Container for all (optional) quantities measured and post-processed by the solver.
Definition at line 13 of file container_set.hpp.
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double | accumulation_time |
| | Accumulation time in seconds.
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double | auto_corr_time |
| | Auto-correlation time.
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double | average_k |
| | Average perturbation order.
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std::optional< double > | average_k_error |
| | Error bar on the average perturbation order.
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mc_weight_t | average_sign |
| | Average Monte-Carlo sign.
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std::optional< double > | average_sign_error |
| | Error bar on the average sign.
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std::optional< chi2_tau_t > | chi2ph_conn_tau_from_M3 |
| | Connected \( \chi^{(2)} \) (particle-hole channel) in imaginary time, obtained from \( M^{(3)} \).
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std::optional< chi2_iw_t > | chi2ph_iw |
| | Correlator \( \chi^{(2)}_{ph}(i\omega) \) (particle-hole channel) in Matsubara frequencies.
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std::optional< chi2_iw_t > | chi2ph_iw_from_M3 |
| | Correlator \( \chi^{(2)}_{ph}(i\omega) \) (particle-hole channel), obtained from \( M^{(3)}_{ph}(\tau) \).
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std::optional< chi2_tau_t > | chi2ph_tau |
| | Correlator \( \chi^{(2)}_{ph}(\tau) \) (particle-hole channel) in imaginary time, obtained by operator insertion.
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std::optional< chi2_tau_t > | chi2ph_tau_from_M3 |
| | Correlator \( \chi^{(2)}_{ph}(\tau) \) (particle-hole channel), obtained from \( M^{(3)}_{ph}(\tau) \).
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std::optional< chi2_tau_t > | chi2pp_conn_tau_from_M3 |
| | Connected \( \chi^{(2)} \) (particle-particle channel) in imaginary time, obtained from \( M^{(3)} \).
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std::optional< chi2_iw_t > | chi2pp_iw |
| | Correlator \( \chi^{(2)}_{pp}(i\omega) \) (particle-particle channel) in Matsubara frequencies.
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std::optional< chi2_iw_t > | chi2pp_iw_from_M3 |
| | Correlator \( \chi^{(2)}_{pp}(i\omega) \) (particle-particle channel), obtained from \( M^{(3)}_{pp}(\tau) \).
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std::optional< chi2_tau_t > | chi2pp_tau |
| | Correlator \( \chi^{(2)}_{pp}(\tau) \) (particle-particle channel) in imaginary time, obtained by operator insertion.
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std::optional< chi2_tau_t > | chi2pp_tau_from_M3 |
| | Correlator \( \chi^{(2)}_{pp}(\tau) \) (particle-particle channel), obtained from \( M^{(3)}_{pp}(\tau) \).
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std::optional< chi2_tau_t > | chi2xph_conn_tau_from_M3 |
| | Connected \( \chi^{(2)} \) (particle-hole-cross channel) in imaginary time, obtained from \( M^{(3)} \).
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std::optional< chi2_iw_t > | chi2xph_iw_from_M3 |
| | Correlator \( \chi^{(2)}_{xph}(i\omega) \) (particle-hole-cross channel), obtained from \( M^{(3)}_{xph}(\tau) \).
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std::optional< chi2_tau_t > | chi2xph_tau_from_M3 |
| | Correlator \( \chi^{(2)}_{xph}(\tau) \) (particle-hole-cross channel), obtained from \( M^{(3)}_{xph}(\tau) \).
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std::optional< chi3_iw_t > | chi3ph_iw |
| | Correlator \( \chi^{(3)}_{ph}(i\omega) \) (particle-hole channel) in Matsubara frequencies.
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std::optional< chi3_iw_t > | chi3ph_iw_nfft |
| | Correlator \( \chi^{(3)}_{ph}(i\omega) \) (particle-hole channel), obtained from the NFFT \( M^{(3)} \) measurement.
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std::optional< chi3_iw_t > | chi3pp_iw |
| | Correlator \( \chi^{(3)}_{pp}(i\omega) \) (particle-particle channel) in Matsubara frequencies.
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std::optional< chi3_iw_t > | chi3pp_iw_nfft |
| | Correlator \( \chi^{(3)}_{pp}(i\omega) \) (particle-particle channel), obtained from the NFFT \( M^{(3)} \) measurement.
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std::optional< chi3_iw_t > | chi3xph_iw |
| | Correlator \( \chi^{(3)}_{xph}(i\omega) \) (particle-hole-cross channel) in Matsubara frequencies.
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std::optional< gf< imfreq > > | chiAB_iw |
| | Correlation function \( \chi_{AB}(i\omega) \) in Matsubara frequencies.
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std::optional< gf< imtime > > | chiAB_tau |
| | Correlation function \( \chi_{AB}(\tau) \) in imaginary time.
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std::optional< block_matrix_t > | density |
| | The density (measured by operator insertion).
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std::optional< chi4_iw_t > | F_iw |
| | The two-particle vertex function \( F \) in purely fermionic notation.
