triqs_ctint.solver.Solver

class triqs_ctint.solver.Solver(beta, gf_struct, n_iw=500, n_tau=5001, use_D=False, use_Jperp=False, n_tau_dynamical_interactions=5001, n_iw_dynamical_interactions=500)

Methods

__init__(beta, gf_struct[, n_iw, n_tau, ...])	Initialise the solver.
hdf5_format	Signature : () -> str
post_process	Signature : () -> None
solve(**params_kw)	Solve the impurity problem.

Attributes

D0_iw	Dynamic density-density interaction in Matsubara frequencies
F_iw	The two-particle vertex function in purely fermionic notation (iw1, iw2, iw3)
G0_iw	Noninteracting Green Function in Matsubara frequencies
G0_shift_iw	The shifted noninteracting Green Function in Matsubara frequencies
G0_shift_tau	The shifted noninteracting Green Function in imaginary time
G2_iw	The two-particle Green function
G2c_iw	The connected part of the two-particle Green function
G_iw	Greens function in Matsubara frequencies (Eq.
Jperp_iw	Dynamic spin-spin interaction in Matsubara frequencies
M3ph_delta	Equal-time peak in M3ph_tau
M3ph_iw	Building block for the fermion boson vertex (ph channel) in Matsubara frequencies
M3ph_iw_nfft	Building block for the fermion boson vertex (ph channel) in Matsubara frequencies using NFFT
M3ph_tau	Building block for the fermion boson vertex (ph channel) in imaginary time
M3pp_delta	Equal-time peak in M3pp_tau
M3pp_iw	Building block for the fermion boson vertex (pp channel) in Matsubara frequencies
M3pp_iw_nfft	Building block for the fermion boson vertex (pp channel) in Matsubara frequencies using NFFT
M3pp_tau	Building block for the fermion boson vertex (pp channel) in imaginary time
M4_iw	Building block for the full vertex function measured directly in Matsubara frequencies using NFFT
M_hartree	Hartree-term of M_tau
M_iw	The Fourier-transform of M_tau.
M_iw_nfft	Same as M_tau, but measured directly in Matsubara frequencies using NFFT
M_tau	Building block for the Green function in imaginary time (Eq.
Sigma_iw	Self-energy in Matsubara frequencies.
auto_corr_time	Auto-correlation time
average_k	Average perturbation order
average_sign	Average sign of the CTINT
chi2ph_conn_tau_from_M3	M2 in the particle-hole channel in imaginary time as obtained from M3
chi2ph_iw	The equal time correlator $chi_2$ in the particle-hole channel in Matsubara frequencies
chi2ph_iw_from_M3	The equal time correlator $chi_2$ in the particle-hole channel in imaginary frequencies as obtained from M3ph_tau
chi2ph_tau	The equal time correlator $chi_2$ in the particle-hole channel in imaginary times as obtained by operator insertion
chi2ph_tau_from_M3	The equal time correlator $chi_2$ in the particle-hole channel in imaginary times as obtained from M3ph_tau
chi2pp_conn_tau_from_M3	M2 in the particle-particle channel in imaginary time as obtained from M3
chi2pp_iw	The equal time correlator $chi_2$ in the particle-particle channel in Matsubara frequencies
chi2pp_iw_from_M3	The equal time correlator $chi_2$ in the particle-particle channel in imaginary frequencies as obtained from M3pp_tau
chi2pp_tau	The equal time correlator $chi_2$ in the particle-particle channel in imaginary times as obtained by operator insertion
chi2pp_tau_from_M3	The equal time correlator $chi_2$ in the particle-particle channel in imaginary times as obtained from M3pp_tau
chi3ph_iw	The equal time correlator $chi_3$ in the particle-hole channel in Matsubara frequencies
chi3ph_iw_nfft	The equal time correlator $chi_3$ in the particle-hole channel in Matsubara frequencies as obtained by the NFFT $M_3$ measurement
chi3pp_iw	The equal time correlator $chi_3$ in the particle-particle channel in Matsubara frequencies
chi3pp_iw_nfft	The equal time correlator $chi_3$ in the particle-particle channel in Matsubara frequencies as obtained by the NFFT $M_3$ measurement
chiAB_iw	The correlation function $chi_AB$ in imaginary frequencies
chiAB_tau	The correlation function $chi_AB$ in imaginary times
constr_params
density	The density matrix (measured by operator insertion)
histogram	Average perturbation order distribution
last_solve_params