Outline of a perturbation theory of the hydrogen molecule. — III

1964 ◽  
Vol 31 (6) ◽  
pp. 1258-1264 ◽  
Author(s):  
E. Corinaldesi
2019 ◽  
Vol 100 (3) ◽  
Author(s):  
Jacek Komasa ◽  
Mariusz Puchalski ◽  
Paweł Czachorowski ◽  
Grzegorz Łach ◽  
Krzysztof Pachucki

1967 ◽  
Vol 45 (8) ◽  
pp. 2533-2542 ◽  
Author(s):  
M. Cohen ◽  
R. P. McEachran ◽  
Sheila D. McPhee

Properties of the lowest even and odd δ states of the hydrogen molecule–ion have been calculated using approximate wave functions. These were derived using a combination of Rayleigh–Schrödinger perturbation theory and variational methods, which have been applied previously to calculate the corresponding wave functions of the lowest σ and π states. Our total molecular energies are in excellent agreement with the recent exact calculations of Hunter and Pritchard (1967). A simple criterion is suggested for judging the accuracy of the approximate orbitals, which indicates that all the molecular properties calculated will be accurate over a wide range of internuclear separations.


1970 ◽  
Vol 48 (17) ◽  
pp. 1991-1995 ◽  
Author(s):  
M. Cohen ◽  
B. W. Southern

The leading terms in a single-center expansion of the static dipole polarizability tensor of the hydrogen molecule has been calculated by means of perturbation theory.


The perturbation theory developed in the preceding part of this series is used to calculate the properties of a set of molecular models which are formed by continuously varying the charges on the protons of the hydrogen molecule. The binding energies and heats of reaction of all such model molecules are calculated, and it is found that the thermochemical behaviour of the models reproduces several interesting features observed in the behaviour of real molecules. For these models the bonding energy of a molecule of type AB is usually greater than the mean value of this quantity for A 2 and B 2 , but this is due mainly to the reduction of the internuclear repulsion energy and not to the ionic-covalent resonance.


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