Ground states of fermionic Hamiltonians limited to M-body interactions cannot achieve maximal M-body entanglement.
lY σ=1 Nσ mσ # ln lQ σ=1 D/l mσ lQ σ=1 Nσ mσ (S43) The symmetry refined upper bound to the entropy then becomes S(M) max(N1, . . . , Nl) = ′X m1,...,ml
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Many-Body Entanglement Properties of Finite Interacting Fermionic Hamiltonians
Ground states of fermionic Hamiltonians limited to M-body interactions cannot achieve maximal M-body entanglement.