FACTORIZATION OF THE MATRIX ELEMENTS OF THREE-ELECTRON OPERATORS USED IN CONFIGURATION-INTERACTION STUDIES OF THE ATOMICfSHELL

1996 ◽  
Vol 62 (1) ◽  
pp. 51-75 ◽  
Author(s):  
B.R. JUDD ◽  
EDWIN LO
Author(s):  
Stefan Hollands

AbstractWe introduce a new approach to find the Tomita–Takesaki modular flow for multi-component regions in general chiral conformal field theory. Our method is based on locality and analyticity of primary fields as well as the so-called Kubo–Martin–Schwinger (KMS) condition. These features can be used to transform the problem to a Riemann–Hilbert problem on a covering of the complex plane cut along the regions, which is equivalent to an integral equation for the matrix elements of the modular Hamiltonian. Examples are considered.


Author(s):  
Mariusz Pawlak ◽  
Marcin Stachowiak

AbstractWe present general analytical expressions for the matrix elements of the atom–diatom interaction potential, expanded in terms of Legendre polynomials, in a basis set of products of two spherical harmonics, especially significant to the recently developed adiabatic variational theory for cold molecular collision experiments [J. Chem. Phys. 143, 074114 (2015); J. Phys. Chem. A 121, 2194 (2017)]. We used two approaches in our studies. The first involves the evaluation of the integral containing trigonometric functions with arbitrary powers. The second approach is based on the theorem of addition of spherical harmonics.


2016 ◽  
Vol 25 (7) ◽  
pp. 073101 ◽  
Author(s):  
Wang Luo ◽  
Rui Li ◽  
Zhiqiang Gai ◽  
RuiBo Ai ◽  
Hongmin Zhang ◽  
...  

2009 ◽  
Vol 2 (S2) ◽  
pp. 13-20 ◽  
Author(s):  
Uzi Kaldor ◽  
Henry F. Schaefer ◽  
Frank E. Harris

1977 ◽  
Vol 32 (8) ◽  
pp. 897-898 ◽  
Author(s):  
Y. K. Chan ◽  
B. S. Rao

Abstract The radial Schrödinger wave equation with Morse potential function is solved for HF molecule. The resulting vibration-rotation eigenfunctions are then used to compute the matrix elements of (r - re)n. These are combined with the experimental values of the electric dipole matrix elements to calculate the dipole moment coefficients, M 1 and M 2.


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