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The Bogoliubov quantum-depletion law for the dilute Bose gas in the thermodynamic limit

For hard spheres (October 5): for every bounded continuous ff and ε>0\varepsilon>0, at all sufficiently small fixed ρ\rho, every thermodynamic accumulation value of 1Nρa3∑k≠0f(k/8πρa) n(k)\frac{1}{N\sqrt{\rho a^3}}\sum_{k\ne0}f(k/\sqrt{8\pi\rho a})\,n(k) is within ε\varepsilon of ∫f dνBog\int f\,d\nu_{\mathrm{Bog}}, uniformly over ground states; taking f=1f=1 gives depletion 83πρa3+o(ρa3)\frac{8}{3\sqrt\pi}\sqrt{\rho a^3}+o(\sqrt{\rho a^3}). A companion proves the same depletion asymptotic for fixed bounded, nonnegative, radial, finite-range potentials with positive scattering length. Not covered: positive temperature, the next-order correction, or unbounded non-hard-core potentials.

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Occurred: Oct 5, 2026

Delta type: SOURCE CLAIM

Assumptions: VibeMathed verification: unreviewed. Publication: announcement. AI contribution: ai-discovered. VibeMathed editorial classifications, scores, notes, relations, and dataset structure are CC BY 4.0. Source statements and linked content retain their own rights.

Canonical aliases: The Bogoliubov quantum-depletion law for the dilute Bose gas in the thermodynamic limit · Bogoliubov depletion law

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VibeMathed record: The Bogoliubov quantum-depletion law for the dilute Bose gas in the thermodynamic limit evidence for this event

The Bogoliubov quantum-depletion law for the dilute Bose gas in the thermodynamic limit evidence for this event

Related: Bose-Einstein condensation at positive temperature in the dilute hard-sphere gas evidence for this event

Companion: Quantum Depletion for Fixed Bounded Repulsive Potentials (October 5, 2026) evidence for this event

For hard spheres (October 5): for every bounded continuous ff and ε>0\varepsilon>0, at all sufficiently small fixed ρ\rho, every thermodynamic accumulation value of 1Nρa3∑k≠0f(k/8πρa) n(k)\frac{1}{N\sqrt{\rho a^3}}\sum_{k\ne0}f(k/\sqrt{8\pi\rho a})\,n(k) is within ε\varepsilon of ∫f dνBog\int f\,d\nu_{\mathrm{Bog}}, uniformly over ground states; taking f=1f=1 gives depletion 83πρa3+o(ρa3)\frac{8}{3\sqrt\pi}\sqrt{\rho a^3}+o(\sqrt{\rho a^3}). A companion proves the same depletion asymptotic for fixed bounded, nonnegative, radial, finite-range potentials with positive scattering length. Not covered: positive temperature, the next-order correction, or unbounded non-hard-core potentials. parent of this event

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