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Extension of the iterated perturbation theory at arbitrary fillings to nonequilibrium steady states
Phys. Rev. B 114, 175122 – Published 16 September, 2026
DOI: https://doi.org/10.1103/lwg4-6tq8
Abstract
We extend the Kajueter-Kotliar [Phys. Rev. Lett. 77, 131 (1996)] iterated perturbation theory (KK-IPT) away from half-filling to nonequilibrium steady states. We benchmark the resulting nonequilibrium KK-IPT approach against the auxiliary master equation approach (AMEA), whose accuracy is controlled in and out of equilibrium. As expected, in equilibrium, KK-IPT reproduces the AMEA results for different fillings with high accuracy at the level of both spectral properties and electron densities. Out of equilibrium, we study quantum transport across a correlated impurity and compute the differential conductance and spectral functions. We find very good agreement between nonequilibrium KK-IPT and AMEA in the parameter regime where the latter is reliable, in particular at moderate temperatures and biases. Although a controlled benchmark is not available in the low-temperature, low-bias regime, where AMEA becomes less reliable, we show that this nonequilibrium KK-IPT impurity solver satisfies the exact spectral sum rules for the first and second moments to high accuracy throughout the entire parameter range studied. These results support nonequilibrium KK-IPT as an approximate description of nonequilibrium steady states away from half-filling. At the same time, comparing against AMEA the double occupancy obtained from the nonequilibrium Galitskii-Migdal expression for the interaction energy shows that the deviation from AMEA remains small near half-filling for moderate and large values of the bias, but grows markedly away from half-filling, delineating the regime in which the method can be trusted quantitatively rather than merely qualitatively.
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References (56)
- A. Georges and G. Kotliar, Hubbard model in infinite dimensions, Phys. Rev. B 45, 6479 (1992).
- A. Georges, G. Kotliar, W. Krauth, and M. J. Rozenberg, Dynamical mean-field theory of strongly correlated fermion systems and the limit of infinite dimensions, Rev. Mod. Phys. 68, 13 (1996).
- H. Aoki, N. Tsuji, M. Eckstein, M. Kollar, T. Oka, and P. Werner, Nonequilibrium dynamical mean-field theory and its applications, Rev. Mod. Phys. 86, 779 (2014).
- E. Gull, A. J. Millis, A. I. Lichtenstein, A. N. Rubtsov, M. Troyer, and P. Werner, Continuous-time Monte Carlo methods for quantum impurity models, Rev. Mod. Phys. 83, 349 (2011).
- P. Werner, A. Comanac, L. de' Medici, M. Troyer, and A. J. Millis, Continuous-time solver for quantum impurity models, Phys. Rev. Lett. 97, 076405 (2006).
- K. G. Wilson, The renormalization group: Critical phenomena and the Kondo problem, Rev. Mod. Phys. 47, 773 (1975).
- R. Bulla, T. A. Costi, and T. Pruschke, Numerical renormalization group method for quantum impurity systems, Rev. Mod. Phys. 80, 395 (2008).
- M. Caffarel and W. Krauth, Exact diagonalization approach to correlated fermions in infinite dimensions: Mott transition and superconductivity, Phys. Rev. Lett. 72, 1545 (1994).
- H. Keiter and J. C. Kimball, Perturbation technique for the Anderson Hamiltonian, Phys. Rev. Lett. 25, 672 (1970).
- M. Eckstein and P. Werner, Nonequilibrium dynamical mean-field calculations based on the noncrossing approximation and its generalizations, Phys. Rev. B 82, 115115 (2010).
- A. Dorda, M. Nuss, W. von der Linden, and E. Arrigoni, Auxiliary master equation approach to non–equilibrium correlated impurities, Phys. Rev. B 89, 165105 (2014).
- D. Werner, J. Lotze, and E. Arrigoni, Configuration interaction based nonequilibrium steady state impurity solver, Phys. Rev. B 107, 075119 (2023).
- T. M. Mazzocchi, P. Gazzaneo, J. Lotze, and E. Arrigoni, Correlated Mott insulators in strong electric fields: Role of phonons in heat dissipation, Phys. Rev. B 106, 125123 (2022).
- P. Gazzaneo, T. M. Mazzocchi, J. Lotze, and E. Arrigoni, Impact ionization processes in a photodriven Mott insulator: Influence of phononic dissipation, Phys. Rev. B 106, 195140 (2022).
