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Electric dipole hyperpolarizability and quadrupole polarizability of methane from finite-field coupled cluster and fourth-order many-body perturbation theory calculations

✍ Scribed by George Maroulis


Publisher
Elsevier Science
Year
1994
Tongue
English
Weight
562 KB
Volume
226
Category
Article
ISSN
0009-2614

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✦ Synopsis


We rely on a finite-field approach to calculate the static dipole ((u) and quadrupole ( C) polarizability and the first (/3) and second ( y) dipole hyperpolarizability of methane. Our best, CCSD( T) values for LY, /II and the mean value of y and C, obtained at&=2.052 aowitha (lls7p4d2f/6s2pld)[6s4p4d2f/4s2pld] basis set, area= 16.39 e* aaE;',jk -8.31 e3aeEb2, jk2312 e' ad Eb3 and c=60.45 e* a$ EC'. The derivatives of (Y, fi and y (symmetric stretch) at & were calculated at the SDQ-MP4 level of theory with a (1 ls7p4dlf/6s2pld)[6s4p4dlf/4s2pld] basis set: (da/dR),=15.7 ez us E;', (dp/dR),= -25.3 e'aa EC* and (dT/clR),=37.4~ lO*e'a$ EC".


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A fourth-order many-body perturbation th
✍ George Maroulis πŸ“‚ Article πŸ“… 1992 πŸ› Elsevier Science 🌐 English βš– 517 KB

The electric dipole moment (p,), dipole polarizability (CQ) and first (Balk) and second (v,,& dipole hyperpolarizability of ammonia were obtained from finite-field self-consistent-field (SCF) and complete fourth-order many-body perturbation theory (MP4) calculations. With z as the C, axis, the follo