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This paper advances the theoretical understanding of lattice few-body quantum systems by establishing rigorous benchmarks and asymptotic expansions for strong-coupling regimes in bosonic trimers. By deriving exact closed-form solutions via uniform elliptic reduction, it provides precise tools for validating numerical schemes used to solve Schrödinger operators on discrete lattices. The work deepens the mathematical foundation required for high-precision simulations of quantum few-body problems and topological band structures.
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A uniform elliptic reduction, an order-matching criterion, and precision benchmarks for the strong-coupling Birman-Schwinger analysis of the lattice three-boson trimer

arXiv2 min read

arXiv:2608.11848v2 Announce Type: replace-cross Abstract: We present a refined strong-coupling Birman-Schwinger analysis of the three-boson lattice Schroedinger operator on Z^2 at the exceptional quasimomentum K = pi. First, we provide an exact closed-form benchmark for the fiber Fredholm determinant, valid for every quasimomentum K, obtained via a uniform elliptic reduction. Second, we formulate and prove a general order-matching criterion that rigorously determines whether a leading-order Fredholm determinant asymptotic, with relative error 1/mu, suffices to fix the constant-order additive energy correction, or if the next-order refinement is required. Applying the criterion at K = pi, we derive the complete strong-coupling ground-state asymptotic expansion z_1^{pi,s}(mu) = -2mu + 6 + 8/mu + O(mu^{-2}), cross-validated against the exact benchmark and two independent high-precision numerical schemes. We rigorously establish the corresponding spectral gap and the Fredholm-determinant underestimation factor 2 + O(mu^{-2}). We independently confirm that the known K = 0 constant requires no analogous refinement. Finally, we contrast the asymptotic precision levels achieved across recent lattice few-body models and draw a structural parallel with the parity-based classification of topological band insulators at time-reversal-invariant momenta.

Abstract:We present a refined strong-coupling Birman-Schwinger analysis of the three-boson lattice Schroedinger operator on Z^2 at the exceptional quasimomentum K = pi. First, we provide an exact closed-form benchmark for the fiber Fredholm determinant, valid for every quasimomentum K, obtained via a uniform elliptic reduction. Second, we formulate and prove a general order-matching criterion that rigorously determines whether a leading-order Fredholm determinant asymptotic, with relative error 1/mu, suffices to fix the constant-order additive energy correction, or if the next-order refinement is required. Applying the criterion at K = pi, we derive the complete strong-coupling ground-state asymptotic expansion z_1^{pi,s}(mu) = -2mu + 6 + 8/mu + O(mu^{-2}), cross-validated against the exact benchmark and two independent high-precision numerical schemes. We rigorously establish the corresponding spectral gap and the Fredholm-determinant underestimation factor 2 + O(mu^{-2}). We independently confirm that the known K = 0 constant requires no analogous refinement. Finally, we contrast the asymptotic precision levels achieved across recent lattice few-body models and draw a structural parallel with the parity-based classification of topological band insulators at time-reversal-invariant momenta.

v2: corrected typos in Tables 2 and 3; refined Corollary 5.4 to include the next-order term; clarified the notation for the series inversion in the proof of Theorem 5.2; added a comparative discussion with the 3D fermionic case. 10 pages

Mathematical Physics (math-ph); Numerical Analysis (math.NA); Spectral Theory (math.SP); Quantum Physics (quant-ph)

arXiv:2608.11848 [math-ph]

(or arXiv:2608.11848v2 [math-ph] for this version)

Full text under the publisher's open licence · 235 words

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