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Coupled Hartree Fock calculation of static dipole polarizabilities and shielding factors of open shell systems

✍ Scribed by A. Gupta; A. K. Bhattacharya; P. K. Mukherjee


Publisher
John Wiley and Sons
Year
1974
Tongue
English
Weight
442 KB
Volume
8
Category
Article
ISSN
0020-7608

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✦ Synopsis


Abstract

Static dipole polarizabilities and shielding factors for the 2__p__ open shell atomic systems are presented using coupled Hartree Fock theory in the framework of the Roothaan formalism. Calculations have been performed for the ground as well as for some valence excited states. A variational approach has been adopted for the determination of the first‐order perturbed functions. The results are compared with those obtained from the correlated calculations and other techniques. The shielding factor values are in excellent agreement with the theoretical N/Z ratio.


📜 SIMILAR VOLUMES


Coupled hartree–fock calculation of stat
✍ A. Gupta; H. P. Roy; P. K. Mukherjee 📂 Article 📅 1975 🏛 John Wiley and Sons 🌐 English ⚖ 335 KB

## Abstract In this paper a calculation of the static quadrupole polarizabilities and the shielding factors of the atoms and ions of the 2__p__ open shell systems is presented. A fully coupled Hartree–Fock method using the Roothaan formalism is adopted. Calculations have been done for the ground as

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✍ H. P. Roy; A. Gupta; P. K. Mukherjee 📂 Article 📅 1977 🏛 John Wiley and Sons 🌐 English ⚖ 381 KB

## Abstract In this paper static dipole polarizabilities and shielding factors of 3__p__ open‐shell atomic systems from A1 to C1 are presented using coupled Hartree‐Fock theory in the Roothaan scheme. The calculation was made for the ground as well as for some valence excited states of the ions. A

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✍ A. K. Bhattacharya; P. K. Mukherjee 📂 Article 📅 1973 🏛 John Wiley and Sons 🌐 English ⚖ 403 KB

## Abstract Uniform field quadrupole polarizabilities and shielding factors of the first three ions of 2‐, 3‐, and 4‐electron sequences in their ground states have been calculated in the coupled Hartree‐Fock (CHF) scheme. For comparison the uncoupled Hartree‐Fock (UHF) results are also presented. I