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2009 J. Phys.: Condens. Matter 21 474204 (10pp) doi: 10.1088/0953-8984/21/47/474204
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Abstract.
The group function theory by Tolpygo and McWeeny is a useful tool in treating quantum
systems that can be represented as a set of localized electronic groups (e.g. atoms, molecules
or bonds). It provides a general means of taking into account intra-correlation effects inside
the groups without assuming that the interaction between the groups is weak. For
non-orthogonal group functions the arrow diagram (AD) technique provides a convenient
procedure for calculating matrix elements
of arbitrary symmetrical operators
which are needed, for example, for calculating the total energy of the system or its
electron density. The total wavefunction of the system
is represented as an antisymmetrized product of non-orthogonal electron group functions
ΦI of each
group I
in the system. However, application of the AD theory to extended (e.g. infinite)
systems (such as biological molecules or crystals) is not straightforward,
since the calculation of the mean value of an operator requires that each
term of the diagram expansion be divided by the normalization integral
S =
Ψ|Ψ
which is given by an AD expansion as well. In our previous work, we cast the mean value
of a symmetrical operator
in the form of an AD expansion which is a linear combination of linked (connected) ADs
multiplied by numerical pre-factors. To obtain the pre-factors, a method based on power
series expansion with respect to overlap was developed and tested for a simple 1D
Hartree–Fock (HF) ring model. In the present paper this method is first tested on a 2D HF
model, and we find that the power series expansion for the pre-factors converges extremely
slowly to the exact solution. Instead, we suggest another, more powerful, method
based on a continued fraction expansion of the pre-factors that approaches the
exact solution much faster. The method is illustrated on the calculation of the
electron density for the 2D HF model. It provides a powerful technique for treating
extended systems consisting of a large number of strongly localized electronic groups.
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