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Electromagnetic response of a dipole-coupled ellipsoidal bilayer

Ambjörnsson, T. LU ; Apell, S. P. and Mukhopadhyay, G. (2004) In Physical Review E 69(3).
Abstract
We derive an expression for the polarizability of an ellipsoidally shaped cell-like structure at field frequencies where membrane molecular resonances (vibrational and electronic) are important. We first present analytical results for the dielectric function of a flat, dipole coupled, bilayer consisting of molecules with one prominent resonance frequency. Due to the nature of the dipole coupling the dielectric function is different for the field being parallel or perpendicular to the bilayer normal with two new resonance frequencies ω=˜ω0∥ and ω=˜ω0⊥. We then combine this anisotropic bilayer dielectric function with the analytical solution of Gauss equation for an ellipsoid with an anisotropic coating (the coating dielectric function being... (More)
We derive an expression for the polarizability of an ellipsoidally shaped cell-like structure at field frequencies where membrane molecular resonances (vibrational and electronic) are important. We first present analytical results for the dielectric function of a flat, dipole coupled, bilayer consisting of molecules with one prominent resonance frequency. Due to the nature of the dipole coupling the dielectric function is different for the field being parallel or perpendicular to the bilayer normal with two new resonance frequencies ω=˜ω0∥ and ω=˜ω0⊥. We then combine this anisotropic bilayer dielectric function with the analytical solution of Gauss equation for an ellipsoid with an anisotropic coating (the coating dielectric function being different parallel and perpendicular to the coating normal) in order to find the polarizability of an ellipsoidal bilayer membrane. In particular, we find that for a thin-walled (compared to the size of the cell) membrane the resonance frequencies of the polarizability are the same as for a flat bilayer (independent of the cell shape). However, our analytic result for the geometric weights for the oscillator strengths is sensitive to the shape; the geometric weight for the ω=˜ω0⊥
(ω=˜ω0∥) peak is largest when the external field is along the largest (smallest) axis. The geometric weights are shown to be constrained by three sum rules. (Less)
Please use this url to cite or link to this publication:
author
publishing date
type
Contribution to journal
publication status
published
subject
in
Physical Review E
volume
69
issue
3
publisher
American Physical Society
ISSN
1539-3755
DOI
10.1103/PhysRevE.69.031914
language
English
LU publication?
no
id
75b55228-3573-493e-8a72-dacecd202690
alternative location
https://link.aps.org/doi/10.1103/PhysRevE.69.031914
date added to LUP
2019-05-03 11:47:15
date last changed
2019-08-06 16:42:40
@article{75b55228-3573-493e-8a72-dacecd202690,
  abstract     = {We derive an expression for the polarizability of an ellipsoidally shaped cell-like structure at field frequencies where membrane molecular resonances (vibrational and electronic) are important. We first present analytical results for the dielectric function of a flat, dipole coupled, bilayer consisting of molecules with one prominent resonance frequency. Due to the nature of the dipole coupling the dielectric function is different for the field being parallel or perpendicular to the bilayer normal with two new resonance frequencies ω=˜ω0∥ and ω=˜ω0⊥. We then combine this anisotropic bilayer dielectric function with the analytical solution of Gauss equation for an ellipsoid with an anisotropic coating (the coating dielectric function being different parallel and perpendicular to the coating normal) in order to find the polarizability of an ellipsoidal bilayer membrane. In particular, we find that for a thin-walled (compared to the size of the cell) membrane the resonance frequencies of the polarizability are the same as for a flat bilayer (independent of the cell shape). However, our analytic result for the geometric weights for the oscillator strengths is sensitive to the shape; the geometric weight for the ω=˜ω0⊥ <br/>(ω=˜ω0∥) peak is largest when the external field is along the largest (smallest) axis. The geometric weights are shown to be constrained by three sum rules.},
  articleno    = {031914},
  author       = {Ambjörnsson, T. and Apell, S. P. and Mukhopadhyay, G.},
  issn         = {1539-3755},
  language     = {eng},
  number       = {3},
  publisher    = {American Physical Society},
  series       = {Physical Review E},
  title        = {Electromagnetic response of a dipole-coupled ellipsoidal bilayer},
  url          = {http://dx.doi.org/10.1103/PhysRevE.69.031914},
  volume       = {69},
  year         = {2004},
}