Non-adiabatic matrix elements connecting the discrete and continuous spectra of the two-centre problem in quantum mechanics

1977 ◽  
Vol 10 (7) ◽  
pp. 1335-1343 ◽  
Author(s):  
L I Ponomarev ◽  
T P Puzynina ◽  
L N Somov
2003 ◽  
Vol 93 (1) ◽  
pp. 47-47
Author(s):  
A. C. Ilarraza-Lomelí ◽  
M. N. Valdés-Martínez ◽  
A. L. Salas-Brito ◽  
R. P. Martínez-y-Romero ◽  
H. N. Núñez-Yépez

2000 ◽  
Vol 53 (4) ◽  
pp. 613 ◽  
Author(s):  
A. M. Stewart

With the use of the generalised multipolar gauge, a completely general proof is obtained for a result asserted by J. H. Van Vleck in 1932 but never fully proved by him. Specifically it is demonstrated that the matrix elements of the magnetic moment operator are independent of the origin of the vector potential for electromagnetic fields that are non-uniform in space and non-constant in time. A general survey of the principles of the quantum mechanics of solid state and molecular magnetism is also given to set the problem in its context. Based on the multipolar gauge, a simple conversion of the interaction Hamiltonian from the form of A.p to E.r plus higher order terms is demonstrated.


The usual method of calculating the diagonal matrix elements of an integral power of the radius r in an inverse square quantum system is that due to Waller. His procedure is based on the Schrödinger form of the theory, and utilizes in particular the generating series for the Langueree polynomials. For negative powers, Dirac's very elegant theory of "q-numbers," developed in these 'proceedings' during the early days of quantum mechanics, furnishes an interesting alternative method which appears to have been overlooked, and which we believe is easier. From his theory the following rule can be derived: Suppose that we desire the mean value (diagonal element) of 1/r s , where s is an integer greater than unity. We write down the experssion with A(α l + β l e - i x + γ l e i x ) s-2 A = 16π 4 m 2 z 2 e 4 /( l + ½) n 3 h 4 , α l = 4π 2 m z e 2 / h 2 l ( l +1), β l = 2π 2 m Z e 2 / h 2 ( l +½)( l +1)[1-( l +1) 2 / n 2 ]½, γ l = 2π 2 m z e 2 / h 2 l ( l +½)[1- l 2 / n 2 ]½.


Author(s):  
Max Born ◽  
H. W. Peng

The difficulties met in the usual treatment of quantised field theories seem to us somewhat similar to those which occurred in Bohr's semi-classical quantum mechanics of particles. In this theory the orbits were described by Fourier series in the time; there was no exact correspondence between the periodic terms of this series and quantum transitions, but only an approximate one for terms of high order. Matrix mechanics considers not the Fourier series, but the single terms which are generalised into matrix elements having not one but two indices. This generalisation is founded on Ritz's combination principle.


2004 ◽  
Vol 59 (9) ◽  
pp. 568-590
Author(s):  
Wolfhard Koch ◽  
Bastian Freyb ◽  
Juan Francisco Sánchez Ruiza ◽  
Thomas Sciorc

The analysis based on Rüdenberg’s well-known letter of 1951, which has been outlined for molecules in a preceding contribution, has now been transfered to translational periodic systems in one, two, or three dimensions. Entitled “On the Three- and Four-Center Integrals in Molecular Quantum Mechanics”, this letter explicitly presents two approximations only for four-center repulsion integrals. When applied to some types of three-center repulsion integrals, however, these two recipes still imply considerable oversimplifications. Using both one-electron and two-electron routes of Rüdenberg’s expansion, such shortcomings can be avoided strictly. Starting from a simple “Unrestricted and Combined” (U&C) approximation scheme introduced elsewhere, an improved “Restricted and Combined” (R&C) approximation picture for Fock-matrix elements now will be outlined, which does not tolerate any unnecessary oversimplifications. Although the simplicity of the U&C scheme is lost in this case, R&C-approximated Fock-matrix elements still can be constructed from one- and twocenter integrals alone in an effective way. Moreover, due to their dependence on a single geometric parameter, all types of two-center integrals can be calculated in advance for about one hundred fixed interatomic distances at the desired level of sophistication, and stored once and for all. A cubic spline algorithm may be taken to interpolate the actual integral value from each precomputed list.


2003 ◽  
Vol 58 (12) ◽  
pp. 756-784 ◽  
Author(s):  
Wolfhard Koch ◽  
Bastian Freyb ◽  
Juan Francisco Sánchez Ruiza ◽  
Thomas Scior

Rüdenberg’s well-known letter of 1951 entitled “On the Three- and Four-Center Integrals in Molecular Quantum Mechanics” explicitly presents two approximation formulas for four-center repulsion integrals, only. When applied to some types of three-center repulsion integrals, however, these two recipes still imply considerable oversimplifications. Using both one-electron and two-electron routes of Rüdenberg’s truncated expansion, on the other hand, such shortcomings can be avoided strictly. Starting from four simple “Unrestricted and Combined” (U&C) approximation schemes introduced elsewhere, an improved “Restricted and Combined” (R&C) approximation picture for Fock-matrix elements now will be outlined, which does not tolerate any unnecessary oversimplifications. Although the simplicity of the U&C scheme is lost in this case, R&C-approximated Fock-matrix elements still can be constructed from one- and two-center integrals alone in an effective way. Moreover, due to their dependence on a single geometric parameter, all types of two-center integrals can be calculated in advance for about one hundred fixed interatomic distances at the desired level of sophistication and stored once and for all. A cubic spline algorithm may be taken to interpolate the actual integral value from each precomputed list.


2000 ◽  
Vol 53 (4) ◽  

With the use of the generalised multipolar gauge, a completely general proof is obtained for a result asserted by J. H. Van Vleck in 1932 but never fully proved by him. Specifically it is demonstrated that the matrix elements of the magnetic moment operator are independent of the origin of the vector potential for electromagnetic fields that are non-uniform in space and non-constant in time. A general survey of the principles of the quantum mechanics of solid state and molecular magnetism is also given to set the problem in its context. Based on the multipolar gauge, a simple conversion of the interaction Hamiltonian from the form of A.p to E.r plus higher order terms is demonstrated.


Sign in / Sign up

Export Citation Format

Share Document