Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Springer eBooks

Spin-Paired Spin Eigenfunctions

Ruben Pauncz

Published Jan 1, 1979• 1 citation
Publisher
DOI
10.1007/978-1-4684-8526-4_5

Related papers

The Construction of Spin Eigenfunctions

Ruben Pauncz

Springer eBooks•Jan 1, 2000•55 citations

Spin Eigenfunctions: Construction and Use

Ruben Pauncz

•Jan 1, 1979•129 citations

Investigations of spin-eigenfunction correlated wavefunctions

Frank W. Bobrowicz

•Jan 1, 1974•0 citations

Genealogical Construction of Spin Eigenfunctions

Ruben Pauncz

Springer eBooks•Jan 1, 2000•1 citation

Construction of Spin Eigenfunctions by the Projection Operator Method

Ruben Pauncz

Springer eBooks•Jan 1, 1979•0 citations

N Representability of Fermion Density Matrices

Karl F. Freed

The proof of Smith, which gives the solution to the N-representability problem of the first-order density matrix for the case of N even and a nondegenerate energy eigenstate, is also shown to be valid for certain linear combinations of degenerate states. A connection is shown between these proper linear combinations and the eigenfuctions of a perturbed Hamiltonian for which all of the degeneracies have been lifted. For the case of S=0, all the eigenfunctions of the pth-order density matrix (natural p functions) can be taken to be eigenfunctions of total spin (Σ lim i=1pSi)2,and if orbital angular momentum is a constant of the motion, these natural p functions are eigenfunctions of the total orbital angular momentum for L=0. Simple wavefunctions are presented for which the natural 2 functions are not all eigenfunctions of the total pair spin. It is then shown that for MS=0 (any integral spin) or for L=1, ML=0, the natural 2 functions are eigenfunctions of (S1+S2)2 and (L1+L2)2, respectively.

The Journal of Chemical Physics•Nov 15, 1967•6 citations
The proof of Smith, which gives the solution to the N-representability problem of the first-order density matrix for the case of N even and a nondegenerate energy eigenstate, is also shown to be valid for certain linear combinations of degenerate states. A connection is shown between these proper linear combinations and the eigenfuctions of a perturbed Hamiltonian for which all of the degeneracies have been lifted. For the case of S=0, all the eigenfunctions of the pth-order density matrix (natural p functions) can be taken to be eigenfunctions of total spin (Σ lim i=1pSi)2,and if orbital angular momentum is a constant of the motion, these natural p functions are eigenfunctions of the total orbital angular momentum for L=0. Simple wavefunctions are presented for which the natural 2 functions are not all eigenfunctions of the total pair spin. It is then shown that for MS=0 (any integral spin) or for L=1, ML=0, the natural 2 functions are eigenfunctions of (S1+S2)2 and (L1+L2)2, respectively.