An effective field theory exists describing a very large class of
biophysically interesting Coulomb gas systems: the lowest order (mean-field)
version of this theory takes the form of a generalized Poisson-Boltzmann
theory. Interaction terms depend on details (finite-size effects, multipole
properties, etc). Convergence of the loop expansion holds only if mutual
interactions of mobile charges are small compared to their interaction with the
fixed-charge environment, which is frequently not the case. Problems with the
strongly- coupled effective theory can be circumvented with an alternative
local lattice formulation, with real positive action. In realistic situations,
with variable dielectric, a determinant of the Poisson operator must be
inserted to generate correct electrostatics. Methods adopted from unquenched
lattice QCD do this very efficiently.
%0 Generic
%1 Duncan2006Lattice
%A Duncan, Anthony
%D 2006
%K medicine
%T Lattice Field Theory Methods in Modern Biophysics
%U http://arxiv.org/abs/hep-lat/0609064
%X An effective field theory exists describing a very large class of
biophysically interesting Coulomb gas systems: the lowest order (mean-field)
version of this theory takes the form of a generalized Poisson-Boltzmann
theory. Interaction terms depend on details (finite-size effects, multipole
properties, etc). Convergence of the loop expansion holds only if mutual
interactions of mobile charges are small compared to their interaction with the
fixed-charge environment, which is frequently not the case. Problems with the
strongly- coupled effective theory can be circumvented with an alternative
local lattice formulation, with real positive action. In realistic situations,
with variable dielectric, a determinant of the Poisson operator must be
inserted to generate correct electrostatics. Methods adopted from unquenched
lattice QCD do this very efficiently.
@misc{Duncan2006Lattice,
abstract = {{An effective field theory exists describing a very large class of
biophysically interesting Coulomb gas systems: the lowest order (mean-field)
version of this theory takes the form of a generalized Poisson-Boltzmann
theory. Interaction terms depend on details (finite-size effects, multipole
properties, etc). Convergence of the loop expansion holds only if mutual
interactions of mobile charges are small compared to their interaction with the
fixed-charge environment, which is frequently not the case. Problems with the
strongly- coupled effective theory can be circumvented with an alternative
local lattice formulation, with real positive action. In realistic situations,
with variable dielectric, a determinant of the Poisson operator must be
inserted to generate correct electrostatics. Methods adopted from unquenched
lattice QCD do this very efficiently.}},
added-at = {2019-02-23T22:09:48.000+0100},
archiveprefix = {arXiv},
author = {Duncan, Anthony},
biburl = {https://www.bibsonomy.org/bibtex/27cc71c6f48208ffa1f9d4497e2289df1/cmcneile},
citeulike-article-id = {3821507},
citeulike-linkout-0 = {http://arxiv.org/abs/hep-lat/0609064},
citeulike-linkout-1 = {http://arxiv.org/pdf/hep-lat/0609064},
day = 28,
eprint = {hep-lat/0609064},
interhash = {314f0c11636f45d586c4ecb313db5a57},
intrahash = {7cc71c6f48208ffa1f9d4497e2289df1},
keywords = {medicine},
month = sep,
posted-at = {2012-10-28 07:57:02},
priority = {2},
timestamp = {2019-02-23T22:15:27.000+0100},
title = {{Lattice Field Theory Methods in Modern Biophysics}},
url = {http://arxiv.org/abs/hep-lat/0609064},
year = 2006
}