## 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
Waller–Hartree spin-free method
✍ Scribed by T. K. Lim
- Publisher
- John Wiley and Sons
- Year
- 1974
- Tongue
- English
- Weight
- 656 KB
- Volume
- 8
- Category
- Article
- ISSN
- 0020-7608
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✦ Synopsis
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 present Waller‐Hartree spin function free method. There exists a one‐to‐one correspondence between Slater's determinantal wave function and the Waller–Hartree double determinantal wave function. Explicit expressions for the S^2^ operator, Löwdin's spin projector, matric basis and several different forms of spin‐projected functions are given for the Waller–Hartree formalism. The results are compared with other methods including those of Slater, Matsen, Gallup, Goddard and Segal. The differences are quite significant. New spin operators are worked out using creation‐destruction operators. A knowledge of group theory is not required in this Waller–Hartree method. We have also shown that the Waller–Hartree method is more convenient than Slater's method with spin functions especially in the evaluation of the functional ℋ︁Ψ/Ψ. The advantages and disadvantages in the use of a linear combination of N! Hartree products and linear combinations of all possible double determinants are discussed. In addition, a formula for the calculation of the Sanibel coefficients C(S, M, i) is obtained.
📜 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
## 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
## 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 pr