triqs_ctint.solver_core.SolverCore
- class triqs_ctint.solver_core.SolverCore
Bases:
objectThe CT-INT solver.
Dispatched C++ constructor(s).
[1] (constr_params_: ConstrParamsT)
Construct a CT-INT solver.
- Parameters:
- constr_params_ConstrParamsT
Set of parameters used to construct the solver.
Attributes
Dynamic density-density interaction \(D_0(i\omega)\) in Matsubara frequencies (DLR mesh).
The two-particle vertex function \(F\) in purely fermionic notation.
The two-particle vertex function \(F\) (particle-hole channel).
The two-particle vertex function \(F\) (particle-particle channel).
Non-interacting Green's function \(G_0(i\omega)\) in Matsubara frequencies.
Inverse of the non-interacting Green's function \(G_0^{-1}(i\omega)\).
The shifted non-interacting Green's function in Matsubara frequencies.
The shifted non-interacting Green's function in imaginary time.
Connected part of the two-particle Green's function \(G^{(2)}\).
The two-particle Green's function \(G^{(2)}\).
Connected part of the two-particle Green's function \(G^{(2)}\) (particle-hole channel).
The two-particle Green's function \(G^{(2)}\) (particle-hole channel).
Connected part of the two-particle Green's function \(G^{(2)}\) (particle-particle channel).
The two-particle Green's function \(G^{(2)}\) (particle-particle channel).
Green's function \(G(i\omega)\) in Matsubara frequencies.
Dynamic spin-spin interaction \(J_\perp(i\omega)\) in Matsubara frequencies (DLR mesh).
Equal-time peak of \(M^{(3)}_{ph}(\tau)\).
Building block \(M^{(3)}_{ph}(i\omega)\) (particle-hole channel) for the fermion-boson vertex in Matsubara frequencies.
Building block \(M^{(3)}_{ph}(i\omega)\) (particle-hole channel) for the fermion-boson vertex, measured using NFFT.
Building block \(M^{(3)}_{ph}(\tau)\) (particle-hole channel) for the fermion-boson vertex in imaginary time.
Equal-time peak of \(M^{(3)}_{pp}(\tau)\).
Building block \(M^{(3)}_{pp}(i\omega)\) (particle-particle channel) for the fermion-boson vertex in Matsubara frequencies.
Building block \(M^{(3)}_{pp}(i\omega)\) (particle-particle channel) for the fermion-boson vertex, measured using NFFT.
Building block \(M^{(3)}_{pp}(\tau)\) (particle-particle channel) for the fermion-boson vertex in imaginary time.
Equal-time peak of \(M^{(3)}_{xph}(\tau)\).
Building block \(M^{(3)}_{xph}(i\omega)\) (particle-hole-cross channel) for the fermion-boson vertex in Matsubara frequencies.
Building block \(M^{(3)}_{xph}(\tau)\) (particle-hole-cross channel) for the fermion-boson vertex in imaginary time.
Building block \(M^{(4)}(i\omega)\) for the full vertex, measured in Matsubara frequencies using NFFT.
Building block \(M^{(4)}_{ph}(i\omega)\) (particle-hole channel) for the full vertex, measured using NFFT.
Building block \(M^{(4)}_{pp}(i\omega)\) (particle-particle channel) for the full vertex, measured using NFFT.
Hartree term of \(M(\tau)\).
Fourier transform of \(M(\tau)\).
Same as \(M(\tau)\), but measured directly in Matsubara frequencies using NFFT on the DLR grid.
Building block for the Green's function in imaginary time \(M(\tau)\).
Dynamic self-energy \(\Sigma_{dyn}(i\omega)\) in Matsubara frequencies (DLR, decays to zero).
Static (Hartree) part of the self-energy, \(\Sigma = \Sigma_{dyn} + \Sigma_{hartree}\).
Accumulation time in seconds.
Auto-correlation time.
Average perturbation order.
Error bar on the average perturbation order.
Average Monte-Carlo sign.
Error bar on the average sign.
Connected \(\chi^{(2)}\) (particle-hole channel) in imaginary time, obtained from \(M^{(3)}\).
Correlator \(\chi^{(2)}_{ph}(i\omega)\) (particle-hole channel) in Matsubara frequencies.
Correlator \(\chi^{(2)}_{ph}(i\omega)\) (particle-hole channel), obtained from \(M^{(3)}_{ph}(\tau)\).
Correlator \(\chi^{(2)}_{ph}(\tau)\) (particle-hole channel) in imaginary time, obtained by operator insertion.
Correlator \(\chi^{(2)}_{ph}(\tau)\) (particle-hole channel), obtained from \(M^{(3)}_{ph}(\tau)\).
Connected \(\chi^{(2)}\) (particle-particle channel) in imaginary time, obtained from \(M^{(3)}\).
Correlator \(\chi^{(2)}_{pp}(i\omega)\) (particle-particle channel) in Matsubara frequencies.
Correlator \(\chi^{(2)}_{pp}(i\omega)\) (particle-particle channel), obtained from \(M^{(3)}_{pp}(\tau)\).
Correlator \(\chi^{(2)}_{pp}(\tau)\) (particle-particle channel) in imaginary time, obtained by operator insertion.
Correlator \(\chi^{(2)}_{pp}(\tau)\) (particle-particle channel), obtained from \(M^{(3)}_{pp}(\tau)\).
Connected \(\chi^{(2)}\) (particle-hole-cross channel) in imaginary time, obtained from \(M^{(3)}\).
Correlator \(\chi^{(2)}_{xph}(i\omega)\) (particle-hole-cross channel), obtained from \(M^{(3)}_{xph}(\tau)\).
Correlator \(\chi^{(2)}_{xph}(\tau)\) (particle-hole-cross channel), obtained from \(M^{(3)}_{xph}(\tau)\).
Correlator \(\chi^{(3)}_{ph}(i\omega)\) (particle-hole channel) in Matsubara frequencies.
Correlator \(\chi^{(3)}_{ph}(i\omega)\) (particle-hole channel), obtained from the NFFT \(M^{(3)}\) measurement.
Correlator \(\chi^{(3)}_{pp}(i\omega)\) (particle-particle channel) in Matsubara frequencies.
Correlator \(\chi^{(3)}_{pp}(i\omega)\) (particle-particle channel), obtained from the NFFT \(M^{(3)}\) measurement.
Correlator \(\chi^{(3)}_{xph}(i\omega)\) (particle-hole-cross channel) in Matsubara frequencies.
Correlation function \(\chi_{AB}(i\omega)\) in Matsubara frequencies.
Correlation function \(\chi_{AB}(\tau)\) in imaginary time.
Parameters used to construct the solver.
The density (measured by operator insertion).
Perturbation-order distribution.
Parameters used in the last solve (empty until the solver has been run).
Total number of measurements.
Warmup time in seconds.
Methods
Retrigger post-processing with the last set of parameters.
Solve the impurity problem with a CT-INT calculation.