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[ Last edited by huangck on 2006-4-7 at 20:57 ]
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huangck

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Submissions to:
Computational Physics
Condensed Matter
History of Physics
Instrumentation and Detectors
received from  Tue  4 Apr 06 20:00:02 GMT  to  Wed  5 Apr 06 20:00:03 GMT
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Paper: physics/0604033
Date: Wed, 5 Apr 2006 12:08:39 GMT   (21kb)

Title: Computation of Electrostatic Field near Three-Dimensional Corners and
Edges
Authors: N. Majumdar, S. Mukhopadhyay
Comments: Presented in International Conference on Computational and
Experimental Engineering and Sciences held at IIT Madras, Chennai, India,
during 1-6 December, 2005
Subj-class: Computational Physics; General Physics
\\
Theoretically, the electric field becomes infinite at corners of two and
three dimensions and edges of three dimensions. Conventional finite-element and
boundary element methods do not yield satisfactory results at close proximity
to these singular locations. In this paper, we describe the application of a
fast and accurate BEM solver (which usesexact analytic expressions to compute
the effect of source distributions on flatsurfaces) to compute the electric
field near three-dimensional corners and edges. Results have been obtained for
distances as close as 1$\mu m$ near the corner/edge and good agreement has been
observed between the present results and existing analytical solutions.
\\ ( http://arXiv.org/abs/physics/0604033 ,  21kb)
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Paper: physics/0604034
Date: Wed, 5 Apr 2006 12:16:45 GMT   (40kb)

Title: Development of a BEM Solver using Exact Expressions for Computing the
Influence of Singularity Distributions
Authors: S. Mukhopadhyay, N. Majumdar
Comments: Presented in International Conference on Computational and
Experimental Engineering and Sciences held at IIT Madras, Chennai, India
during 1-6 December, 2005
Subj-class: Computational Physics; General Physics
\\
Closed form expressions for three-dimensional potential and force field due
to singularities distributed on a finite flat surface have been used to develop
a fast and accurate BEM solver. The exact expressions have been investigated in
detail and found to be valid throughout the complete physical domain. Thus, it
has been possible to precisely simulate the complicated characteristics of the
potential and force field in the near-field domain. The BEM solver has been
used to compute the capacitance of a unit square plate and a unit cube. The
obtained values have compared well with very accurate values of the
capacitances available in the literature.
\\ ( http://arXiv.org/abs/physics/0604034 ,  40kb)
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Paper: physics/0604035
Date: Wed, 5 Apr 2006 12:54:45 GMT   (201kb)

Title: Computation of Electrostatic Properties of 3D MEMS Structures
Authors: N. Majumdar, S. Mukhopadhyay
Comments: Presented in International Conference on MEMS and Semiconductor
Nanotechnology held at IIT Kharagpur, Kharagpur, India during 20-22 December,
2005
Subj-class: Computational Physics; General Physics
\\
Micro-Electro-Mechanical Systems (MEMS) normally have fixed or moving
structures with cross-sections of the order of microns ($\mu m$) and lengths of
the order of tens or hundreds of microns. These structures are often plates or
array of thin beams which, owing to their smallness, can be moved or deflected
easily through the application of low voltages. Since electrostatic forces play
a very major role in maneuvering these devices, a thorough understanding of the
electrostatic properties of these structures is of critical importance,
especially in the design phase of MEMS. In many cases, the electrostatic
analysis of MEMS is carried out using boundary element method (BEM), while the
structural analysis is carried out using finite element method (FEM). In this
paper, we focus on accurate electrostatic analysis of MEMS using BEM. In
particular, we consider the problem of computing the charge distribution and
capacitance of thin conducting plates relevant to the numerical simulation of
MEMS. The reason behind the accuracy of the solver is the fact that it uses
closed-form analytic expressions that are valid seamlessly throughout the
physical domain for computing the influence coefficients. Thus, it is possible
to avoid one of the most serious approximations of the BEM, namely, the
assumption that the effect of a charge distributed over a boundary element can
be approximated by charge located at the centroid of the element. Comparison
with other results available in the literature seems to indicate that the
present results are more accurate than the existing ones.
\\ ( http://arXiv.org/abs/physics/0604035 ,  201kb)
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Paper: cond-mat/0604124
Date: Wed, 5 Apr 2006 16:25:26 GMT   (156kb)

