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Coulomb operator

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Quantum mechanical operator used in the field of quantum chemistry
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The Coulomb operator, named after Charles-Augustin de Coulomb, is a quantum mechanical operator used in the field of quantum chemistry. Specifically, it is a term found in the Fock operator. It is defined as:

J ^ j ( 1 ) f i ( 1 ) = f i ( 1 ) | φ j ( 2 ) | 2 1 r 12 d r 2 {\displaystyle {\widehat {J}}_{j}(1)f_{i}(1)=f_{i}(1)\int {\left|\varphi _{j}(2)\right|}^{2}{\frac {1}{r_{12}}}\,dr_{2}}

where

J ^ j ( 1 ) {\displaystyle {\widehat {J}}_{j}(1)} is the one-electron Coulomb operator defining the repulsion resulting from electron j,
f i ( 1 ) {\displaystyle f_{i}(1)} is the one-electron wavefunction of the i t h {\displaystyle i^{th}} electron being acted upon by the Coulomb operator,
φ j ( 2 ) {\displaystyle \varphi _{j}(2)} is the one-electron wavefunction of the j t h {\displaystyle j^{th}} electron,
r i j {\displaystyle r_{ij}} is the distance between electrons ( i ) {\displaystyle (i)} and ( j ) {\displaystyle (j)} .

See also

References

  1. Ramachandran, K. I. (2008). Computational chemistry and molecular modeling : principles and applications. G. Deepa, K. Namboori. Berlin: Springer. p. 107. ISBN 978-3-540-77304-7. OCLC 272298712.
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