Spectral functions of the strongly interacting 3D Fermi gas
arXiv:2311.03953 · doi:10.1103/PhysRevA.109.023324
Abstract
Computing dynamical properties of strongly interacting quantum many-body systems poses a major challenge to theoretical approaches. Usually, one has to resort to numerical analytic continuation of results on imaginary frequencies, which is a mathematically ill-defined procedure. Here, we present an efficient method to compute the spectral functions of the two-component Fermi gas near the strongly interacting unitary limit directly in real frequencies. To this end, we combine the Keldysh path integral that is defined in real time with the self-consistent T-matrix approximation. The latter is known to predict thermodynamic and transport properties in good agreement with experimental observations in ultracold atoms. We validate our method by comparison with thermodynamic quantities obtained from imaginary time calculations and by transforming our real-time propagators to imaginary time. By comparison with state-of-the-art numerical analytic continuation of the imaginary time results, we show that our real-time results give qualitative improvements for dynamical quantities. Moreover, we show that no significant pseudogap regime exists in the self-consistent T-matrix approximation above the critical temperature , an issue that has been under significant debate. We close by pointing out the versatile nature of our method as it can be extended to other systems, like the spin- or mass-imbalanced Fermi gas, other Bose-Fermi models, 2D systems as well as systems out of equilibrium.
21 pages, 11 figures
References in corpus (27)
- Many-Body Physics with Ultracold Gases
- Fermi-liquid instabilities at magnetic quantum phase transitions
- Weakly bound dimers of fermionic atoms
- Using photoemission spectroscopy to probe a strongly interacting Fermi gas
- Generalized Virial Theorem and Pressure Relation for a strongly correlated Fermi gas
- The Equation of State of a Low-Temperature Fermi Gas with Tunable Interactions
- Thermodynamics of the BCS-BEC crossover
- Phase diagram of a two-component Fermi gas with resonant interactions
- Observation of pseudogap behavior in a strongly interacting Fermi gas
- Repulsive Fermi polarons in a resonant mixture of ultracold Li atoms
- Quantum Fluctuations in the Superfluid State of the BCS-BEC Crossover
- Determination of the Superfluid Gap in Atomic Fermi Gases by Quasiparticle Spectroscopy
- Viscosity and scale invariance in the unitary Fermi gas
- Excitation spectra and rf-response near the polaron-to-molecule transition from the functional renormalization group
- Phase diagram of a cold polarized Fermi gas
- Large-N expansion for unitary superfluid Fermi gases
- Spectral response and contact of the unitary Fermi gas
- Numerical analytic continuation: Answers to well-posed questions
- Breathing mode of two-dimensional atomic Fermi gases in harmonic traps
- High-precision numerical solution of the Fermi polaron problem and large-order behavior of its diagrammatic series
- Bosonic Nevanlinna Analytic Continuation
- Beyond-mean-field description of a trapped unitary Fermi gas with mass and population imbalance
- Hetero pairing and component-dependent pseudogap phenomena in an ultracold Fermi gas with mass imbalance
- Evolution of an attractive polarized Fermi gas: From a Fermi liquid of polarons to a non-Fermi liquid at the Fulde-Ferrell-Larkin-Ovchinnikov quantum critical point
- Marginal Fermi liquid at magnetic quantum criticality from dimensional confinement
- Particle and pair spectra for strongly correlated Fermi gases: A real-frequency solver
- Peaks and widths of radio-frequency spectra: An analysis of the phase diagram of ultra-cold Fermi gases
Cited by in corpus (5)
- Theory of the spectral function of Fermi polarons at finite temperature
- Spectral properties and observables in ultracold Fermi gases
- Particle and pair spectra for strongly correlated Fermi gases: A real-frequency solver
- Quantum transport in strongly correlated Fermi gases
- Non-thermal pairing glue of electrons in the steady state