The boundary-induced correction to the accelerated-detector response in punctured Minkowski spacetime is computed exactly, proven absolutely integrable with an O(1) long-time limit for finite Robin parameter beta, and shown to diverge logarithmically in the formal Neumann limit.
Boundary conditions and infrared divergences
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abstract
We review the procedure to construct quasi-free ground states, for real scalar fields whose dynamics is dictated by the Klein-Gordon equation, on standard static Lorentzian manifolds with a time-like boundary. We observe that, depending on the assigned boundary condition of Robin type, this procedure does not always lead to the existence of a suitable bi-distribution $w_2\in \mathcal{D}'(M\times M)$ due to the presence of infrared divergences. As a concrete example we consider a Bertotti-Robinson spacetime in two different coordinate patches. In one case we show that infrared divergences do not occur only for Dirichlet boundary conditions as one might expect a priori, while, in the other case, we prove that they occur only when Neumann boundary conditions are imposed at the time-like boundary.
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Corrections to the Unruh Effect from Robin Boundary Conditions in Punctured Minkowski Spacetime
The boundary-induced correction to the accelerated-detector response in punctured Minkowski spacetime is computed exactly, proven absolutely integrable with an O(1) long-time limit for finite Robin parameter beta, and shown to diverge logarithmically in the formal Neumann limit.