Configuration interaction based nonequilibrium steady state impurity solver
Beschreibung
This directory tree contains the dataset for the publication included here (publication.pdf):
D. Werner, J. Lotze and E. Arrigoni, "Configuration interaction based nonequilibrium steady state impurity solver", Phys. Rev. B 107, 075119 (2023). DOI: 10.1103/PhysRevB.107.075119
The paper introduces a configuration interaction (CI) impurity solver, and its complete-active-space extension (CASCI), within the auxiliary master equation approach (AMEA). AMEA maps the single-impurity Anderson model (impurity with Hubbard interaction U, coupled to two leads) onto an auxiliary open quantum system: an impurity coupled to a finite number of bath sites that are, in turn, coupled to Markovian environments described by a Lindblad equation. The physical hybridization function of the impurity, Delta_phys, is reproduced by fitting the parameters of this auxiliary bath (its on-site energies / hoppings E and its dissipative Lindblad matrices Gamma^(1), Gamma^(2)); the mapping becomes exponentially accurate with the number of bath sites N_B. CI/CASCI allow more bath sites than plain exact diagonalization (ED) at lower cost. The dataset benchmarks CI/CASCI against ED, matrix product states (MPS), and the numerical renormalization group (NRG), and computes the equilibrium and nonequilibrium conductance and the Kondo-peak splitting of the Anderson model.
Units: unless noted otherwise, all energies (U, T, V, omega, ...) are given in units of Gamma, defined by -Im(Delta_phys^R(w=0)) = Gamma. The leads have a flat band of half-bandwidth D = 10*Gamma, smoothed with a fictitious temperature T_fict = 0.5*Gamma. The impurity is particle-hole symmetric (on-site energy eps_imp = -U/2). The bias voltage V (also called phi in the paper) enters as the difference of the two lead chemical potentials, mu_R = V/2 = -mu_L.
Note on file formats: the "example.txt" template refers to a JSON-per-simulation layout used for a different dataset. In THIS dataset the results are instead stored as column-based text files (.csv / .dat), described in detail below, together with the input hybridization functions and the fitted auxiliary-bath parameters needed to reproduce them. Auxiliary material (Python evaluation/plotting scripts, HPC job scripts and stdout logs) is also included; see the last section.
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Naming conventions used throughout
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Green's function / self-energy result files are named, e.g.:
GF_data_real_sites_9_U_4.0_nup_0.3_intend_0_method_CI_inputdata_gam-t0.05v1.dat_.csv
"sites_<n>" -> total number of sites of the auxiliary system = 1 impurity + N_B bath sites (so "sites_7" = N_B = 6, "sites_9" = N_B = 8, "sites_11" = N_B = 10, "sites_17" = N_B = 16)
"U_<x>" -> Hubbard interaction U on the impurity
"nup_<x>" -> m_up = <n_f,up>, the (spin-up) impurity occupation used as a free mean-field/Hartree-Fock parameter of the CI reference state; range [0, 0.5], with 0.5 being half filling (see Sec. III A and Eq. (28) of the paper)
"method_<CI|CASCI>" -> impurity solver used (CI or its complete-active-space extension CASCI)
"intend_<n>" -> internal run index/label (0 in all files here)
"inputdata_gam-t<T>v<V>" -> identifies the input hybridization function used for this run: T is the physical temperature and V the bias voltage of the leads (see next item)
The auxiliary input/parameter files are named "gam-t<T>v<V>" / "hybr-t<T>v<V>":
"t<T>" -> physical temperature T of the leads
"v<V>" -> bias voltage V (= phi) applied across the leads; v0.0 is equilibrium
"-auxN<n>" -> where present, marks a quantity belonging to the fitted auxiliary bath with n total sites (as opposed to the physical target)
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File formats
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CI / CASCI results ("GF_data_real_..._.csv"):
Semicolon (";") separated, no header, 9 columns, one row per frequency:
col 1: omega (frequency grid, units of Gamma)
col 2: Re G^K (= 0) (real part of Keldysh Green's function; zero by construction)
col 3: Im G^K (imaginary part of Keldysh Green's function)
col 4: Re G^R (real part of retarded Green's function)
col 5: Im G^R (imaginary part of retarded Green's function; -pi*Im G^R is the spectral function)
col 6: Re Sigma^K (= 0) (real part of Keldysh self-energy; zero by construction)
col 7: Im Sigma^K (imaginary part of Keldysh self-energy)
col 8: Re Sigma^R (real part of retarded self-energy)
col 9: Im Sigma^R (imaginary part of retarded self-energy)
(i.e. each file contains both the impurity Green's function and self-energy.)
ED reference results (files "Aux_GF.dat" and "Sigma.dat" inside the ED folders):
Space separated, one comment header line, 5 columns:
"%omega real-ret imag-ret real-kel imag-kel"
col 1: omega
col 2: Re (retarded) [G^R for Aux_GF.dat, Sigma^R for Sigma.dat]
col 3: Im (retarded)
col 4: Re (Keldysh) (= 0 by construction)
col 5: Im (Keldysh)
"Aux_GF.dat" is the impurity Green's function of the auxiliary system, "Sigma.dat" the corresponding self-energy. Alongside them:
"MB_out__MBlog_N_E_Gamma.dat" -> the parameters of the auxiliary (Lindblad) many-body system for that run: first the dimension N, then the real matrix E (unitary part: on-site energies and hoppings of Eq. (12)), followed by the two complex matrices Gamma^(1) and Gamma^(2) (the dissipative Lindblad coupling matrices of Eq. (11)); entries "(re,im)".
"MB_out__MBlog_Krylov.dat" -> solver (Krylov/Lanczos) log for that run.
