A Fifth-order Multi-perturbation Derivation of the Energy Coefficients of Polyatomic Molecules

A multiperturbation theory has been developed for molecular systems. In the present paper we extend this theory to fifth order in the energy. The "bare-nucleus" hydrogenic function is chosen as the zero-order wave function rather than the more customary hartree-fock function. With this cho...

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Main Authors: Moh'd Abu-Jafar, Sharif Musameh, Issam Abdelraziq
Format: Article
Language:English
Published: An-Najah National University 1996-09-01
Series:مجلة جامعة النجاح للأبحاث العلوم الطبيعية
Online Access:https://journals.najah.edu/media/journals/full_texts/fifth-order-multi-perturbation-derivation-energy-coefficients-polyatomic-molecules.pdf
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author Moh'd Abu-Jafar
Sharif Musameh
Issam Abdelraziq
author_facet Moh'd Abu-Jafar
Sharif Musameh
Issam Abdelraziq
author_sort Moh'd Abu-Jafar
collection DOAJ
description A multiperturbation theory has been developed for molecular systems. In the present paper we extend this theory to fifth order in the energy. The "bare-nucleus" hydrogenic function is chosen as the zero-order wave function rather than the more customary hartree-fock function. With this choice the multiperturbation wave functions are independent of the nuclear charges and of the total number of nuclear centers and electrons for the molecule and are thus completely transferable to other systems. Making the simplest possible choice, we describe an n-electron, m-center polyatomic molecule as n "hydrogenic" electrons on a single center perturbed by electron-electron and electron-nucleus coulomb interactions. With this choice of zero-order Hamiltonian (H0) the first-order wave function for any polyatomic molecule will consist entirely of two-electron, one-center and one-electron, two-center first-order wave functions. These are exactly transferable from calculations on He-like and H2-like systems. To calculate the first-order and second order correction for the wave function of any polyatomic molecule, we need the first-order and second-order correction for a two-electron atomic wave function, the first-order and second-order correction for a one-electron diatomic molecular wave function and some additional mixed second-order corrections. The wave functions necessary will be two-center, one-electron at most. The second-order wave function for a polyatomic molecule contains additional contributions which cannot be obtained from the simple subsystems, but represent multiple perturbation contributions which are two electron diatomic, and one-electron triatomic in character. The expressions for the multiperturbation energy-expansion coefficients through fifth order are derived.
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spelling doaj-art-10afd5d3c1e1443984cdba0c8f2e94272025-08-20T03:44:04ZengAn-Najah National Universityمجلة جامعة النجاح للأبحاث العلوم الطبيعية1727-21142311-88651996-09-01101718210.35552/anujr.a.10.1.401A Fifth-order Multi-perturbation Derivation of the Energy Coefficients of Polyatomic MoleculesMoh'd Abu-Jafar0Sharif Musameh1Issam Abdelraziq2NoneNonePhysics Department, Faculty of Science, An-Najah National University, Nablus, PalestineA multiperturbation theory has been developed for molecular systems. In the present paper we extend this theory to fifth order in the energy. The "bare-nucleus" hydrogenic function is chosen as the zero-order wave function rather than the more customary hartree-fock function. With this choice the multiperturbation wave functions are independent of the nuclear charges and of the total number of nuclear centers and electrons for the molecule and are thus completely transferable to other systems. Making the simplest possible choice, we describe an n-electron, m-center polyatomic molecule as n "hydrogenic" electrons on a single center perturbed by electron-electron and electron-nucleus coulomb interactions. With this choice of zero-order Hamiltonian (H0) the first-order wave function for any polyatomic molecule will consist entirely of two-electron, one-center and one-electron, two-center first-order wave functions. These are exactly transferable from calculations on He-like and H2-like systems. To calculate the first-order and second order correction for the wave function of any polyatomic molecule, we need the first-order and second-order correction for a two-electron atomic wave function, the first-order and second-order correction for a one-electron diatomic molecular wave function and some additional mixed second-order corrections. The wave functions necessary will be two-center, one-electron at most. The second-order wave function for a polyatomic molecule contains additional contributions which cannot be obtained from the simple subsystems, but represent multiple perturbation contributions which are two electron diatomic, and one-electron triatomic in character. The expressions for the multiperturbation energy-expansion coefficients through fifth order are derived.https://journals.najah.edu/media/journals/full_texts/fifth-order-multi-perturbation-derivation-energy-coefficients-polyatomic-molecules.pdf
spellingShingle Moh'd Abu-Jafar
Sharif Musameh
Issam Abdelraziq
A Fifth-order Multi-perturbation Derivation of the Energy Coefficients of Polyatomic Molecules
مجلة جامعة النجاح للأبحاث العلوم الطبيعية
title A Fifth-order Multi-perturbation Derivation of the Energy Coefficients of Polyatomic Molecules
title_full A Fifth-order Multi-perturbation Derivation of the Energy Coefficients of Polyatomic Molecules
title_fullStr A Fifth-order Multi-perturbation Derivation of the Energy Coefficients of Polyatomic Molecules
title_full_unstemmed A Fifth-order Multi-perturbation Derivation of the Energy Coefficients of Polyatomic Molecules
title_short A Fifth-order Multi-perturbation Derivation of the Energy Coefficients of Polyatomic Molecules
title_sort fifth order multi perturbation derivation of the energy coefficients of polyatomic molecules
url https://journals.najah.edu/media/journals/full_texts/fifth-order-multi-perturbation-derivation-energy-coefficients-polyatomic-molecules.pdf
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