We extend the Gross-Perry-Yaffe approach of hot flat space instability to Minkowski space. This is done by examining the massless gravitational perturbation in a saddle point approximation of the partition function. In particular, we show that a nonconformal instability appears in the transverse-traceless tensor sector (massless gravitons) if a Schwarzschild wormhole background is considered. The appearance of an instability in the whole manifold is here interpreted as a black hole pair creation. The instability of .at space via black hole pair creation is further explored evaluating the Casimir energy to one loop in a Hamiltonian approach. A variational approach associated to a Sturm-Liouville problem is used to evaluate the Casimir energy by means of trial wave functionals of Gaussian form. The Casimir energy is here interpreted as an induced cosmological constant associated to the Sturm-Liouville eigenvalue. To handle with divergences which appear to one loop approximation, we use a zeta function regularization. A renormalization and a renormalization group equation are involved to handle with ultra-violet divergences.

The cosmological constant and the stability of Flat Space

GARATTINI, Remo
2006-01-01

Abstract

We extend the Gross-Perry-Yaffe approach of hot flat space instability to Minkowski space. This is done by examining the massless gravitational perturbation in a saddle point approximation of the partition function. In particular, we show that a nonconformal instability appears in the transverse-traceless tensor sector (massless gravitons) if a Schwarzschild wormhole background is considered. The appearance of an instability in the whole manifold is here interpreted as a black hole pair creation. The instability of .at space via black hole pair creation is further explored evaluating the Casimir energy to one loop in a Hamiltonian approach. A variational approach associated to a Sturm-Liouville problem is used to evaluate the Casimir energy by means of trial wave functionals of Gaussian form. The Casimir energy is here interpreted as an induced cosmological constant associated to the Sturm-Liouville eigenvalue. To handle with divergences which appear to one loop approximation, we use a zeta function regularization. A renormalization and a renormalization group equation are involved to handle with ultra-violet divergences.
book chapter - capitolo di libro
Inglese
2006
MOORE, D. C.
1-59454-660-6
215
259
zeta function regularization;pair creation;Sturm-Liouville;cosmological constant;Casimir energy
It was J. A. Wheeler who first conjectured that spacetime could be subjected to topology fluctuation at the Planck scale [J.A. Wheeler, Ann. Phys. 2 (1957) 604]. This means that spacetime undergoes a deep and rapid transformation in its structure. This changing spacetime is best known as "spacetime foam", which can be taken as a model for the quantum gravitational vacuum. A related quantum process in this context is black hole pair creation. Indeed, an intriguing property of quantum physics is the particle creation generated by external fields, like a constant electric or magnetic field, or by quantum fluctuation of the vacuum. In this last case only virtual particles are involved. However when the energy scale is large enough virtual particles can be transformed into real. In line of principle the same mechanism can be shared by the gravitational field where virtual black holes [R.B. Mann and Simon F. Ross Phys.Rev.D 53, 2254, 1995; S.W. Hawking, Phys. Rev. D 53, 3099-3107, 1996] can be created and annihilated in analogy with particle physics. This particular phenomenon has been investigated in different contexts and in particular when a cosmological constant is introduced [R. Bousso and S.W. Hawking, Phys. Rev. D 52, 5659 (1995); R. Bousso and S.W. Hawking, Phys. Rev. D 54, 5659 (1995)]. In this work we probe the stability problem in presence of a cosmological constant by means of variational methods [P. Ginsparg and M.J. Perry, Nucl. Phys. B 222 (1983) 245; R.E. Young, Phys. Rev. D 28, (1983) 2436; R.E. Young, Phys. Rev. D 28 (1983) 2420; M.S. Volkov and A. Wipf, Nucl. Phys. B 582 (2000), 313; hep-th/0003081]. The interesting final aspect is a stable bubble foam picture.
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1.2 Contributi in volume - Book chapters::1.2.01 Contributi in volume (Capitoli o Saggi) - Book Chapters/Essays
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Garattini, Remo
1
268
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/10446/19948
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