Permutation defects between wavefunction replicas yield multipartite entanglement measures that capture the chiral central charge from bulk states in chiral topological phases.
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Girsanov transformation on an SDE representation of the Fermi-Hubbard model yields a factorization-independent formula that proves antiferromagnetic signs for spin-spin correlations at half-filling on bipartite lattices at any temperature and supplies approximate ground-state energies via ODEs.
Generalized coherent information acts as a sharp phase-transition indicator over the entire p-T plane in the 2D ±J random-bond Ising model, yielding a high-precision multicritical point estimate p_c=0.1092212(4) with reduced finite-size effects.
citing papers explorer
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Probing chiral topological states with permutation defects
Permutation defects between wavefunction replicas yield multipartite entanglement measures that capture the chiral central charge from bulk states in chiral topological phases.
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Thermodynamics of the Fermi-Hubbard Model through Stochastic Calculus and Girsanov Transformation
Girsanov transformation on an SDE representation of the Fermi-Hubbard model yields a factorization-independent formula that proves antiferromagnetic signs for spin-spin correlations at half-filling on bipartite lattices at any temperature and supplies approximate ground-state energies via ODEs.
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Revisiting Nishimori multicriticality through the lens of information measures
Generalized coherent information acts as a sharp phase-transition indicator over the entire p-T plane in the 2D ±J random-bond Ising model, yielding a high-precision multicritical point estimate p_c=0.1092212(4) with reduced finite-size effects.