2018
DOI: 10.1088/1361-6382/aaa623
|View full text |Cite
|
Sign up to set email alerts
|

Code subspaces for LLM geometries

Abstract: We consider effective field theory around classical background geometries with a gauge theory dual, in the class of LLM geometries. These are dual to half-BPS states of N = 4 SYM. We find that the language of code subspaces is natural for discussing the set of nearby states, which are built by acting with effective fields on these backgrounds. This work extends our previous work by going beyond the strict infinite N limit. We further discuss how one can extract the topology of the state beyond N → ∞ and find t… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
19
0

Year Published

2018
2018
2024
2024

Publication Types

Select...
6

Relationship

1
5

Authors

Journals

citations
Cited by 17 publications
(19 citation statements)
references
References 39 publications
0
19
0
Order By: Relevance
“…Despite the expected lack of classical bridges in the BPS limit, the description of the naked singularity and its phase space interpretation in section 4.2, will allow us to identify the regions in spacetime where such quantum connectivity exists. These are precisely the gray areas in phase space describing the naked singularity in the semiclassical limit 20 .…”
Section: Two Boundary Epr=er In Llmmentioning
confidence: 90%
See 3 more Smart Citations
“…Despite the expected lack of classical bridges in the BPS limit, the description of the naked singularity and its phase space interpretation in section 4.2, will allow us to identify the regions in spacetime where such quantum connectivity exists. These are precisely the gray areas in phase space describing the naked singularity in the semiclassical limit 20 .…”
Section: Two Boundary Epr=er In Llmmentioning
confidence: 90%
“…In fact, since LLM geometries are determined by the expectation value of the single particle phase space density, typical pure states describing at least N c giant gravitons |Ψ typical can not be distinguished from their ensemble averages when probed by low energy observables in classical gravity [82,[95][96][97]. Hence, the product state |Ψ typical ⊗ |Ψ typical is also effectively captured by figure 15 in 20 When restricting the probe operators O L and O R to be half-BPS SO(4) symmetric, there exist conservation laws that can make correlations (5.3) vanish. From now on, it is assumed that given some density ρ, the choice of probes O L and O R is such that (5.3) does not vanish.…”
Section: Product Statesmentioning
confidence: 99%
See 2 more Smart Citations
“…This subspace, which behaves like the Fock space for the t k operators, can be regarded as a code subspace for the algebra around the vacuum state. In [29], this code subspace was discussed around special excited states corresponding to rectangular Young tableaus. In matrix model language, this is a closed string representation of the Hilbert space.…”
Section: )mentioning
confidence: 99%