The Casimir Polder force on a small polarizable particle (a ``point'' particle) situated in a wedge-shaped cavity with perfectly conducting walls is calculated, at zero temperature. Various special cases are examined. In particular, agreement with the conventional Casimir Polder formula is obtained
Casimir Effect for a Perfectly Conducting Wedge in Terms of Local Zeta Function
✍ Scribed by V.V. Nesterenko; G. Lambiase; G. Scarpetta
- Publisher
- Elsevier Science
- Year
- 2002
- Tongue
- English
- Weight
- 130 KB
- Volume
- 298
- Category
- Article
- ISSN
- 0003-4916
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✦ Synopsis
The vacuum energy density of electromagnetic field inside a perfectly conducting wedge is calculated by making use of the local zeta function technique. This regularization completely eliminates divergent expressions in the course of calculations and gives rise to a finite expression for the energy density in question without any subtractions. Employment of the Hertz potentials for constructing the general solution to the Maxwell equations results in a considerable simplification of the calculations. Transition to the global zeta function is carried out by introducing a cutoff nearby the cusp at the origin. Proceeding from this the heat kernel coefficients are calculated and the high temperature asymptotics of the Helmholtz free energy and of the torque of the Casimir forces are found. The wedge singularity gives rise to a specific high temperature behavior ∼T 2 of the quantities under consideration. The obtained results are directly applicable to the free energy of a scalar massless field and electromagnetic field on the background of a cosmic string.
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