Consequently, a chemical potential term −µ ˆN would only shift ener- gies by a constant −µN in that sector and hence shift µ1 by the same constant

Physically, we work in the canonical ensemble, diagonalize ˆHHub in a fixed- N particle sector

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quant-ph · 2026-03-11 · unverdicted · novelty 7.0

Ground states of fermionic Hamiltonians limited to M-body interactions cannot achieve maximal M-body entanglement.

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Many-Body Entanglement Properties of Finite Interacting Fermionic Hamiltonians quant-ph · 2026-03-11 · unverdicted · none · ref 52
Ground states of fermionic Hamiltonians limited to M-body interactions cannot achieve maximal M-body entanglement.