MPS reference results (files "MPS_data_T<T>_GR.json" and "..._SR.json"):
JSON. A list of series objects, each with an "x" array (frequency grid) and the corresponding function values. "GR" holds the retarded Green's function G^R, "SR" the retarded self-energy Sigma^R.
Physical / auxiliary hybridization functions (files "hybr-t<T>v<V>[...]" under hybridization_function/.../hybfunc/):
Space separated, one comment header line, 3 columns:
"% omega imag-ret imag-keld"
col 1: omega
col 2: Im Delta^R (imaginary part of the retarded hybridization function)
col 3: Im Delta^K (imaginary part of the Keldysh hybridization function)
Files without a suffix are the physical hybridization Delta_phys; files with "-auxN<n>" are the hybridization of the fitted auxiliary bath with n sites (cf. Eq. (14) and the cost function Eq. (17)).
Fitted auxiliary-bath parameter files (files "gam-t<T>v<V>[_<n>_sites].dat" under hybridization_function/.../gammas/):
The fitted auxiliary-system (Lindblad) parameters (E and Gamma matrices, same content as "MB_out__MBlog_N_E_Gamma.dat" above) that are fed to the CI/CASCI/ED solver as the "inputdata gam-..." referenced by the result-file names. These are the quantities needed to reproduce the solver runs.
Conductance vs temperature, NRG reference (files under conductance_eq/cond_NRG_.../cond_U_<U>_high_acc_long):
Semicolon separated, 2 columns:
col 1: temperature T
col 2: linear conductance G (equilibrium, V = 0)
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Directory structure (mapped to the paper)
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"comparison_with_ED" -> benchmark of CI against numerically exact ED for the Anderson impurity model, for N_B = 6 (7 sites), U = 6, T = 0.05, as a function of the mean-field parameter m_up ("nup") and of the bias voltage V. This underlies the method-parameter analysis (choice of m_up) and the CI-vs-ED accuracy of the paper.
"GFs_n_up_sweep_CI/" -> CI results (the ".csv" files described above), one per (nup, V).
"GFs_n_up_sweep_ED/" -> ED "exact" results, organized in one subfolder per input hybridization ("gam-t0.05v0.0", "gam-t0.05v0.333", ...), each containing Aux_GF.dat, Sigma.dat and the MB_out__* auxiliary-system parameter/log files.
"hybridization_function/sites_7/" -> the inputs and fit for N_B = 6: "hybfunc/" (physical and fitted auxiliary hybridization functions), "gammas/" (fitted auxiliary-bath parameter files), "output/" (HPC stdout logs of the fitting sweep), plus a small helper script.
"evluation_scripts/" -> Python script (evalute_sweep.py) that reads the CI and ED files and computes/plots the error (note: folder name is spelled "evluation").
"comparison_with_MPS" -> benchmark of the impurity Green's function / self-energy across three solvers at U = 6, T = 0.05:
"ED_GFs_7_sites_U_6_T_0.05/" -> ED result (N_B = 6).
"CI_GFs_9_sites_U_6_T_0.05/" -> CI result (N_B = 8).
"MPS_GFs_17_sites_U_6_T_0.05/" -> MPS reference (N_B = 16), as the two JSON files (GR, SR).
"hybridization_function/" -> corresponding input hybridization and fitted bath parameters.
"evaluation_scripts/" -> plotting/analysis scripts.
"conductance_eq" -> equilibrium (V = 0) linear conductance as a function of temperature, for U = 4, 6, 8, used to demonstrate the T/T_K scaling collapse. The temperature is swept via the many "gam-t<T>v0.0" input hybridizations.
"ED_GFs_7_sites_V_0_U_4_6_8/" -> ED conductance data (N_B = 6).
"CI_GFs_9_sites_V_0_U_4_6_8/" -> CI conductance data (N_B = 8).
"CI_GFs_11_sites_V_0_U_4_6_8/" -> CI conductance data (N_B = 10).
"cond_NRG_V_0_U_4_6_8/" -> NRG reference conductance vs temperature (cond_U_4.0/6.0/8.0_high_acc_long; two-column T ; G files).
"hybridization_function/", "evalutation_scripts/" -> inputs and analysis scripts (folder name spelled "evalutation").
"conductance_non_eq" -> nonequilibrium conductance and Kondo-peak splitting as a function of bias voltage, at fixed Kondo temperature T_K = 0.25 (U = 4, CASCI, N_B = 8 / 9 sites). The bias voltage V ("v...") is swept, at fixed temperature (t0.12).
"CI_GFs_TK_0.25_9_sites/" -> the CASCI Green's function / self-energy ".csv" files, one per bias voltage.
"hybridization_function/", "evalutation_scripts/" -> inputs and analysis scripts.
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Auxiliary (non-data) files
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For completeness and reproducibility the tree also contains:
"*.py" -> Python evaluation / plotting scripts (and "*.pyc" their compiled bytecode caches; these can be ignored).
"*.out", "*.out-<n>", "*.pbs" -> stdout logs and submit scripts of the HPC (PBS) batch jobs that produced the fits/sweeps; kept as a provenance record and not needed to use the data.
The primary scientific data are the ".csv" (CI/CASCI), ".dat" (ED, hybridization, NRG conductance) and ".json" (MPS) files described in the "File formats" section above. The fitted auxiliary-bath parameter files ("gammas/gam-*.dat", "MB_out__MBlog_N_E_Gamma.dat") together with the physical hybridization functions provide the full input needed to regenerate the solver results.
This research was funded in part by the Austrian Science Fund (FWF) [Grant DOI:10.55776/P33165]
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- Publikation: 10.1103/PhysRevB.107.075119 (DOI)