A New Wavelet-Based Paradigm for Hierarchical
Coarse-Graining applied to Materials Modeling*
Ahmed E. Ismail, Gregory C. Rutledge, and George Stephanopoulos
Department of Chemical Engineering, MIT, Cambridge, MA 02139
Abstract— We outline how the wavelet transform, a hi-
erarchical averaging scheme, can be used to perform both
structural and topological coarse-graining in systems with
multiscale physical behavior, such as Ising lattices and polymer
models. We illustrate how to create sampling mechanisms,
which we call wavelet-accelerated Monte Carlo (WAMC), to
study these systems and obtain qualitative and quantitatively
accurate results in orders of magnitude less time than using
atomistic simulations.
I. I NTRODUCTION
While there have been impressive computational gains
afforded in recent years through advances both in computer
hardware and in the expected gains predicted from Moore’s
law, it is also clear that relying on improvements in com-
putational performance will ultimately be insuf ficient for
advancing the state-of-the-art in molecular simulation. In re-
sponse, many researchers have turned their attention toward
the development of a variety of algorithms for advancing the
time and length scales accessible to molecular simulations.
One limitation common to many of these algorithms is
their limited focus—they are generally designed to study
only a specific set of molecular chemistries. However, it is
well known that many physical systems possess common
structural properties, including self-similarity. As a result,
we have created a new simulation paradigm for studying
systems with structured behavior over various length scales
which exploits these links.
Our method is based upon the wavelet transform [1–3,
among others]. Although most commonly used for signal
processing and image analysis, we use it for its data com-
pression properties. The basic principle in our application
of the wavelet transform is that we use a characteristic
property of our objects—such as the spin of a magnetic
particle, or the position of an atom along the backbone
of a chain molecule—as the basis for our sampling. The
wavelet transform is then used to develop coarse-grained
representations of “effective” or “block” variables, as well
as potentials, describing the behavior of the system over
successively larger length scales. This approach has several
advantages, including generality with respect to the range
of systems to which it can be applied; extensibility, as
it can be used as the basis for a hierarchical simulation
scheme; and ef ficiency, as the resulting algorithm is capable
of yielding qualitatively accurate predictions of behavior
over a wide range of parameters orders of magnitude faster
than is capable with traditional atomistic simulations. We
discuss our development of this paradigm, in the form
of a new simulation technique, wavelet-accelerated Monte
Carlo, through its application to lattice systems and to
polymer random walks.
To date, the wavelet framework transform has not been
extensively applied to models in statistical mechanics.
Huang uses wavelet analysis to observe the statistical dis-
tribution of multiplicity fluctuations in a lattice gas [4],
while Gamero et al. employ wavelets to introduce their
notion of multiresolution entropy, but for dynamic signal
analysis rather than statistical mechanics simulations [5].
O’Carroll attempts to establish a theoretical foundation
connecting wavelets to the block renormalization group
[6], [7]. The most extensive discussion of the relationship
between wavelets and renormalization group theory is a
recent monograph by Battle [8].
II. USING THE WAVELET TRANSFORM AS A
COARSE- GRAINING SCHEME
There are two principal means for carrying out coarse-
graining of a physical system: we can call these approaches
structural and topological. Structural approaches operate
on the simulation space, dividing it into regions, and then
combining the regions from one scale to another. Topolog-
ical approaches operate on the particles inserted into the
simulation space, so that the rules for coarse-graining the
system do not depend upon any specific physical structure
of the simulation space, such as a lattice, but instead upon
the structure of the particles. Ising lattices and polymer
chains typify each of these individual approaches. We show
how to develop coarse-grained simulations for each of these
models below.
A. The Ising model
The Ising model is the standard model for studying the
thermodynamic behavior of lattice systems, such as spin
magnets, lattice gases, and binary alloys [9]. The Hamil-
tonian for the Ising model, which contains both nearest-
neighbor pairwise interactions as well as interactions be-
tween lattice sites and an external field, can be generally
written in the form
−βH =
X
i
h
i
σ
i
+
X
i
X
j
J
ij
σ
i
σ
j
, (1)
where σ
i
is either the occupation number or the spin of
lattice site i, h
i
is the strength of the external field in the
Proceeding of the 2004 American Control Conference
Boston, Massachusetts June 30 - July 2, 2004
0-7803-8335-4/04/$17.00 ©2004 AACC
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