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arXiv:0905.3539 · Journal of Computational and Applied Mathematics

Fisher information and kinetic energy functionals: A dequantization approach

Ian P. Hamilton, Ricardo Antonio Mosna

Published Mar 1, 2009• 20 citations
arXivHTMLPDF
DOI
10.1016/j.cam.2009.02.087

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Multi-Sector Forge ISA: Non-Commutativity of Sector Dequantizations and Annealing-Order-Dependent Computation

Ian Richard C Buckley

PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The Forge ISA operates with a single annealing parameter β. For systems with multiple coupled degrees of freedom, the natural generalisation assigns an independent β_i to each sector. The central result is a non-commutativity theorem: the sector dequantization operators T_∞^c and T_∞^s satisfy [T_∞^c, T_∞^s] = 0 ⟺ I_cs = 0 where I_cs = ⟨H_c H_s⟩ − ⟨H_c⟩⟨H_s⟩ is the off-diagonal Fisher information coupling. When sectors are coupled (I_cs ≠ 0), dequantization order matters: the joint e-geodesic path on the product Fisher manifold outperforms sector-by-sector annealing by ΔE = 0.35 at U = 4t on the half-filled 4-site Hubbard chain (99.3% vs 82.7% of ground state energy). A new Hubbard limit is identified: the spin-frozen limit (β_s → ∞, β_c finite) reduces to a hard-core Bose gas, complementing the known charge-frozen limit (Heisenberg AFM, Anderson 1959). The annealing-order holonomy is the thermodynamic analogue of the Aharonov-Bohm effect, largest near the Mott transition where Fisher curvature peaks. Series: Paper 325 (doi:10.5281/zenodo.20400638) → Paper 419 (doi:10.5281/zenodo.20694527) → Paper 443 (doi:10.5281/zenodo.20752384) → Paper 453 (this paper). Keywords Forge ISA, multi-sector annealing, non-commutativity, Fisher information, Hubbard model, hard-core Bose gas, Mott transition, information geometry, e-geodesic, annealing order, holonomy, Aharonov-Bohm, thermodynamic computation, natural gradient, dequantization

•Jun 20, 2026•0 citations
We present a dequantization procedure based on a variational approach whereby quantum fluctuations latent in the quantum momentum are suppressed. This is done by adding generic local deformations to the quantum momentum operator which give rise to a deformed kinetic term quantifying the amount of ``fuzzyness'' caused by such fluctuations. Considered as a functional of such deformations, the deformed kinetic term is shown to possess a unique minimum which is seen to be the classical kinetic energy. Furthermore, we show that extremization of the associated deformed action functional introduces an essential nonlinearity to the resulting field equations which are seen to be the classical Hamilton-Jacobi and continuity equations. Thus, a variational procedure determines the particular deformation that has the effect of suppressing the quantum fluctuations, resulting in dequantization of the system.
PENDING QUALITY AUDIT (2026-08). The file is restricted while this record is reviewed as part of a systematic audit of the author's corpus. It has not yet been assessed. Metadata and DOI remain public, and access can be requested. The Forge ISA operates with a single annealing parameter β. For systems with multiple coupled degrees of freedom, the natural generalisation assigns an independent β_i to each sector. The central result is a non-commutativity theorem: the sector dequantization operators T_∞^c and T_∞^s satisfy [T_∞^c, T_∞^s] = 0 ⟺ I_cs = 0 where I_cs = ⟨H_c H_s⟩ − ⟨H_c⟩⟨H_s⟩ is the off-diagonal Fisher information coupling. When sectors are coupled (I_cs ≠ 0), dequantization order matters: the joint e-geodesic path on the product Fisher manifold outperforms sector-by-sector annealing by ΔE = 0.35 at U = 4t on the half-filled 4-site Hubbard chain (99.3% vs 82.7% of ground state energy). A new Hubbard limit is identified: the spin-frozen limit (β_s → ∞, β_c finite) reduces to a hard-core Bose gas, complementing the known charge-frozen limit (Heisenberg AFM, Anderson 1959). The annealing-order holonomy is the thermodynamic analogue of the Aharonov-Bohm effect, largest near the Mott transition where Fisher curvature peaks. Series: Paper 325 (doi:10.5281/zenodo.20400638) → Paper 419 (doi:10.5281/zenodo.20694527) → Paper 443 (doi:10.5281/zenodo.20752384) → Paper 453 (this paper). Keywords Forge ISA, multi-sector annealing, non-commutativity, Fisher information, Hubbard model, hard-core Bose gas, Mott transition, information geometry, e-geodesic, annealing order, holonomy, Aharonov-Bohm, thermodynamic computation, natural gradient, dequantization