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Generalized quantum Zernike Hamiltonians: Polynomial Higgs-type algebras and algebraic derivation of the spectrum

Rutwig Campoamor-Stursberg, Francisco J. Herranz, Danilo Latini, Ian Marquette, Alfonso Blasco

TL;DR

This work introduces a generalized quantum Zernike framework with Hamiltonians $\hat{\mathcal{H}}_N = \hat{p}_1^2+\hat{p}_2^2+\sum_{k=1}^N \gamma_k (\hat{q}_1 \hat{p}_1+\hat{q}_2 \hat{p}_2)^k$, showing that quantum superintegrability persists for all $N$. The authors construct quantum symmetry algebras—polynomial Higgs-type algebras—that are mapped, via a basis change, to deformed oscillator algebras with a factorized structure function $\Phi=\Phi_1\Phi_2$, enabling an algebraic derivation of spectra. They solve explicitly the quadratic ($N=2$), cubic ($N=3$), and quartic ($N=4$) cases, and prove conjectures for $N=5$, providing two spectral branches and interpretations as superintegrable perturbations of the Zernike system and of curved isotropic oscillators on $\mathbf S^2$, $\mathbf H^2$, and $\mathbf E^2$. The framework paves the way for general $N$ by presenting a precise conjectural structure for the symmetry algebra and spectrum, with potential applications to momentum-dependent perturbations in curved spaces and beyond.

Abstract

We consider the quantum analog of the generalized Zernike systems given by the Hamiltonian: $$ \hat{\mathcal{H}} _N =\hat{p}_1^2+\hat{p}_2^2+\sum_{k=1}^N γ_k (\hat{q}_1 \hat{p}_1+\hat{q}_2 \hat{p}_2)^k , $$ with canonical operators $\hat{q}_i,\, \hat{p}_i$ and arbitrary coefficients $γ_k$. This two-dimensional quantum model, besides the conservation of the angular momentum, exhibits higher-order integrals of motion within the enveloping algebra of the Heisenberg algebra $\mathfrak h_2$. By constructing suitable combinations of these integrals, we uncover a polynomial Higgs-type symmetry algebra that, through an appropriate change of basis, gives rise to a deformed oscillator algebra. The associated structure function $Φ$ is shown to factorize into two commuting components $Φ=Φ_1 Φ_2$. This framework enables an algebraic determination of the possible energy spectra of the model for the cases $N=2,3,4$, the case $N=1$ being canonically equivalent to the harmonic oscillator. Based on these findings, we propose two conjectures which generalize the results for all $N\ge 2$ and any value of the coefficients $γ_k$, that they are explicitly proven for $N=5$. In addition, all of these results can be interpreted as superintegrable perturbations of the original quantum Zernike system corresponding to $N=2$ which are also analyzed and applied to the isotropic oscillator on the sphere, hyperbolic and Euclidean spaces.

Generalized quantum Zernike Hamiltonians: Polynomial Higgs-type algebras and algebraic derivation of the spectrum

TL;DR

This work introduces a generalized quantum Zernike framework with Hamiltonians , showing that quantum superintegrability persists for all . The authors construct quantum symmetry algebras—polynomial Higgs-type algebras—that are mapped, via a basis change, to deformed oscillator algebras with a factorized structure function , enabling an algebraic derivation of spectra. They solve explicitly the quadratic (), cubic (), and quartic () cases, and prove conjectures for , providing two spectral branches and interpretations as superintegrable perturbations of the Zernike system and of curved isotropic oscillators on , , and . The framework paves the way for general by presenting a precise conjectural structure for the symmetry algebra and spectrum, with potential applications to momentum-dependent perturbations in curved spaces and beyond.

Abstract

We consider the quantum analog of the generalized Zernike systems given by the Hamiltonian: with canonical operators and arbitrary coefficients . This two-dimensional quantum model, besides the conservation of the angular momentum, exhibits higher-order integrals of motion within the enveloping algebra of the Heisenberg algebra . By constructing suitable combinations of these integrals, we uncover a polynomial Higgs-type symmetry algebra that, through an appropriate change of basis, gives rise to a deformed oscillator algebra. The associated structure function is shown to factorize into two commuting components . This framework enables an algebraic determination of the possible energy spectra of the model for the cases , the case being canonically equivalent to the harmonic oscillator. Based on these findings, we propose two conjectures which generalize the results for all and any value of the coefficients , that they are explicitly proven for . In addition, all of these results can be interpreted as superintegrable perturbations of the original quantum Zernike system corresponding to which are also analyzed and applied to the isotropic oscillator on the sphere, hyperbolic and Euclidean spaces.

Paper Structure

This paper contains 12 sections, 3 theorems, 87 equations, 5 figures, 1 table.

Key Result

Proposition 1

The set of equations (b12) yields four types of solutions for the representation-dependent constant $u$ and the spectrum of the Hamiltonian $\hat{\mathcal{H}} _2$ in (b4) depending on the parameter ${n}\in\{1,2,\dots\}$, that is, $u=u( {n})$ and $E=E( {n})$. Introducing these expressions into (c9),

Figures (5)

  • Figure 1: The discrete spectrum (\ref{['es2']}) of the spherical oscillator on $\mathbf S^2$ for the first ten states $1\le n\le 10$ according to three values of the curvature $\kappa\in\{0.5,\, 0.25,\, 0.15\}$ starting from the upper dots together with the Euclidean spectrum (\ref{['ee2']}) with $\kappa=0$ in the lowest values.
  • Figure 2: The finite discrete spectrum (\ref{['eh2']}) of the hyperbolic oscillator on $\mathbf H^2$ for the three values of the curvature $\kappa\in\{-0.25,\, -0.16,\, -0.12\}$ corresponding to $n_{\rm max}\in\{4,\, 6,\, 8\}$ (\ref{['constraints']}) starting from the lower dots, respectively, together with the Euclidean spectrum (\ref{['ee2']}) with $\kappa=0$ in the highest values.
  • Figure 3: The discrete spectrum (\ref{['s4a']}) of the cubic spherical perturbation of the oscillator on $\mathbf E^2$ for the first ten states $1\le n\le 10$ according to three values of the parameter $\mu\in\{-0.05,\, -0.025,\, -0.01\}$ starting from the upper dots together with the Euclidean spectrum (\ref{['ee2']}) with $\mu=0$ in the lowest values.
  • Figure 4: The finite discrete spectrum (\ref{['s4b']}) of the cubic hyperbolic perturbation of the oscillator on $\mathbf E^2$ for three values $\mu\in\{0.06,\, 0.03,\, 0.015\}$ corresponding to $n_{\rm max}\in\{3,\, 5,\, 7\}$ (\ref{['s4c']}) starting from the lower dots, respectively, together with the Euclidean spectrum (\ref{['ee2']}) with $\mu=0$ in the highest values.
  • Figure 5: The finite discrete spectrum (\ref{['s4f']}) of the cubic hyperbolic perturbation of the spherical oscillator on $\mathbf S^2$ with $\kappa=+1$ for $\mu\in\{0.2,\, 0.12,\, 0.1,\, 0.07\}$ corresponding to $n_{\rm max}\in\{4,\, 6,\, 8,\, 10\}$ (\ref{['s4g']}) starting from the lower dots.

Theorems & Definitions (5)

  • Proposition 1
  • Proposition 2
  • Proposition 3
  • Conjecture 1
  • Conjecture 2