Instability of flat space at finite temperature

David J. Gross, Malcolm J. Perry, and Laurence G. Yaffe
Phys. Rev. D 25, 330 – Published 15 January 1982
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Abstract

The instabilities of quantum gravity are investigated using the path-integral formulation of Einstein's theory. A brief review is given of the classical gravitational instabilities, as well as the stability of flat space. The Euclidean path-integral representation of the partition function is employed to discuss the instability of flat space at finite temperature. Semiclassical, or saddle-point, approximations are utilized. We show how the Jeans instability arises as a tachyon in the graviton propagator when small perturbations about hot flat space are considered. The effect due to the Schwarzschild instanton is studied. The small fluctuations about this instanton are analyzed and a negative mode is discovered. This produces, in the semiclassical approximation, an imaginary part of the free energy. This is interpreted as being due to the metastability of hot flat space to nucleate black holes. These then evolve by evaporation or by accretion of thermal gravitons, leading to the instability of hot flat space. The nucleation rate of black holes is calculated as a function of temperature.

  • Received 29 June 1981

DOI:https://doi.org/10.1103/PhysRevD.25.330

©1982 American Physical Society

Authors & Affiliations

David J. Gross and Malcolm J. Perry

  • Department of Physics, Princeton University, Princeton, New Jersey 08544

Laurence G. Yaffe

  • Department of Physics, California Institute of Technology, Pasadena, California 91109

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Vol. 25, Iss. 2 — 15 January 1982

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