Casimir calculations in Meep

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==Introduction== ==Introduction==
-In this section, we introduce the equations and basic considerations+To do
-involved in computing the force using the method presented in+
-[refs]. Note that we keep the details of the derivation to a minimum+
-and instead focus on the calculational aspects of the resulting+
-algorithm.+
- +
-The basic steps involved in computing the Casimir force, as outlined+
-in [ref], are:+
- +
-1. Map the problem onto a new problem with dissipation. Here, as in+
-[ref], we choose a frequency-independent conductivity "sigma".+
- +
-2. Measure the electric '''E''' and magnetic '''H''' fields in response to+
-current pulses placed separately at each point along a surface+
-enclosing the body of interest.+
- +
-3. Integrate these fields in spave over the enclosing surface and then+
-integrate this result, multiplied by a known function <math>g(-t)</math>, over+
-time t.+
- +
-[The manner in which (1) and (2) are performed plays a large role on+
-the efficiency of the method. For example, computing the fields due to+
-ach source separately at each point on the surface, as described in+
-(2), would require a separate Meep calculation for each source (and+
-polarization). As described in [ref], and further below, it is+
-possible to modify the calculation of these steps so as to optimize+
-the calculation of the stress tensor over the spatial surface. For the+
-purpose of this introduction, however, we do not require specific+
-details on how we handle the spatial integration.]+
==Parallel plates== ==Parallel plates==

Revision as of 18:49, 3 April 2009

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Casimir calculations in Meep

It is possible to use the Meep time-domain simulation code in order to calculate Casimir forces (and related quantities), a quantum-mechanical force that can arise even between neutral bodies due to quantum vacuum fluctuations in the electromagnetic field, or equivalently as a result of geometry dependence in the quantum vacuum energy.

Calculating Casimir forces in a classical time-domain Maxwell simulation like Meep is possible because of a new algorithm described in:

  • Alejandro W. Rodriguez, Alexander P. McCauley, John D. Joannopoulos, and Steven G. Johnson, "Casimir forces in the time domain: I. Theory," arXiv preprint archive article arXiv:0904.0267 (April 2009).
  • Alexander P. McCauley, Alejandro W. Rodriguez, John D. Joannopoulos, and Steven G. Johnson, "Casimir forces in the time domain: II. Applications," manuscript in preparation (2009).

This page will provide some tutorial examples showing how these calculations are performed for simple geometries.

Introduction

To do

Parallel plates

To do.

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