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std::optional< chi4_iw_t > | Fph_iw |
| | The two-particle vertex function \( F \) (particle-hole channel).
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std::optional< chi4_iw_t > | Fpp_iw |
| | The two-particle vertex function \( F \) (particle-particle channel).
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std::optional< chi4_iw_t > | G2_conn_iw |
| | Connected part of the two-particle Green's function \( G^{(2)} \).
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std::optional< chi4_iw_t > | G2_iw |
| | The two-particle Green's function \( G^{(2)} \).
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std::optional< chi4_iw_t > | G2ph_conn_iw |
| | Connected part of the two-particle Green's function \( G^{(2)} \) (particle-hole channel).
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std::optional< chi4_iw_t > | G2ph_iw |
| | The two-particle Green's function \( G^{(2)} \) (particle-hole channel).
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std::optional< chi4_iw_t > | G2pp_conn_iw |
| | Connected part of the two-particle Green's function \( G^{(2)} \) (particle-particle channel).
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std::optional< chi4_iw_t > | G2pp_iw |
| | The two-particle Green's function \( G^{(2)} \) (particle-particle channel).
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g_iw_t | G_iw |
| | Green's function \( G(i\omega) \) in Matsubara frequencies.
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std::optional< std::vector< double > > | histogram |
| | Perturbation-order distribution.
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std::optional< chi2_tau_t > | M3ph_delta |
| | Equal-time peak of \( M^{(3)}_{ph}(\tau) \).
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std::optional< chi3_iw_t > | M3ph_iw |
| | Building block \( M^{(3)}_{ph}(i\omega) \) (particle-hole channel) for the fermion-boson vertex in Matsubara frequencies.
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std::optional< chi3_iw_t > | M3ph_iw_nfft |
| | Building block \( M^{(3)}_{ph}(i\omega) \) (particle-hole channel) for the fermion-boson vertex, measured using NFFT.
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std::optional< chi3_tau_t > | M3ph_tau |
| | Building block \( M^{(3)}_{ph}(\tau) \) (particle-hole channel) for the fermion-boson vertex in imaginary time.
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std::optional< chi2_tau_t > | M3pp_delta |
| | Equal-time peak of \( M^{(3)}_{pp}(\tau) \).
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std::optional< chi3_iw_t > | M3pp_iw |
| | Building block \( M^{(3)}_{pp}(i\omega) \) (particle-particle channel) for the fermion-boson vertex in Matsubara frequencies.
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std::optional< chi3_iw_t > | M3pp_iw_nfft |
| | Building block \( M^{(3)}_{pp}(i\omega) \) (particle-particle channel) for the fermion-boson vertex, measured using NFFT.
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std::optional< chi3_tau_t > | M3pp_tau |
| | Building block \( M^{(3)}_{pp}(\tau) \) (particle-particle channel) for the fermion-boson vertex in imaginary time.
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std::optional< chi2_tau_t > | M3xph_delta |
| | Equal-time peak of \( M^{(3)}_{xph}(\tau) \).
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std::optional< chi3_iw_t > | M3xph_iw |
| | Building block \( M^{(3)}_{xph}(i\omega) \) (particle-hole-cross channel) for the fermion-boson vertex in Matsubara frequencies.
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std::optional< chi3_tau_t > | M3xph_tau |
| | Building block \( M^{(3)}_{xph}(\tau) \) (particle-hole-cross channel) for the fermion-boson vertex in imaginary time.
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std::optional< chi4_iw_t > | M4_iw |
| | Building block \( M^{(4)}(i\omega) \) for the full vertex, measured in Matsubara frequencies using NFFT.
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std::optional< chi4_iw_t > | M4ph_iw |
| | Building block \( M^{(4)}_{ph}(i\omega) \) (particle-hole channel) for the full vertex, measured using NFFT.
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std::optional< chi4_iw_t > | M4pp_iw |
| | Building block \( M^{(4)}_{pp}(i\omega) \) (particle-particle channel) for the full vertex, measured using NFFT.
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std::optional< block_matrix_t > | M_hartree |
| | Hartree term of \( M(\tau) \).
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std::optional< g_iw_t > | M_iw |
| | Fourier transform of \( M(\tau) \).
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std::optional< g_dlr_iw_t > | M_iw_nfft |
| | Same as \( M(\tau) \), but measured directly in Matsubara frequencies using NFFT on the DLR grid.
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std::optional< block_gf< imtime, M_tau_target_t > > | M_tau |
| | Building block for the Green's function in imaginary time \( M(\tau) \).
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uint64_t | nmeasures |
| | Total number of measurements.
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g_iw_t | Sigma_dyn_iw |
| | Dynamic self-energy \( \Sigma_{dyn}(i\omega) \) in Matsubara frequencies (DLR, decays to zero).
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std::optional< block_matrix_t > | Sigma_hartree |
| | Static (Hartree) part of the self-energy, \( \Sigma = \Sigma_{dyn} + \Sigma_{hartree} \).
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double | warmup_time |
| | Warmup time in seconds.
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