๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

On the Generation of Operator Equivalents and the Calculation of Their Matrix Elements

โœ Scribed by I.D. Ryabov


Publisher
Elsevier Science
Year
1999
Tongue
English
Weight
64 KB
Volume
140
Category
Article
ISSN
1090-7807

No coin nor oath required. For personal study only.

โœฆ Synopsis


To find all components T ุŽq (k) โ€ซุโ€ฌ N k,q J ุŽ q ยฅ mโ€ซ0ุโ€ฌ kุŠq (ุŽ1) kุŠm a(k, q; m)J z m (0 < q < k) of an irreducible tensor operator of rank k, a recursion formula for the coefficients a(k, q; m) is derived. Various kinds of operator equivalents and forms of their expression are examined. Matrix elements of operator equivalents are expressed through the coefficients a(k, q; m). A table for the coefficients a(k, q; m) with k โ€ซุโ€ฌ 2, 4, and 6 is given.


๐Ÿ“œ SIMILAR VOLUMES


On the rapid evaluation of cofactors in
โœ Fokke Dijkstra; Joop H. Van Lenthe ๐Ÿ“‚ Article ๐Ÿ“… 1998 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 153 KB

The calculation of matrix elements involving nonorthogonal orbitals is speeded up by recognizing the orthogonalities between orbitals, leading to generalized Slater rules. The block structure present in the overlap matrix makes an efficient evaluation of its cofactors possible. These cofactors are c

Symmetry reduction of the matrix element
โœ Shi-Jun Zhong; Yin-Gui Wang; Qian-Er Zhang ๐Ÿ“‚ Article ๐Ÿ“… 1996 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 674 KB

Local coordinate systems are chosen for each quadruple of atoms relative to a four-center integral, in order to avoid linear combinations of orbitals when symmetry operations perform on an orbital. This choice can utilize the complete molecular symmetry to attain the optimal number of symmetry-uniqu

Generalized Hankel operators and the gen
โœ Wolfgang Knirsch; Georg Schneider ๐Ÿ“‚ Article ๐Ÿ“… 2006 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 168 KB

## Abstract In this paper we consider Hankel operators $ \tilde H \_{{\bar z}^k}$ = (__Id__ โ€“ __P__ ~1~)$ \bar z^k $ from __A__ ^2^(โ„‚, |__z__ |^2^) to __A__ ^2,1^(โ„‚, |__z__ |^2^)^โŠฅ^. Here __A__ ^2^(โ„‚, |__z__ |^2^) denotes the Fock space __A__ ^2^(โ„‚, |__z__ |^2^) = {__f__: __f__ is entire and โ€–__f_