Title: Critical behavior of the random-anisotropy model in the
strong-anisotropy limit
Authors: Francesco Parisen Toldin, Andrea Pelissetto, Ettore Vicari
Comments: 24 pages, 13 figs
Subj-class: Disordered Systems and Neural Networks
\\
We investigate the nature of the critical behavior of the random-anisotropy
Heisenberg model (RAM), which describes a magnetic system with random uniaxial
single-site anisotropy, such as some amorphous alloys of rare earths and
transition metals. In particular, we consider the strong-anisotropy limit
(SRAM), in which the Hamiltonian can be rewritten as the one of an Ising
spin-glass model with correlated bond disorder. We perform Monte Carlo
simulations of the SRAM on simple cubic L^3 lattices, up to L=30, measuring
correlation functions of the replica-replica overlap, which is the order
parameter at a glass transition. The corresponding results show critical
behavior and finite-size scaling. They provide evidence of a finite-temperature
continuous transition with critical exponents $\eta_o=-0.24(4)$ and
$\nu_o=2.4(6)$. These results are close to the corresponding estimates that
have been obtained in the usual Ising spin-glass model with uncorrelated bond
disorder, suggesting that the two models belong to the same universality class.
We also determine the leading correction-to-scaling exponent finding $\omega =
1.0(4)$.
\\ ( http://arXiv.org/abs/cond-mat/0604124,  156kb)
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Paper: cond-mat/0604126
Date: Wed, 5 Apr 2006 15:47:35 GMT   (81kb)

Title: Strong disorder renormalization group study of S=1/2 Heisenberg
antiferromagnet layers/bilayers with bond randomness, site dilution and dimer
dilution
Authors: Yu-Cheng Lin, Heiko Rieger, Nicolas Laflorencie, and Ferenc Igloi
Comments: 12 pages, 13 figures
Subj-class: Disordered Systems and Neural Networks
\\
Using a numerical implementation of strong disorder renormalization group, we
study the low-energy, long-distance properties of layers and bilayers of $S =
1/2$ Heisenberg antiferromagnets with different type of disorder: bond
randomness, site and dimer dilution. Generally the systems exhibit an ordered
and a disordered phase separated by a phase boundary on which the static
critical exponents appear to be independent of bond randomness in the strong
disorder regime, while the dynamical exponent is a continuous function of the
bond disorder strength. The low-energy fixed points of the off-critical phases
are affected by the actual form of the disorder, and the disorder induced
dynamical exponent depends on the disorder strength. As the strength of bond
disorder is increased, there is a set of crossovers in the properties of the
low-energy singularities. For weak disorder quantum fluctuations play the
dominant role. For intermediate disorder non-localized disorder fluctuations
are relevant, which become localized for even stronger bond disorder. We also
present some quantum Monte Carlo simulations results to support the strong
disorder renormalization approach.
\\ ( http://arXiv.org/abs/cond-mat/0604126,  81kb)
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Paper: cond-mat/0604127
Date: Wed, 5 Apr 2006 11:49:12 GMT   (207kb)

Title: Excitation energy transfer between closely spaced multichromophoric
systems: Effects of band mixing and intraband relaxation
Authors: C. Didraga, V. A. Malyshev, and J. Knoester
Comments: 13 pages, 6 PostScript figures
Subj-class: Disordered Systems and Neural Networks; Materials Science
\\
We theoretically analyze the excitation energy transfer between two closely
spaced linear molecular J-aggregates, whose excited states are Frenkel
excitons. The aggregate with the higher (lower) exciton band edge energy is
considered as the donor (acceptor). The celebrated theory of F\"orster
resonance energy transfer (FRET), which relates the transfer rate to the
overlap integral of optical spectra, fails in this situation. We point out that
in addition to the well-known fact that the point-dipole approximation breaks
down (enabling energy transfer between optically forbidden states), also the
perturbative treatment of the electronic interactions between donor and
acceptor system, which underlies the F\"orster approach, in general loses its
validity due to overlap of the exciton bands. We therefore propose a
nonperturbative method, in which donor and acceptor bands are mixed and the
energy transfer is described in terms of a phonon-assisted energy relaxation
process between the two new (renormalized) bands. The validity of the
conventional perturbative approach is investigated by comparing to the
nonperturbative one; in general this validity improves for lower temperature
and larger distances (weaker interactions) between the aggregates. We also
demonstrate that the interference between intraband relaxation and energy
transfer renders the proper definition of the transfer rate and its evaluation
from experiment a complicated issue, which involves the initial excitation
condition.
\\ ( http://arXiv.org/abs/cond-mat/0604127,  207kb)
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Paper: cond-mat/0604130
Date: Wed, 5 Apr 2006 12:37:17 GMT   (55kb)

Title: Exciton Dephasing and Thermal Line Broadening in Molecular Aggregates
Authors: D. J. Heijs, V. A. Malyshev, and J. Knoester
Comments: 11 pages, 3 PostScript figures
Subj-class: Disordered Systems and Neural Networks; Materials Science
Journal-ref: J. Lumin. 119-120, 271 (2006)
\\
Using a model of Frenkel excitons coupled to a bath of acoustic phonons in
the host medium, we study the temperature dependence of the dephasing rates and
homogeneous line width in linear molecular aggregates. The model includes
localization by disorder and predicts a power-law thermal scaling of the
effective homogeneous line width. The theory gives excellent agreement with
temperature dependent absorption and hole-burning experiments on aggregates
and more.........................
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