## Abstract In this paper we show that with the equivalent transformation **P**^__r__^ = (−1)^__P__^(**P**^σ^)^−1^ the spin function dependent methods such as Slater's method without group theory or Goddard's method with group theory differ only in different antisymmetric requirements from the pres
Young operators and the Waller–Hartree spinfree method
✍ Scribed by T. K. Lim
- Publisher
- John Wiley and Sons
- Year
- 1975
- Tongue
- English
- Weight
- 220 KB
- Volume
- 9
- Category
- Article
- ISSN
- 0020-7608
No coin nor oath required. For personal study only.
✦ Synopsis
Abstract
The basic equivalent transformation P^σ^ = (−1)^p^ (P^r^)^−1^ as developed recently [6] is used to transform between the Young operators for a two‐row standard tableau and its conjugate two‐column standard tableau. These Young operators are shown to be the Löwdin spin projectors in the spin function‐dependent methods and the spin projectors in the spin function‐free methods. The sandwich operator of Gallup and the last diagonal element of the matric basis of Matsen are shown to be the special cases of our more general matric projectors. Several different forms of the Löwdin spin projectors, spin projectors, and matric projectors are shown and their relations are discussed.
📜 SIMILAR VOLUMES
## Abstract The relations between the Waller–Hartree spin‐free method and the symmetric group theory are given. It is shown that the Gallup method is a special case of ours with __S__ = __M__. Furthermore, all the irreducible representation matrices and other matrices needed are written explicitly
The Wallcr-Hartrce method is apphcd to perform CI calculations. It results in a generahzation of the method utilizing the symmetric group in tams of "sandwich representations". rcccntly developed by Gallup. The spin dcgcncracy difficuIty isovcrcomc efficiently. Results are prcscnted for tip and comp
## Abstract Spin densities in the Waller–Hartree spin‐free method were found to be the same as in the spin‐projected Slater determinant method. The reduced spin projector **__Q__** is introduced and its relation with the spin projector **__P__** is discussed. An equation is obtained to show that a
## Abstract A many‐electron theory is developed for the determination of pure spin state wave‐functions and energies to avoid the difficulties in doing integration. The Waller–Hartree pure spin state wave‐functions are very convenient for this purpose. The required explicit formulas for the values