Abstract

The information loss paradox is usually stated as an incompatibility between general relativity and quantum mechanics. However, the assumptions leading to the problem are often overlooked and, in fact, a careful inspection of the main hypothesises suggests a radical reformulation of the problem. Indeed, we present a thought experiment involving a black hole that emits radiation and, independently of the nature of the radiation, we show the existence of an incompatibility between (i) the validity of the laws of general relativity to describe infalling matter far from the Planckian regime, and (ii) the so-called central dogma which states that as seen from an outside observer a black hole behaves like a quantum system whose number of degrees of freedom is proportional to the horizon area. We critically revise the standard arguments in support of the central dogma, and argue that they cannot hold true unless some new physics is invoked even before reaching Planck scales. This suggests that the information loss problem, in its current formulation, is not necessarily related to any loss of information or lack of unitarity. Therefore, in principle, semiclassical general relativity and quantum mechanics can be perfectly compatible before reaching the final stage of the black hole evaporation where, instead, a consistent theory of quantum gravity is needed to make any prediction.

Highlights

  • Respect, there is not really a paradox but it could be just our ignorance about Planck-scale physics that prevents us from concluding anything definite about what happens to the information during black hole evaporation [6]

  • We present a thought experiment involving a black hole that emits radiation and, independently of the nature of the radiation, we show the existence of an incompatibility between (i) the validity of the laws of general relativity to describe infalling matter far from the Planckian regime, and (ii) the so-called central dogma which states that as seen from an outside observer a black hole behaves like a quantum system whose number of degrees of freedom is proportional to the horizon area

  • The contradiction we found in our thought experiment is between B2b and B3, that is, between the laws of general relativity governing the physics of infalling matter and the central dogma; while B2a and B3 can in principle be perfectly compatible

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Summary

Is there an information loss paradox?

It is often stated that the thermal nature of black holes eventually leads to an incompatibility between semiclassical general relativity and one of the pillar of quantum mechanics, i.e. the unitarity of the S-matrix, leading to the well-known information loss paradox [4]. We strongly believe that the assumptions on which the paradoxical implications rely are often overlooked, and deserve a deeper and thorough inspection. It is crucial to reformulate the problem by highlighting and critically revising all the basic assumptions that are usually made. In what follows we carefully analyze three different scenarios that are normally considered

Case A: unitarity problem
Case B: entropy problem
Case C: no paradox
Standard arguments for the central dogma
Physical configuration
Contradiction between B2 and B3
Stronger contradiction
Limitations of the standard arguments
Comments on black hole complementarity and firewall
Discussion
Full Text
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