- T. M. Mazzocchi, D. Werner, P. Gazzaneo, and E. Arrigoni, Correlated Mott insulators in a strong electric field: The effects of phonon renormalization, Phys. Rev. B 107, 155103 (2023).
- T. M. Mazzocchi, D. Werner, M. Aichhorn, and E. Arrigoni, Mixed-configuration approximation for multiorbital systems out of equilibrium, Phys. Rev. B 112, 155127 (2025).
- G. Cohen, E. Gull, D. R. Reichman, and A. J. Millis, Taming the dynamical sign problem in real-time evolution of quantum many-body problems, Phys. Rev. Lett. 115, 266802 (2015).
- A. E. Antipov, Q. Dong, J. Kleinhenz, G. Cohen, and E. Gull, Currents and Green's functions of impurities out of equilibrium: Results from inchworm quantum Monte Carlo, Phys. Rev. B 95, 085144 (2017).
- A. Erpenbeck, E. Gull, and G. Cohen, Quantum Monte Carlo method in the steady state, Phys. Rev. Lett. 130, 186301 (2023).
- A. Erpenbeck, T. Blommel, L. Zhang, W.-T. Lin, G. Cohen, and E. Gull, Steady-state properties of multi-orbital systems using quantum Monte Carlo, J. Chem. Phys. 161, 094104 (2024).
- F. B. Anders, Steady-state currents through nanodevices: A scattering-states numerical renormalization-group approach to open quantum systems, Phys. Rev. Lett. 101, 066804 (2008).
- J. E. Han, Nonequilibrium statistics of a biased Kondo resonance, Phys. Rev. B 113, 045141 (2026).
- Y. N. Fernández, M. Jeannin, P. T. Dumitrescu, T. Kloss, J. Kaye, O. Parcollet, and X. Waintal, Learning Feynman diagrams with tensor trains, Phys. Rev. X 12, 041018 (2022).
- A. J. Kim and P. Werner, Strong coupling impurity solver based on quantics tensor cross interpolation, Phys. Rev. B 111, 125120 (2025).
- A. Georges and W. Krauth, Physical properties of the half-filled Hubbard model in infinite dimensions, Phys. Rev. B 48, 7167 (1993).
- H. Kajueter and G. Kotliar, New iterative perturbation scheme for lattice models with arbitrary filling, Phys. Rev. Lett. 77, 131 (1996).
- W.-R. Lee and K. Park, Dielectric breakdown via emergent nonequilibrium steady states of the electric-field-driven Mott insulator, Phys. Rev. B 89, 205126 (2014).
- A. Martin-Rodero, F. Flores, M. Baldo, and R. Pucci, A new solution to the Anderson-Newns Hamiltonian of chemisorption, Solid State Commun. 44, 911 (1982).
- A. Martín-Rodero, E. Louis, F. Flores, and C. Tejedor, Interpolative solution for the periodic Anderson model of mixed-valence compounds, Phys. Rev. B 33, 1814 (1986).
- M. Potthoff, T. Wegner, and W. Nolting, Interpolating self-energy of the infinite-dimensional Hubbard model: Modifying the iterative perturbation theory, Phys. Rev. B 55, 16132 (1997).
- L.-F. Arsenault, P. Sémon, and A.-M. S. Tremblay, Benchmark of a modified iterated perturbation theory approach on the fcc lattice at strong coupling, Phys. Rev. B 86, 085133 (2012).
- N. Dasari, W. R. Mondal, P. Zhang, J. Moreno, M. Jarrell, and N. S. Vidhyadhiraja, A multi-orbital iterated perturbation theory for model Hamiltonians and real material-specific calculations of correlated systems, Eur. Phys. J. B 89, 202 (2016).
- E. G. C. P. van Loon, Two-particle correlations and the metal-insulator transition: Iterated perturbation theory revisited, Phys. Rev. B 105, 245104 (2022).
- N. Tsuji and P. Werner, Nonequilibrium dynamical mean-field theory based on weak-coupling perturbation expansions: Application to dynamical symmetry breaking in the Hubbard model, Phys. Rev. B 88, 165115 (2013).
- J. Schwinger, Brownian motion of a quantum oscillator, J. Math. Phys. 2, 407 (1961).
