Ensembles in M-theory and holography

A bstract We discuss that the string/M-theory partition function requires a choice of ensembles, depending on which background fields are held fixed. The background fields correspond to worldvolume couplings in the effective action approach to the superstring, which we extrapolate to the M2-brane. One natural ensemble in this context, which we call the M2-ensemble, corresponds to fixing the value of the M-theory three-form potential. In holographic setups the choice of ensemble is important when comparing to observables in the dual field theory. Indeed, in AdS 4 holography the M2-ensemble does not map gravitational observables directly to field theory observables at a fixed rank N , but rather to observables in the grand canonical ensemble. We remark that many M2-brane partition functions take a simple form in this ensemble hinting at one-loop exactness. We also discuss how in AdS 7 holography, the M2-ensemble does correspond to the canonical ensemble in the field theory, i.e. the (2,0) theory at fixed rank N .

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-11-14
DOI
https://doi.org/10.1007/jhep11(2025)078
Citations
6
Primary Topic
Black Holes and Theoretical Physics
Type
article
Field-Weighted Citation Impact
11.22

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article

Ensembles in M-theory and holography

Friðrik Freyr Gautason, Jesse van Muiden
6 citations
Journal of High Energy Physics
Black Holes and Theoretical Physics
11.22
article

Ensembles in M-theory and holography

Friðrik Freyr Gautason, Jesse van Muiden
article en
6 citations

Abstract

A bstract We discuss that the string/M-theory partition function requires a choice of ensembles, depending on which background fields are held fixed. The background fields correspond to worldvolume couplings in the effective action approach to the superstring, which we extrapolate to the M2-brane. One natural ensemble in this context, which we call the M2-ensemble, corresponds to fixing the value of the M-theory three-form potential. In holographic setups the choice of ensemble is important when comparing to observables in the dual field theory. Indeed, in AdS 4 holography the M2-ensemble does not map gravitational observables directly to field theory observables at a fixed rank N , but rather to observables in the grand canonical ensemble. We remark that many M2-brane partition functions take a simple form in this ensemble hinting at one-loop exactness. We also discuss how in AdS 7 holography, the M2-ensemble does correspond to the canonical ensemble in the field theory, i.e. the (2,0) theory at fixed rank N .

Journal of High Energy PhysicsVol. 2025(11)
University of Southampton (GB), Imperial College London (GB)
KU Leuven, Science and Technology Facilities Council
Openalex Percentile: Top 2%
Black Holes and Theoretical Physics
11.22
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Ensembles in M-theory and holography — Friðrik Freyr Gautason, Jesse van Muiden · Journal of High Energy Physics (2025) | TGRS Research Map | TGRS