Diagonalizing Bose Gases in the Gross-Pitaevskii Regime and Beyond
Morris Brooks
TL;DR
This work develops an algebraic, Bogoliubov-type diagonalization framework for dilute Bose gases in the GP regime and beyond. By combining a Feshbach–Schur renormalization of the two-body interaction with a many-body transformation, it obtains a block-diagonal Hamiltonian that yields a rigorous lower bound matching the GP energy plus the Lee-Huang-Yang (LHY) correction, and it characterizes the low-lying excitation spectrum. The analysis extends to scaling exponents $0\le \kappa<\tfrac{1}{8}$, establishing a sharp link between the many-body spectrum and the Bogoliubov predictions up to $N^{-\tau}$ corrections, and provides an improved upper bound on the ground-state energy that includes a logarithmic $\log N / N$ term. Central to the approach are careful error controls of Bogoliubov-type terms, a priori condensation estimates, and the construction of trial states that annihilate the relevant quasiparticle operators, enabling precise energy comparisons.
Abstract
We present a novel approach to the Bogoliubov theory of dilute Bose gases, allowing for an elementary derivation of the celebrated Lee-Huang-Yang formula in the Gross-Pitaevskii regime. Furthermore, we identify the low lying excitation spectrum beyond the Gross-Pitaevskii scaling, extending a recent result [3] to significantly more singular scaling regimes. Finally, we provide an upper bound on the ground state energy in the Gross-Pitaevskii regime that captures the correct expected order of magnitude beyond the Lee-Huang-Yang formula.
