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Exact Density Profiles of 1D Quantum Fluids in the Thomas-Fermi Limit: Geometric Hierarchy to the Tonks-Girardeau Gas

Hiroki Suyari

Abstract

We present a geometric framework for 1D quantum fluids across interaction regimes in the Thomas-Fermi limit. Based on the Linearization Principle via the $q$-logarithm, macroscopic density profiles form a discrete hierarchy: the ideal Bose gas ($q=1$), the mean-field Gross-Pitaevskii condensate ($q=-1$), and the strongly correlated Tonks-Girardeau gas ($q=-3$). We further derive a universal sound velocity scaling, $c \propto ρ^{(1-q)/4}$. This establishes a non-perturbative link between static geometry and dynamical excitations in many-body systems.

Exact Density Profiles of 1D Quantum Fluids in the Thomas-Fermi Limit: Geometric Hierarchy to the Tonks-Girardeau Gas

Abstract

We present a geometric framework for 1D quantum fluids across interaction regimes in the Thomas-Fermi limit. Based on the Linearization Principle via the -logarithm, macroscopic density profiles form a discrete hierarchy: the ideal Bose gas (), the mean-field Gross-Pitaevskii condensate (), and the strongly correlated Tonks-Girardeau gas (). We further derive a universal sound velocity scaling, . This establishes a non-perturbative link between static geometry and dynamical excitations in many-body systems.
Paper Structure (15 sections, 11 equations, 1 figure)

This paper contains 15 sections, 11 equations, 1 figure.

Figures (1)

  • Figure 1: Normalized density profiles $n(x)/n(0)$ in a harmonic trap derived from the Linearization Principle for different values of the geometric index $q$. The profiles demonstrate the discrete hierarchy from the ideal Bose gas ($q=1$, dashed line), to the mean-field BEC in the Thomas-Fermi limit ($q=-1$, solid line), and the strongly correlated Tonks-Girardeau gas ($q=-3$, dash-dotted line).