vibrational transition integral by direct numerical quadrature, rather than from the analytical expressions.
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