Skip to content
DraconiticResearch
Search Sources API
206,690 studies31 sourcesUpdated 48 min ago
PreprintarXiv licencearXiv

One-Particle Resonances and Eigenstate Thermalization in Periodic Free-Fermion Lattices

Abstract

We study eigenstate fluctuations of the particle number in the nearest-neighbour free-fermion model on the periodic cubic lattice (ℤ/Lℤ)d. For every fixed dimension, every particle number, every subvolume, and every normalized energy eigenstate, we prove a bound of order NLd−1 for the particle-number variance. The corresponding eigenstate-thermalization estimate is of order Ld−1/(Nη2) for fluctuations of relative size η. In particular, at positive particle density the bound decays as the inverse linear size. The proof decomposes the centered particle-number operator according to one-particle energy transfer and treats the zero- and nonzero-transfer components separately. The nonzero-transfer part is controlled by a sharp resonance bound, proved from Mann's theorem on relations among roots of unity, while the zero-transfer part is estimated by a Hilbert-Schmidt argument. These bounds are optimal in every dimension: the maximal nonzero-gap multiplicity has order Ld−1, and suitable many-body eigenstates realize matching variance lower bounds and show that the concentration bound cannot be improved in estimates uniform in the tolerance parameter.

Related

  1. Frequency-dependent capacitance matrix formulation for Fabry--Pérot resonances. Part II: One-dimensional periodic media
    Habib Ammari, Bowen Li, Ping Liu +1
    arXivPreprintarXiv licenceFull textAnalysis & PDEsarXiv
  2. Higher Regularity of Time-Periodic Solutions to Nonautonomous Hyperbolic Problems: Away from Resonances
    Irina Kmit, Lutz Recke
    arXivPreprintCC BY 4.0Full textAnalysis & PDEsarXiv
  3. On the metric spaces of lattices and periodic point sets
    Alexey Garber, iga Virk, Nicolò Zava
    Journal of Applied and Computational TopologyPeer-reviewedCC BY 4.0Full textGeneral mathematicsPMC
  4. Eigenstate thermalisation at the edge for Wigner matrices
    Giorgio Cipolloni, László Erdős, Joscha Henheik
    Annales de l Institut Henri Poincaré Probabilités et StatistiquesPeer-reviewedLicence not statedFull text33 citedStatisticsOpenAlex
  5. Quantum geometry of connected state manifolds: When diabolic points act as bridges between eigenstate manifolds
    Jan Střeleček, Jakub Novotný, Pavel Cejnar
    arXivPreprintCC BY 4.0Full textMathematical physicsQuantum physics & quantum informationarXiv
BibTeX
@misc{benoist2026oneparticle,
  title = {{One-Particle Resonances and Eigenstate Thermalization in Periodic Free-Fermion Lattices}},
  author = {Tristan Benoist and Vojkan Jakšić and Claude-Alain Pillet and Anna Szczepanek and Cornelia Vogel},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2611.12701},
  eprint = {2611.12701},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2611.12701},
}
RIS
TY  - UNPB
TI  - One-Particle Resonances and Eigenstate Thermalization in Periodic Free-Fermion Lattices
AU  - Tristan Benoist
AU  - Vojkan Jakšić
AU  - Claude-Alain Pillet
AU  - Anna Szczepanek
AU  - Cornelia Vogel
PY  - 2026
DA  - 2026/11/09
PB  - arXiv
DO  - 10.48550/arxiv.2611.12701
UR  - https://arxiv.org/abs/2611.12701
AB  - We study eigenstate fluctuations of the particle number in the nearest-neighbour free-fermion model on the periodic cubic lattice (ℤ/Lℤ)^d. For every fixed dimension, every particle number, every subvolume, and every normalized energy eigenstate, we prove a bound of order NL^d−1 for the particle-number variance. The corresponding eigenstate-thermalization estimate is of order L^d−1/(Nη^2) for fluctuations of relative size η. In particular, at positive particle density the bound decays as the inverse linear size. The proof decomposes the centered particle-number operator according to one-particle energy transfer and treats the zero- and nonzero-transfer components separately. The nonzero-transfer part is controlled by a sharp resonance bound, proved from Mann's theorem on relations among roots of unity, while the zero-transfer part is estimated by a Hilbert-Schmidt argument. These bounds are optimal in every dimension: the maximal nonzero-gap multiplicity has order L^d−1, and suitable many-body eigenstates realize matching variance lower bounds and show that the concentration bound cannot be improved in estimates uniform in the tolerance parameter.
ER  -