Abstract

We consider a real, massive scalar field both on the $n$-dimensional anti--de Sitter (AdS$_n$) spacetime and on its universal cover CAdS$_n$. In the second scenario, we extend the recent analysis on PAdS$_n$, the Poincar\'e patch of AdS$_n$, first determining all admissible boundary conditions of Robin type that can be applied on the conformal boundary. Most notably, contrary to what happens on PAdS$_n$, no bound state mode solution occurs. Subsequently, we address the problem of constructing the two-point function for the ground state satisfying the admissible boundary conditions. All these states are locally of Hadamard form being obtained via a mode expansion which encompasses only the positive frequencies associated to the global timelike Killing field on CAdS$_n$. To conclude we investigate under which conditions any of the two-point correlation functions constructed on the universal cover defines a counterpart on AdS$_n$, still of Hadamard form. Since this spacetime is periodic in time, it turns out that this is possible only for Dirichlet boundary conditions, though for a countable set of masses of the underlying field, or for Neumann boundary conditions, though only for even dimensions and for one given value of the mass.

Highlights

  • Quantum field theory on curved backgrounds is a rapidly developing branch of theoretical physics especially within the algebraic approach [1,2]

  • To conclude we investigate under which conditions any of the two-point correlation functions constructed on the universal cover defines a counterpart on AdSn, still of Hadamard form

  • The following discussion complements that in [8] where the ground state for a massive real scalar field with arbitrary boundary conditions of Robin type has been constructed in the Poincarepatch of an n-dimensional anti–de Sitter spacetime

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Summary

INTRODUCTION

Quantum field theory on curved backgrounds is a rapidly developing branch of theoretical physics especially within the algebraic approach [1,2]. In order to disentangle the above two problems, our first step consists of considering CAdSn, the universal cover of anti–de Sitter spacetime, which is a manifold still possessing a conformal boundary, but no closed timelike curve In this setting it is known that the Klein-Gordon equation leads to a well-defined initial value problem, though most of the literature assumes only Dirichlet boundary conditions. As a matter of fact, since the Poincarepatch possesses a global timelike Killing field, in [8], it has been studied the existence for each boundary condition of Robin type of ground states associated with the Klein-Gordon equation. While they do not exist whenever bound state mode solutions occur, in all other cases they can be constructed explicitly in terms of their associated two-point correlation function In addition they enjoy several notable physical properties, such as the Hadamard condition. In the Appendix we discuss some more technical aspects concerning the construction of the two-point functions and we show, in particular, that no bound state mode solution occurs

SCALAR FIELD IN ADS SPACETIME
Klein-Gordon equation
BOUNDARY CONDITIONS
Two-point function in CAdSn
Two-point function in AdSn
CONCLUSIONS
ΓðaÞ or
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