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A microscopic model of black hole evaporation in two dimensions
A bstract We present a microscopic model of black hole (BH) ‘evaporation’ in asymptotically AdS 2 spacetimes dual to the low energy sector of the SYK model. To describe evaporation, the SYK model is coupled to a bath comprising of N f free scalar fields Φ i . We consider a linear combination of coup...
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Published in: | The journal of high energy physics 2023-08, Vol.2023 (8), p.171-68, Article 171 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | A
bstract
We present a microscopic model of black hole (BH) ‘evaporation’ in asymptotically
AdS
2
spacetimes dual to the low energy sector of the SYK model. To describe evaporation, the SYK model is coupled to a bath comprising of
N
f
free scalar fields Φ
i
. We consider a linear combination of couplings of the form
O
SY K
(
t
)∑
i
Φ
i
(0,
t
), where
O
SY K
involves products of the Kourkoulou-Maldacena operator
iJ
/
N
∑
k
=
1
N
/
2
s
k
′
ψ
2
k
−
1
t
ψ
2
k
t
specified by a spin vector
s
′
. We discuss the time evolution of a product of (i) a pure state of the SYK system, namely a BH microstate characterized by a spin vector
s
and an effective BH temperature
T
BH
, and (ii) a Calabrese-Cardy state of the bath characterized by an effective temperature
T
bath
. We take
T
bath
≪
T
BH
, and
T
BH
much lower than the characteristic UV scale
J
of the SYK model, allowing a description in terms of the time reparameterization mode. Tracing over the bath degrees of freedom leads to a Feynman-Vernon type effective action for the SYK model, which we study in the low energy limit. The leading large
N
behaviour of the time reparameterization mode is found, as well as the
O
1
/
N
fluctuations. The latter are characterized by a non-Markovian non-linear stochastic differential equation with non-local Gaussian noise. In a restricted range of couplings, we find two classes of solutions which asymptotically approach (a) a BH at a lower temperature, and (b) a horizonless geometry. We identify these with partial and complete BH evaporation, respectively. Importantly, the asymptotic solution in both cases involves the scalar product of the spin vectors
s.s
′
, which carries some information about the initial state. By repeating the dynamical process
O
(
N
2
) times with different choices of the spin vector
s
′
, one can in principle reconstruct the initial BH microstate. |
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ISSN: | 1029-8479 1029-8479 |
DOI: | 10.1007/JHEP08(2023)171 |