Skip to content
DraconiticResearch
Search Sources API
178,033 studies31 sourcesUpdated 17 min ago
PreprintCC BY 4.0arXiv

Exact fermionic matrix elements from the Bethe-ansatz solution of the Richardson-Gaudin model

Abstract

We introduce an effective Hamiltonian description of mesoscopic superconducting systems based on the Bethe-ansatz solution of the Richardson--Gaudin model. Our central result is a compact determinant formula for the matrix elements of fermionic creation and annihilation operators, expressed entirely in terms of eigenvalue-based variables. This formula allows single-electron tunneling terms to be represented directly in the eigenbasis of the Richardson--Gaudin model, extending the eigenvalue-based framework beyond overlaps and previously known form factors. As a benchmark, we apply the method to a superconducting Anderson impurity model comprising a quantum dot coupled to an ultrasmall superconducting grain. The resulting low-energy description, formulated naturally in the canonical ensemble, captures even-odd effects, subgap excitations, and quantum-dot physics. The same framework gives access to observables not previously computed for such grain-dot systems in the canonical ensemble, such as the fixed-particle-number optical conductivity and flux-tunable spectra.

Related

  1. The Quasiparticle Ansatz for Relativistic Continuous Matrix Product States
    Silviu S. Pufu, Benjamin T. Søgaard, Spyros Terlemes
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsarXiv
  2. Hydrodynamic description of correlation matrix eigenvalues in a finite temperature expanding free fermionic gas
    Atharva Naik, Madhumita Saha, David A. Huse +2
    arXivPreprintarXiv licenceFull textAtomic, molecular & optical physicsCondensed matterarXiv
  3. Universal random matrix behavior of a Fermionic quantum gas
    Maxime Dixmerias, Giuseppe Del Vecchio Del Vecchio, Cyprien Daix +6
    Nature CommunicationsPeer-reviewedCC BY-NC-ND 4.0Full text2 citedCondensed matterQuantum physics & quantum informationCrossrefHAL
  4. Systematic study of E2 matrix elements in the framework of the Triaxial Projected Shell Model
    Stefan Frauendorf, Syed Rouoof, Gowhar Bhat +5
    arXivPreprintCC BY 4.0Full textNuclear physicsarXiv
  5. Breaking the Spin Degeneracy for Distributions of Off-Diagonal Scattering Matrix Elements in the Case of Symplectic Symmetry
    Nils Gluth, Thomas Guhr
    arXivPreprintarXiv licenceFull textMathematical physicsHigh-energy & particle physicsarXiv
BibTeX
@misc{johannsen2026exact,
  title = {{Exact fermionic matrix elements from the Bethe-ansatz solution of the Richardson-Gaudin model}},
  author = {Peter D. Johannsen and Valerii K. Kozin and Jelena Klinovaja and Daniel Loss},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2611.03141},
  eprint = {2611.03141},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2611.03141},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Exact fermionic matrix elements from the Bethe-ansatz solution of the Richardson-Gaudin model
AU  - Peter D. Johannsen
AU  - Valerii K. Kozin
AU  - Jelena Klinovaja
AU  - Daniel Loss
PY  - 2026
DA  - 2026/11/02
PB  - arXiv
DO  - 10.48550/arxiv.2611.03141
UR  - https://arxiv.org/abs/2611.03141
AB  - We introduce an effective Hamiltonian description of mesoscopic superconducting systems based on the Bethe-ansatz solution of the Richardson--Gaudin model. Our central result is a compact determinant formula for the matrix elements of fermionic creation and annihilation operators, expressed entirely in terms of eigenvalue-based variables. This formula allows single-electron tunneling terms to be represented directly in the eigenbasis of the Richardson--Gaudin model, extending the eigenvalue-based framework beyond overlaps and previously known form factors. As a benchmark, we apply the method to a superconducting Anderson impurity model comprising a quantum dot coupled to an ultrasmall superconducting grain. The resulting low-energy description, formulated naturally in the canonical ensemble, captures even-odd effects, subgap excitations, and quantum-dot physics. The same framework gives access to observables not previously computed for such grain-dot systems in the canonical ensemble, such as the fixed-particle-number optical conductivity and flux-tunable spectra.
ER  -