Thermodynamics of the BMN matrix model at strong coupling
arXiv:1411.5541 · doi:10.1007/JHEP03(2015)069
Abstract
We construct the black hole geometry dual to the deconfined phase of the BMN matrix model at strong 't Hooft coupling. We approach this solution from the limit of large temperature where it is approximately that of the non-extremal D0-brane geometry with a spherical horizon. This geometry preserves the symmetry of the matrix model trivial vacuum. As the temperature decreases the horizon becomes deformed and breaks the to the symmetry of the matrix model. When the black hole free energy crosses zero the system undergoes a phase transition to the confined phase described by a Lin-Maldacena geometry. We determine this critical temperature, whose computation is also within reach of Monte Carlo simulations of the matrix model.
28+7 pages, 9 figures
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Cited by in corpus (10)
- Bootstrap bounds on D0-brane quantum mechanics
- Exploring new variational quantum circuit ansatzes for solving matrix models
- Finite-temperature phase diagram of the BMN matrix model on the lattice
- Witten index of BMN matrix quantum mechanics
- Moduli dynamics as a predictive tool for thermal maximally supersymmetric Yang-Mills at large N
- A Charge Constraint in BMN
- Simulations of Bosonic BMN Matrix Model
- The Low Energy Limit of BFSS Quantum Mechanics
- Emergent Geometries from the BMN Matrix Model
- Non-perturbative phase structure of the bosonic BMN matrix model