Linear Response Functions Respecting Ward-Takahashi Identity and Fluctuation-Dissipation Theorem within Approximation
arXiv:2208.10401 · doi:10.1103/PhysRevB.107.085106
Abstract
The calculation of response functions in correlated electronic systems is one of the most important problems in the condensed matter physics. To obtain a physical response function, preserving both the Ward-Takahashi identity and the fluctuation-dissipation theorem are crucial. Here we propose a self-consistent many body method within the GW framework to calculate the response functions based on the fluctuation-dissipation theorem, which also satisfies the Ward-Takahashi identity. The validity of this methodology is demonstrated on the two-dimensional one-band Hubbard model, where both the Ward-Takahashi identity and fluctuation-dissipation theorem are verified numerically. Moreover, comparing to the accurate spin susceptibility of the determinantal Monte Carlo approach, the results obtained from our method are quite satisfactory and the computational cost are greatly reduced.
arXiv comment12 pages, 4 figures, supplemental material 15 pages
References in corpus (8)
- The GW method
- The GW compendium: A practical guide to theoretical photoemission spectroscopy
- Tracking the Footprints of Spin Fluctuations: A MultiMethod, MultiMessenger Study of the Two-Dimensional Hubbard Model
- Spin-dependent Hedin's equations
- Chiral anomaly and strength of the electron-electron interaction in graphene
- How to read between the lines of electronic spectra: the diagnostics of fluctuations in strongly correlated electron systems
- Covariant gaussian approximation in Ginzburg - Landau model
- Full self-consistency versus quasiparticle self-consistency in diagrammatic approaches: Exactly solvable two-site Hubbard Model