ELSEVIER
21February1994
PhysicsLetters A 185 (1994) 435-439
PHYSICS LETTERS A
Numerical analysis of moments expansions
Jay D. Mancini 1, Yu Zhou, Peter F. Meier
Department of Physics, Universityof Zurich, CH-8057Zurich, Switzerland
William J. Massano
Department of Science, State Universityof New York, Maritime College, Ft. Schuyler, Bronx, NY 10465, USA
Janice D. Prie
Department of Physics, Fordham University, Bronx, NY 10458, USA
Received 21 September 1993;acceptedfor Publication 22 December 1993
Communicatedby J. Flouquet
Abstract
We present numerical results for the estimate of the ground state energy for two quantum many-body systems using the con-
nected moments expansion (CMX) and a newly developed alternate moments expansion (AMX ). Comparisons are made with
an equivalent Lanczos scheme which yields a variational upper bound for the ground state energy. For each system, the utility of
both expansions is evaluated as they pertain to relevant regions of parameter space. A brief description of the (numerical) nature
of the singularities which may arise in the series expansions is also given.
1. Introduction
A number of years ago an analytic expansion for
the ground state energy of any quantum system was
developed by Cioslowski [ 1 ]. This connected mo-
ments expansion (CMX) has its roots in the t-expan-
sion theorem of Horn and Weinstein [ 2 ] and is re-
lated to a cumulant expansion [ 3,4 ] thus giving it the
property of being size-extensive. Although there have
been numerous successes of the method cited in the
literature (see, e.g., Ref. [ 5 ] ), there also exist many-
body Hamiltonians for which, in certain regions of
parameter space, singularities in the expansion may
arise [6,7]. It should be emphasized that there are a
Permanent address: Department of Physics, FordhamUniver-
sity, Bronx, NY 10458,USA.
number of attractive features to any series which
arises from a moment expansion. These include fa-
cility in constructing any order in the series because
of the simple structure of the recursive algorithm, the
series to any order is size-extensive and, unlike for
perturbational techniques, there is no ambiguity in
the partitioning of the Hamiltonian into strong and
weak terms and no problems with (quasi-) degener-
act of the eigenfunctions of the unperturbed
Hamiltonian.
Recently Mancini, Zhou and Meier [ 8 ] have pre-
sented an in-depth theoretical study of a certain class
of moments expansion. Several properties of the con-
nected moments expansion were discussed as well as
an analytic proof of the cancellation of singularities
to all orders of the expansion. Also presented was the
derivation of an alternate moments expansion
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