Single-trace realization conjecture for one-dimensional Dirac ensembles

Let DD be the Dirac operator in a formal Dirac ensemble of type (1,0)(1,0) or (0,1)(0,1), with coupling constants tjt_j and partition function

Z=Get24TrD2jdtj2jTrDjdD.Z = \int_{\mathcal{G}}e^{-\frac{{t_{2}}}{4}\operatorname{Tr} D^{2} - \sum_{j\geq}^{d} \frac{t_{j}}{2 j}\operatorname{Tr} D^{j}}dD.

Here G\mathcal{G} is the relevant Dirac-ensemble integration space, and HN\mathcal{H}_N denotes the space of N×NN\times N Hermitian matrices. Single-trace realization conjecture. The coupling constants tjt_j can be tuned so that the integral becomes

HNeN2TrH2jdcjjNTrHjdH,\int_{\mathcal{H}_{N}}e^{-\frac{N}{2}\operatorname{Tr} H^{2} - \sum_{j\geq}^{d} \frac{c_{j}}{ j}N\operatorname{Tr} H^{j}}dH,

where the new coupling constants cjc_j, expressed in terms of the tjt_j, can take any real values. This conjecture asserts that the coupling-constant space of these one-dimensional Dirac ensembles contains the corresponding single-trace matrix models, despite the shared coupling constants of the single- and multi-trace terms.

Sources & referencesView supporting material

Primary source

Hamed Hessam, Masoud Khalkhali and Nathan Pagliaroli, “Double scaling limits of Dirac ensembles and Liouville quantum gravity”, arXiv:2204.14206 (2023).

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