We study the relative zeta function for the couple of operators A0 and Aα, where A0 is the free unconstrained Laplacian in L2(Rd) (d ≥ 2) and Aα is the singular perturbation of A0 associated to the presence of a delta interaction supported by a hyperplane. In our setting the operatorial parameter α, which is related to the strength of the perturbation, is of the kind α = α (-Δ||), where -Δ|| is the free Laplacian in L2(Rd-1). Thus α may depend on the components of the wave vector parallel to the hyperplane; in this sense Aα describes a semitransparent hyperplane selecting transverse modes. As an application we give an expression for the associated thermal Casimir energy. Whenever α = χI(-Δ||), where χI is the characteristic function of an interval I, the thermal Casimir energy can be explicitly computed.

Relative-Zeta and Casimir Energy for a Semitransparent Hyperplane Selecting Transverse Modes

Fermi, Davide;Posilicano, Andrea
2017-01-01

Abstract

We study the relative zeta function for the couple of operators A0 and Aα, where A0 is the free unconstrained Laplacian in L2(Rd) (d ≥ 2) and Aα is the singular perturbation of A0 associated to the presence of a delta interaction supported by a hyperplane. In our setting the operatorial parameter α, which is related to the strength of the perturbation, is of the kind α = α (-Δ||), where -Δ|| is the free Laplacian in L2(Rd-1). Thus α may depend on the components of the wave vector parallel to the hyperplane; in this sense Aα describes a semitransparent hyperplane selecting transverse modes. As an application we give an expression for the associated thermal Casimir energy. Whenever α = χI(-Δ||), where χI is the characteristic function of an interval I, the thermal Casimir energy can be explicitly computed.
2017
Springer INdAM Series
9783319589039
9783319589046
Casimir effect
Delta-interactions
Finite temperature quantum fields
Relative zeta function
Zeta regularization
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11311/1281866
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