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Entanglement Content of Quasi-Particle Excitations

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arxiv 1805.04948 v1 pith:BQFTOPZT submitted 2018-05-13 cond-mat.stat-mech hep-thmath-phmath.MPquant-ph

Entanglement Content of Quasi-Particle Excitations

classification cond-mat.stat-mech hep-thmath-phmath.MPquant-ph
keywords entanglementexcitationsquantumquasi-particlefinitechaincontentharmonic
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We investigate the quantum entanglement content of quasi-particle excitations in extended many-body systems. We show that such excitations give an additive contribution to the bi-partite von Neumann and R\'enyi entanglement entropies that takes a simple, universal form. It is largely independent of the momenta and masses of the excitations, and of the geometry, dimension and connectedness of the entanglement region. The result has a natural quantum information theoretic interpretation as the entanglement of a state where each quasi-particle is associated with two qubits representing their presence within and without the entanglement region, taking into account quantum (in)distinguishability. This applies to any excited state composed of finite numbers of quasi-particles with finite De Broglie wavelengths or finite intrinsic correlation length. We derive this result analytically in one-dimensional massive bosonic and fermionic free field theories and for simple setups in higher dimensions. We provide numerical evidence for the harmonic chain and the two-dimensional harmonic lattice in all regimes where excitations have quasi-particle properties. Finally, we provide supporting calculations for integrable spin chain models and other situations without particle production. Our results point to new possibilities for creating entangled states using many-body quantum systems.

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Cited by 2 Pith papers

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    In the Federbush model, branch-point twist field form factors and first-order quench corrections are independent of the topological coupling λ, so Rényi entropies of the infinite-volume vacuum match two free Dirac fermions.

  2. Additivity of disjoint interval entanglement in quasiparticle excited states

    quant-ph 2026-01 conditional novelty 6.0

    For quasiparticle excited states with large momentum differences, double-interval reflected entropy, mutual information, and logarithmic negativity add: X_{K1∪K2} = X_{K1} + X_{K2}.