triqs_ctint.solver_core.SolverCore
- class triqs_ctint.solver_core.SolverCore
The Solver class
- Attributes:
D0_iw
Dynamic density-density interaction in Matsubara frequencies
F_iw
The two-particle vertex function in purely fermionic notation (iw1, iw2, iw3)
Fph_iw
The two-particle vertex function in the ph channel
Fpp_iw
The two-particle vertex function in the pp channel
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
G2ph_iw
The two-particle Green function (ph channel)
G2phc_iw
The connected part of the two-particle Green function (ph channel)
G2pp_iw
The two-particle Green function (pp channel)
G2ppc_iw
The connected part of the two-particle Green function (pp channel)
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
M3xph_delta
Equal-time peak in M3ph_tau
M3xph_iw
Building block for the fermion boson vertex (xph channel) in Matsubara frequencies
M3xph_tau
Building block for the fermion boson vertex (xph channel) in imaginary time
M4_iw
Building block for the full vertex function measured directly in Matsubara frequencies using NFFT
M4ph_iw
Building block for the full vertex function (ph channel) measured directly in Matsubara frequencies using NFFT
M4pp_iw
Building block for the full vertex function (pp channel) 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
chi2xph_conn_tau_from_M3
M2 in the particle-hole-cross channel in imaginary time as obtained from M3
chi2xph_iw_from_M3
The equal time correlator $chi_2$ in the particle-hole-cross channel in imaginary frequencies as obtained from M3ph_tau
chi2xph_tau_from_M3
The equal time correlator $chi_2$ in the particle-hole-cross channel in imaginary times as obtained from M3ph_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
chi3xph_iw
The equal time correlator $chi_3$ in the particle-hole-cross channel in Matsubara frequencies
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
Methods
Signature : () -> str
Signature : () -> None
Solve method that performs CTINT calculation
Methods
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Signature : () -> str |
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Signature : () -> None |
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Solve method that performs CTINT calculation |
Attributes
Dynamic density-density interaction in Matsubara frequencies |
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The two-particle vertex function in purely fermionic notation (iw1, iw2, iw3) |
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The two-particle vertex function in the ph channel |
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The two-particle vertex function in the pp channel |
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Noninteracting Green Function in Matsubara frequencies |
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The shifted noninteracting Green Function in Matsubara frequencies |
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The shifted noninteracting Green Function in imaginary time |
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The two-particle Green function |
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The connected part of the two-particle Green function |
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The two-particle Green function (ph channel) |
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The connected part of the two-particle Green function (ph channel) |
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The two-particle Green function (pp channel) |
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The connected part of the two-particle Green function (pp channel) |
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Greens function in Matsubara frequencies (Eq. |
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Dynamic spin-spin interaction in Matsubara frequencies |
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Equal-time peak in M3ph_tau |
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Building block for the fermion boson vertex (ph channel) in Matsubara frequencies |
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Building block for the fermion boson vertex (ph channel) in Matsubara frequencies using NFFT |
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Building block for the fermion boson vertex (ph channel) in imaginary time |
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Equal-time peak in M3pp_tau |
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Building block for the fermion boson vertex (pp channel) in Matsubara frequencies |
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Building block for the fermion boson vertex (pp channel) in Matsubara frequencies using NFFT |
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Building block for the fermion boson vertex (pp channel) in imaginary time |
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Equal-time peak in M3ph_tau |
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Building block for the fermion boson vertex (xph channel) in Matsubara frequencies |
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Building block for the fermion boson vertex (xph channel) in imaginary time |
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Building block for the full vertex function measured directly in Matsubara frequencies using NFFT |
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Building block for the full vertex function (ph channel) measured directly in Matsubara frequencies using NFFT |
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Building block for the full vertex function (pp channel) measured directly in Matsubara frequencies using NFFT |
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Hartree-term of M_tau |
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The Fourier-transform of M_tau. |
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Same as M_tau, but measured directly in Matsubara frequencies using NFFT |
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Building block for the Green function in imaginary time (Eq. |
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Self-energy in Matsubara frequencies. |
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Auto-correlation time |
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Average perturbation order |
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Average sign of the CTINT |
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M2 in the particle-hole channel in imaginary time as obtained from M3 |
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The equal time correlator $chi_2$ in the particle-hole channel in Matsubara frequencies |
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The equal time correlator $chi_2$ in the particle-hole channel in imaginary frequencies as obtained from M3ph_tau |
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The equal time correlator $chi_2$ in the particle-hole channel in imaginary times as obtained by operator insertion |
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The equal time correlator $chi_2$ in the particle-hole channel in imaginary times as obtained from M3ph_tau |
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M2 in the particle-particle channel in imaginary time as obtained from M3 |
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The equal time correlator $chi_2$ in the particle-particle channel in Matsubara frequencies |
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The equal time correlator $chi_2$ in the particle-particle channel in imaginary frequencies as obtained from M3pp_tau |
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The equal time correlator $chi_2$ in the particle-particle channel in imaginary times as obtained by operator insertion |
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The equal time correlator $chi_2$ in the particle-particle channel in imaginary times as obtained from M3pp_tau |
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M2 in the particle-hole-cross channel in imaginary time as obtained from M3 |
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The equal time correlator $chi_2$ in the particle-hole-cross channel in imaginary frequencies as obtained from M3ph_tau |
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The equal time correlator $chi_2$ in the particle-hole-cross channel in imaginary times as obtained from M3ph_tau |
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The equal time correlator $chi_3$ in the particle-hole channel in Matsubara frequencies |
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The equal time correlator $chi_3$ in the particle-hole channel in Matsubara frequencies as obtained by the NFFT $M_3$ measurement |
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The equal time correlator $chi_3$ in the particle-particle channel in Matsubara frequencies |
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The equal time correlator $chi_3$ in the particle-particle channel in Matsubara frequencies as obtained by the NFFT $M_3$ measurement |
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The equal time correlator $chi_3$ in the particle-hole-cross channel in Matsubara frequencies |
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The correlation function $chi_AB$ in imaginary frequencies |
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The correlation function $chi_AB$ in imaginary times |
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The density matrix (measured by operator insertion) |
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Average perturbation order distribution |
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