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Coherent states for the exotic Landau problem and related properties

Isiaka Aremua

Abstract

This work presents a comprehensive study of the exotic Landau model in a two-dimensional noncommutative plane. Beginning with the classical formulation where two conserved quantities $\mathcal{P}_i$ and $\mathcal{K}_i$ are derived, we proceed to the quantum level where these lead to two independent oscillator representations generating bosonic Fock spaces $Γ_{\mathcal{P}}$ and $Γ_{\mathcal{K}}$. Coherent states satisfying all Klauder's criteria are explicitly constructed, and their physical properties including normalization, continuity, resolution of the identity, temporal stability, and action identity are rigorously proven. We further develop matrix vector coherent states and quaternionic vector coherent states, examining their mathematical structure and physical implications. Detailed calculations of the free particle propagator via path integrals, uncertainty relations, and time evolution of probability densities are provided.

Coherent states for the exotic Landau problem and related properties

Abstract

This work presents a comprehensive study of the exotic Landau model in a two-dimensional noncommutative plane. Beginning with the classical formulation where two conserved quantities and are derived, we proceed to the quantum level where these lead to two independent oscillator representations generating bosonic Fock spaces and . Coherent states satisfying all Klauder's criteria are explicitly constructed, and their physical properties including normalization, continuity, resolution of the identity, temporal stability, and action identity are rigorously proven. We further develop matrix vector coherent states and quaternionic vector coherent states, examining their mathematical structure and physical implications. Detailed calculations of the free particle propagator via path integrals, uncertainty relations, and time evolution of probability densities are provided.
Paper Structure (24 sections, 9 theorems, 117 equations, 4 figures)

This paper contains 24 sections, 9 theorems, 117 equations, 4 figures.

Key Result

Proposition 3.1

This property consists in the following statement: where the norm $||.||_{\mathcal{HS}}$ is that of Hilbert-Schmidt.

Figures (4)

  • Figure 1: Plots of the temporal density of probability $\varrho_{z_0}(z,t)$\ref{['tempdensmeijer000']}: (a): for $m=2$; (b): for $m=5$; (c): for $m=7$, as a function of the angle $\theta \in [0, \pi]$, argument of the complex nmber $z = |z| e^{i\theta}$, and the time $t \in [0, 5]$ (in normalized units).
  • Figure 2: Plots of the Photon Number Distribution (PND) (\ref{['pnd000']}) versus $x = |z|$ and $y= |z'|$: (a) for $m = 2$ and $n = 2$; (b) for $m = 2$ and $n = 10$; (c) for $m = 10$ and $n = 2$.
  • Figure 3: Plots of the function $F(r,\vartheta,\phi)$ (\ref{['func007']}) depending on $r, \vartheta \equiv v \in [0, 2\pi)$, and $\phi \equiv u \in [0, \pi]$: (a): $m = 2, r = \sqrt{2}$; (b): $m = 5, r = \sqrt{2}$; (c): $m = 7, r = \sqrt{2}$.
  • Figure 4: Plots of the temporal probability density $\varrho_{\mathfrak{Q}_0}(\mathfrak{Q},t)$ (\ref{['qvcstempdens000']}) versus $V_0(t) \equiv \vartheta_0(t) = \vartheta_0 - \omega^{*}t \in [0, 2\pi), t \in [0, \infty)$ (in normalized units) and $V\equiv\vartheta \in [0, 2\pi)$, with $\omega^{*} = 2.5. 10^{-3}$(in normalized units) and $r_0, r$ and $\rho$ fixed:(a): $m = 2, \vartheta =\pi/6$; (b): $m = 5, \vartheta =\pi/6$; (c): $m = 7, \vartheta =\pi/6$; (d): $m = 2, \vartheta_0= \pi/6$; (e): $m = 5, \vartheta_0 =\pi/6$; (f): $m = 7, \vartheta_0 = \pi/6$. .

Theorems & Definitions (13)

  • Remark 2.1
  • Proposition 3.1
  • Proposition 3.2
  • Proposition 3.3
  • Proposition 3.4
  • Remark 3.5
  • Proposition 3.6
  • Proposition 4.1
  • Remark 4.2
  • Proposition 4.3
  • ...and 3 more