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Tight binding models for high temperature superconductors


This page lists a set of tight-binding models that are suitable to describe high temperature superconductors

Some of the models have been compiled from the literature for comparison, others are calculated using first principles calculations or adjusted to match experimental measured quantities.
For each model, the hopping parameters are given in a comma separated file (csv), and basic plots of the band structure and Fermi surface are provided for comparison. The tight-binding file contains lines with the following format:
rx, ry, rz, a, b, Re(t), Im(t)
Here ri is the i-th component of the real space vector that describes the hopping process, a and b are integer numbers labeling the orbitals and the last two entries are the real and imaginary part of the hopping (usually given in eV).
The corresponding Bloch Hamiltonian (in orbital representation) can be obtained by a Fourier transform and summation over all lines to yield the matrix Hab.

Models


Directory up
./2d_kz_NaN2d version of model, hoppings out of plane ignored
./2d_kz_12d version of model at kz=pi
./2d_kz_02d version of model at kz=0
5 band model for FeSe matching the eigenenergies as measured within Bogoliubov quasiparticle interference (BQPI, Sprau et al.) and consistent with ARPES measurements of the Fermi surface and with measurements of estimated areas of Fermi surface cuts via quantum oscillations (Terashima et al.). The data file can be downloaded from the links below. The spin-orbit coupling is approximately included as (imaginary) on-site couplings as, described in
Andreas Kreisel, Yan Wang, Thomas A. Maier, Peter J. Hirschfeld, Douglas J. Scalapino
Phys. Rev. B 88, 094522 (2013)
Spin fluctuations and superconductivity in KxFe2-ySe2

If you use the data provided here, please cite the original work that published the tight binding parameters:
Peter O. Sprau, Andrey Kostin, Andreas Kreisel, Anna E. Böhmer, Valentin Taufour, Paul C. Canfield, Shantanu Mukherjee, Peter J. Hirschfeld, Brian M. Andersen, J.C. Séamus Davis
Science, 357, 75 (2017)
Discovery of Orbital-Selective Cooper Pairing in FeSe
the same tight file is also published in the supplemental materials here
Two-dimensional models derived from this electronic structure can be found following the links above.

This model has also been used in the following works:
A. Kreisel, Brian M. Andersen, Peter O. Sprau, Andrey Kostin, J.C. Séamus Davis, P. J. Hirschfeld
Phys. Rev. B 95, 174504 (2017)
Orbital selective pairing and gap structures of iron-based superconductors

Download model and figures: FeSe_BQPI.tar.gz


Download model and figures: FeSe_highres_3d.tar.gz

ChiqData_FeSe_5_SM_hr.datpath.png
Susceptibility in the nematic state of FeSe calculated using a model including orbital selective quasiparticle weights that enhances spin-fluctuations at (π, 0).
FeSe_5Fermisurf_1.png
Fermi surface of FeSe from the tight-binding parametrization.
FeSe_5Gammakkp5_FeSe_5_dress_1222_hr.txtcGapfunction_1.png
Superconducting order parameter as calculated from a modified spin-fluctuation theory.
FeSe_5_SM++.txt_klistbands.png
Details of the electronic structure along high symmetry directions, colors indicate orbital with largest matrix element.
FeSe_5_SM_hr_vFermi.png
Fermi velocity as calculated from the tight-binding parameterization.
Gammakkp5_FeSe_5_SM.txtc_dos_gf_new.png
Density of states of the tight-binding model.

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