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Subadditive average distances and quantum promptness
A central property of a classical geometry is that the geodesic distance between two events is additive . When considering quantum fluctuations in the metric or a quantum or statistical superposition of different spacetimes, additivity is generically lost at the level of expectation values. In the p...
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Published in: | Classical and quantum gravity 2023-08, Vol.40 (16), p.165013 |
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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 central property of a classical geometry is that the geodesic distance between two events is
additive
. When considering quantum fluctuations in the metric or a quantum or statistical superposition of different spacetimes, additivity is generically lost at the level of expectation values. In the presence of a superposition of metrics, distances can be made diffeomorphism invariant by considering the frame of a family of free-falling observers or a pressureless fluid, provided we work at sufficiently low energies. We propose to use the average squared distance between two events
⟨
d
2
(
x
,
y
)
⟩
as a proxy for understanding the effective quantum (or statistical) geometry and the emergent causal relations among such observers. At each point, the average squared distance
⟨
d
2
(
x
,
y
)
⟩
defines an average metric tensor. However, due to non-additivity,
⟨
d
2
(
x
,
y
)
⟩
is not the (squared) geodesic distance associated with it. We show that departures from additivity can be conveniently captured by a bi-local quantity
C
(
x
,
y
)
. Violations of additivity build up with the mutual separation between
x
and
y
and can correspond to
C
0 (superadditive). We show that average Euclidean distances are always subadditive: they satisfy the triangle inequality but generally fail to saturate it. In Lorentzian signature there is no definite result about the sign of
C
, most physical examples give
C
|
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ISSN: | 0264-9381 1361-6382 |
DOI: | 10.1088/1361-6382/ace583 |