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This paper investigates the spectral properties of Dirac operators on the noncommutative Moyal plane, specifically analyzing how affine deformations and gauge couplings influence local compactness and Landau level degeneracy. By establishing rigorous criteria for these behaviors at metric-degenerate points, the work advances theoretical frameworks in noncommutative quantum mechanics without addressing practical AI or quantum hardware applications.
Affine Left--Right Dirac Data on the Moyal Plane, with an Application to $U(1)_\star$ Gauge Coupling in Noncommutative Quantum Mechanics
arXiv:2605.10250v3 Announce Type: replace-cross Abstract: We study even non-unital Dirac data on the two-dimensional Moyal plane with fixed deformation parameter \(\vartheta\neq0\), whose Dirac operator is affine in the left and right regular coordinate multipliers, with coefficient matrices \(T_L\) and \(T_R\). Two invariants organize this class. The right block controls algebra--Dirac transversality: local compactness holds if and only if \(\det T_R\neq0\), with \(|\det T_R|\) determining the local volume coefficient and \(\operatorname{sgn}\det T_R\) the oriented Gaussian \(K\)-homology pairing. Independently, \(\Gamma=\vartheta(\det T_L-\det T_R)\) controls the spectral regime and, together with \(|\det T_R|\), the exact localized heat trace: \(\Gamma\neq0\) gives infinitely degenerate Landau levels, while for \(\Gamma=0\) in the transverse regime the spectrum is \(\mathbb R\) with empty point spectrum. Applied to Wallet's Landau--Moyal family, the criterion shows that local compactness survives at the metric-degenerate point \(\xi_{\mathrm W}=1\) but fails at \(\xi_{\mathrm W}=-1\), thereby resolving the local-compactness behaviour at both exceptional one-sided points. We then derive a distinguished affine family from a fixed nondegenerate sector \((\hbar_0,\vartheta_0,B_0)\) of the kinematical symmetry group of two-dimensional noncommutative quantum mechanics. The sector fixes the effective Moyal scale \(\vartheta_{\mathrm{eff}}=\vartheta_0/(1-\vartheta_0B_0/\hbar_0)\) and \(T_R\), while an affine \(U(1)_\star\) background coupling deforms only the left affine part of the Dirac operator. Consequently, local compactness, noncommutative volume and \(K\)-homology class remain unchanged, whereas \(\Gamma=\tfrac12(1-eF_{xy}/B_0)\) drives a transition at \(eF_{xy}=B_0\) from Landau levels to spectrum \(\mathbb R\) with empty point spectrum.
Abstract:We study even non-unital Dirac data on the two-dimensional Moyal plane with fixed deformation parameter \(\vartheta\neq0\), whose Dirac operator is affine in the left and right regular coordinate multipliers, with coefficient matrices \(T_L\) and \(T_R\). Two invariants organize this class. The right block controls algebra--Dirac transversality: local compactness holds if and only if \(\det T_R\neq0\), with \(|\det T_R|\) determining the local volume coefficient and \(\operatorname{sgn}\det T_R\) the oriented Gaussian \(K\)-homology pairing. Independently, \(\Gamma=\vartheta(\det T_L-\det T_R)\) controls the spectral regime and, together with \(|\det T_R|\), the exact localized heat trace: \(\Gamma\neq0\) gives infinitely degenerate Landau levels, while for \(\Gamma=0\) in the transverse regime the spectrum is \(\mathbb R\) with empty point spectrum. Applied to Wallet's Landau--Moyal family, the criterion shows that local compactness survives at the metric-degenerate point \(\xi_{\mathrm W}=1\) but fails at \(\xi_{\mathrm W}=-1\), thereby resolving the local-compactness behaviour at both exceptional one-sided points. We then derive a distinguished affine family from a fixed nondegenerate sector \((\hbar_0,\vartheta_0,B_0)\) of the kinematical symmetry group of two-dimensional noncommutative quantum mechanics. The sector fixes the effective Moyal scale \(\vartheta_{\mathrm{eff}}=\vartheta_0/(1-\vartheta_0B_0/\hbar_0)\) and \(T_R\), while an affine \(U(1)_\star\) background coupling deforms only the left affine part of the Dirac operator. Consequently, local compactness, noncommutative volume and \(K\)-homology class remain unchanged, whereas \(\Gamma=\tfrac12(1-eF_{xy}/B_0)\) drives a transition at \(eF_{xy}=B_0\) from Landau levels to spectrum \(\mathbb R\) with empty point spectrum.
40 pages. Substantially revised with a new title and reorganized presentation. The general affine left--right Dirac framework on the Moyal plane is developed first, with NCQM and (U(1)_\star) gauge coupling as applications. Analytic results and the discussion of exceptional Landau spectral triples are strengthened
arXiv:2605.10250 [math-ph]
(or arXiv:2605.10250v3 [math-ph] for this version)
Full text under the publisher's open licence · 273 words
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