- L. V. Keldysh, Diagram technique for nonequilibrium processes, Zh. Eksp. Theor. Fiz. 47, 1515 (1964) [Sov. Phys. JETP 20, 1018 (1965)].
- H. Haug and A.-P. Jauho, Quantum Kinetics in Transport and Optics of Semiconductors (Springer, Heidelberg, 1998).
- Throughout this work the onsite energy is chosen to be spin independent.
- M. Potthoff, T. Herrmann, T. Wegner, and W. Nolting, The moment sum rule and its consequences for ferromagnetism in the Hubbard model, Phys. Status Solidi B 210, 199 (1998).
- T. M. Mazzocchi and E. Arrigoni, Iterated perturbation theory for Mott insulators in a static electric field with optical phonons, Phys. Status Solidi B 261, 2300486 (2024).
- We note that, out of equilibrium, the Friedel sum rule discussed in previous work [26, 32] does not apply, and its proper generalization remains unclear. Nonetheless, benchmark comparisons with the AMEA impurity solver indicate that the IPT- approximation performs satisfactorily in all cases considered so far.
- Each impurity solver run discussed in this work was initialized from the same fixed cold-start initial guess () with no continuation or warm starting between neighboring bias points: each point is an independent root-finding problem for . All runs converged to a unique, physical solution (, finite and at every frequency), with no case of multiple attracting fixed points, not even when the initial guess was changed for a few selected data points (not shown), or unphysical output anywhere in this work. This is consistent with the robust convergence already reported for the equilibrium KK-IPT scheme in Ref. [26]. However, we did find instances of nonconvergence when the initial guess for was too close to either 0 or 1.
- For details on the AMEA impurity solver, we refer the reader to our previous work [11, 12].
- R. Bulla, A. C. Hewson, and T. Pruschke, Numerical renormalization group calculations for the self-energy of the impurity Anderson model, J. Phys.: Condens. Matter 10, 8365 (1998).
- Y. Meir and N. S. Wingreen, Landauer formula for the current through an interacting electron region, Phys. Rev. Lett. 68, 2512 (1992).
- We point out that the retarded and Keldysh components of the impurity GF as well as the Keldysh component of the lead GF retain a nontrivial dependence on and . However, for our choice of leads, neither of these parameters enters the retarded (advanced) reservoir GF.
- The precise range of validity depends on both and ; see the shaded regions in Fig. 3. At , AMEA is reliable down to , essentially independently of temperature (cf. also Ref. [12], Fig. 6 therein, which suggests that the conductance obtained by numerical derivative, and thus error amplifying, is accurate for at intermediate ). At , the reliable range extends down to at low temperature () and at high temperature (). At , it extends down to at low temperature and at high temperature. In short, the bias threshold below which AMEA becomes unreliable grows sharply with , while temperature plays a secondary role that only becomes significant once .
- T. M. Mazzocchi, Extension of the iterated perturbation theory at arbitrary fillings to nonequilibrium steady states [Dataset], Graz University of Technology, 2026, https://doi.org/10.3217/xz6v9-9jp08.
- https://github.com/mazzocch/neq-kk-ipt-solver.
- G. Stefanucci and R. van Leeuwen, Nonequilibrium Many-body Theory of Quantum Systems: A Modern Introduction (Cambridge University Press, Cambridge, 2013).
- D. N. Zubarev, Double-time Green functions in statistical physics, Sov. Phys.–Usp. 3, 320 (1960).
- A. B. Harris and R. V. Lange, Single-particle excitations in narrow energy bands, Phys. Rev. 157, 295 (1967).
- W. Nolting, Methode der Spektralmomente für das Hubbard-Modell eines schmalen-Bandes, Z. Phys. 255, 25 (1972).
- J. J. Deisz, D. W. Hess, and J. W. Serene, Vertex symmetry and the asymptotic frequency dependence of the self-energy, Phys. Rev. B 55, 2089 (1997).
- X. Wang, H. T. Dang, and A. J. Millis, High-frequency asymptotic behavior of self-energies in quantum impurity models, Phys. Rev. B 84, 073104 (2011).
- V. Turkowski and J. K. Freericks, Nonequilibrium sum rules for the retarded self-energy of strongly correlated electrons, Phys. Rev. B 77, 205102 (2008).