1961
DOI: 10.1051/jphysrad:019610022010900
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Sur le calcul variationnel des propriétés moléculaires

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Cited by 5 publications
(2 citation statements)
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“…Condition ($, I $1) = 0, which involves (Olr10) = 0 (i.e., the r origin is at the center of electronic charge), ensures that is normalized through second order, and the minimal second order energy is [ 15,201 + (If (+, 1 # 0 and E"' # 0, the u , solution for v = 0 does not give the minimal second-order energy, and the former E'*' expression is no longer available [21]).…”
Section: Time-dependent Schrodinger Equation At the First-order Pertumentioning
confidence: 99%
“…Condition ($, I $1) = 0, which involves (Olr10) = 0 (i.e., the r origin is at the center of electronic charge), ensures that is normalized through second order, and the minimal second order energy is [ 15,201 + (If (+, 1 # 0 and E"' # 0, the u , solution for v = 0 does not give the minimal second-order energy, and the former E'*' expression is no longer available [21]).…”
Section: Time-dependent Schrodinger Equation At the First-order Pertumentioning
confidence: 99%
“…In our previous papers [1,22,23] we developed a variationperturbation approach [24,25] based on the use of a timedependent gauge-invariant (TDGI) operator able to give dynamic dipole polarizabilities a(u). This TDGI approach is used here and extended in order to obtain the third-order energy and to achieve the first dynamic hyperpolarizabilities from the erst-order perturbed ket function.…”
Section: Introductionmentioning
confidence: 99%