Abstract

Weyl–Heisenberg ensembles are translation-invariant determinantal point processes on mathbb {R}^{2d} associated with the Schrödinger representation of the Heisenberg group, and include as examples the Ginibre ensemble and the polyanalytic ensembles, which model the higher Landau levels in physics. We introduce finite versions of the Weyl–Heisenberg ensembles and show that they behave analogously to the finite Ginibre ensembles. More specifically, guided by the observation that the Ginibre ensemble with N points is asymptotically close to the restriction of the infinite Ginibre ensemble to the disk of area N, we define finite WH ensembles as adequate finite approximations of the restriction of infinite WH ensembles to a given domain Omega . We provide a precise rate for the convergence of the corresponding one-point intensities to the indicator function of Omega , as Omega is dilated and the process is rescaled proportionally (thermodynamic regime). The construction and analysis rely neither on explicit formulas nor on the asymptotics for orthogonal polynomials, but rather on phase-space methods. Second, we apply our construction to study the pure finite Ginibre-type polyanalytic ensembles, which model finite particle systems in a single Landau level, and are defined in terms of complex Hermite polynomials. On a technical level, we show that finite WH ensembles provide an approximate model for finite polyanalytic Ginibre ensembles, and we quantify the corresponding deviation. By means of this asymptotic description, we derive estimates for the rate of convergence of the one-point intensity of polyanalytic Ginibre ensembles in the thermodynamic limit.

Highlights

  • We present a canonical construction of finite Weyl–Heisenberg ensembles and show that they enjoy properties similar to the finite Ginibre ensemble

  • We develop a new approach based on spectral methods and harmonic analysis in phase space and show that the finite WH ensembles associated with a Hermite function are asymptotically close to finite polyanalytic ensembles

  • As a first step towards a description of finite pure polyanalytic ensembles, we introduce a general construction of finite versions of Weyl–Heisenberg ensembles that may be of independent interest

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Summary

Weyl–Heisenberg Ensembles

We study the class of determinantal point processes on R2d whose correlation kernel is given as. Modulo conjugation with a phase factor, this is essentially the kernel of the infinite Ginibre ensemble Another important class of examples arises by choosing g to be a Hermite function. The abstract construction is instrumental to study the asymptotic properties of a important class of finite-dimensional determinantal point processes, namely the finite pure polyanalytic Ginibre ensembles, which model the electron density in higher Landau levels. This is an example where the Plancherel–Rotach asymptotics of the basis functions are not available. Our analysis of the finite polyanalytic ensembles has two steps: (i) the abstract construction of finite WH ensembles and their thermodynamic limits; (ii) the comparison of the finite WH ensembles associated with Hermite functions and the finite pure polyanalytic ensembles

Planar Hermite Ensembles
Finite Weyl–Heisenberg Ensembles
Scaled Limits and Rates of Convergence
Approximation of Finite Polyanalytic Ensembles by WH Ensembles
Simultaneous Observability
Organization
The Short-Time Fourier Transform
Special Windows
The Range of the Short-Time Fourier Transform
Metaplectic Rotation
Time-Frequency Localization and Toeplitz Operators
The Weyl Correspondence
Definitions
Universality and Rates of Convergence
Eigenfunctions of Toeplitz Operators
Eigenvalues of Toeplitz Operators
Identification as a WH Ensemble
Comparison Between Finite WH and Polyanalytic Ensembles
Change of Quantization
Comparison of Correlation Kernels
Transference to Finite Pure Polyanalytic Ensembles
The One-Point Intensity of Finite Polyanalytic Ensembles
Restriction Versus Localization
An Extension of Kostlan’s Theorem
Functions of Bounded Variation
Trace-Class Operators
Properties of Modulation Spaces
Polyanalytic Bargmann-Fock Spaces
Pure Polyanalytic-Fock Spaces
Full Text
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