Abstract
Gravitational collapse into a black hole has been extensively studied with classical sources. We develop a new formalism to simulate quantum fields forming a black hole. By choosing a convenient coherent state, this formalism taps into well-established techniques used for classical collapse and adds on the evolution of the mode functions of the quantum field operator. Divergences are regularized with the cosmological constant and Pauli-Villars fields. Using a massless spherically symmetric scalar field as an example, we demonstrate the effectiveness of the formalism by reproducing some classical results in gravitational collapse, and identifying the difference due to the quantum effects. We also find that Choptuik scaling in critical collapse survives in the semiclassical simulation, and furthermore the quantum deviation from the classical Choptuik scaling decreases when the system approaches the critical point.
Highlights
Theoretically, black holes along with their quantum properties have caused great puzzles and great advances in our understanding of gravity and quantum field theory
We develop a new formalism to simulate quantum fields forming a black hole
Using a massless spherically symmetric scalar field as an example, we demonstrate the effectiveness of the formalism by reproducing some classical results in gravitational collapse, and identifying the difference due to the quantum effects
Summary
The theory for the simulation of the collapse of a spherically symmetric classical massless scalar field is discussed using the methods of [48] but with a different gauge choice. The geometrical side of the Einstein equation will be presented using variables that make the evolution equations better suited for lattice simulations, and we show how to include the matter fields. Before connecting the geometry to the matter equations, the gauge choices are reviewed briefly. Note that in the simulation all the fundamental constants are set to one, = c = MP = 1.
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