DMFT
This page gives hints on how to perform a DMFT calculation with the ABINIT package.
Introduction¶
DFT fails to describe the ground state and/or the excited states such as many lanthanides, actinides or transition metals. Indeed, exchange correlation functionals are not (yet) able to describe the strong repulsive Coulomb interactions occurring among electrons in partly filled localized d or f orbitals.
A way to improve the description of strongly correlated systems is to explicitly include the strong repulsive Coulomb interactions in the Hamiltonian. Solving it in the static mean field approximation, gives the DFT+U method ([Anisimov1991], [Liechtenstein1995]), implemented in ABINIT [Amadon2008a]. The Dynamical Mean Field Theory [Georges1996] (DMFT), goes beyond, by solving exactly the local correlations for an atom in an effective field (i.e., an Anderson model). The effective field reproduces the effect of the surrounding correlated atoms and is thus selfconsistently related to the solution of the Anderson model [Georges1996].
The combination of DFT with DMFT [Georges2004], [Kotliar2006] (usedmft= 1) relies on:

The definition of correlated orbitals. In ABINIT, we use Wannier functions built using projected local orbitals [Amadon2008]. Wannier functions are unitarily related to a selected set of Kohn Sham (KS) wavefunctions, specified in ABINIT by band indices dmftbandi and dmftbandf. As empty bands are necessary to build Wannier functions, it is required in DMFT calculations that the KS Hamiltonian is correctly diagonalized: use high values for nnsclo and nline. In order to make a first rough estimation of the orbital character of KS bands and choose the band index, the band structure with highlighted atomic orbital character (so called fatbands ) can be plotted, using the pawfatbnd variable. Band structures obtained from projected orbitals Wannier functions can also be plotted using plowan_compute and related variables.

The choice of the screened Coulomb interaction U (upawu) and J (jpawu). Note that up to version 7.10.5 (but not in later versions) jpawu= 0 is required if the density matrix in the correlated subspace is not diagonal.

The choice of the double counting correction [Amadon2012]. The current default choice in ABINIT is dmft_dc= 1 which corresponds to the full localized limit.

The method of resolution of the Anderson model. In ABINIT, it can be the Hubbard I method [Amadon2012] (dmft_solv= 2), the Continuous time Quantum Monte Carlo (CTQMC) method [Gull2011],[Bieder2014] (dmft_solv= 5) or the static mean field method (dmft_solv= 1), equivalent to usual DFT+U [Amadon2012]).
The practical solution of the DFT+DMFT scheme is usually presented as a double loop over, first, the local Green’s function, and second the electronic local density [Amadon2012]. The number of iterations of the two loops are determined by dmft_iter and nstep. However, in the general case, the most efficient way to carry out fully consistent DFT+DMFT calculations is to keep only the loop governed by nstep, while dmft_iter=1 [Bieder2014], dmft_rslf= 1 (to read the selfenergy file at each step of the DFT loop) and prtden= 1 (to be able to restart the calculation of each step of the DFT loop from the density file). Lastly, one linear and one logarithmic grid are used for Matsubara frequencies [Kotliar2006] determined by dmft_nwli and dmft_nwlo (Typical values are 10000 and 100, but convergence should be studied). More information can be obtained in the log file by setting pawprtvol=3.
The main output of the calculations are the imaginary time Green’s function , from which spectral functions can be obtained using an external maximum entropy code [Bergeron2016], selfenergies, from which quasiparticle renormalization weight can be extracted, the density matrix of correlated orbitals, and the internal energies [Amadon2006]. The electronic entropic contribution to the free energy can also be obtained using dmft_entropy and dmft_nlambda.
The efficient CTQMC code in ABINIT, which is the most time consuming part of DMFT, uses the hybridization expansion [Werner2006], [Gull2011] with a densitydensity multiorbital interaction [Gull2011]. Moreover, the hybridization function [Gull2011] is assumed to be diagonal in the orbital (or flavor) index. This is exact for cubic symmetry without spin orbit coupling but, in general, one should always check that the offdiagonal terms are much smaller than the diagonal ones. A link to the exact rotationally invariant interaction CTQMC code of the TRIQS library is also available using dmft_solv=7.
As the CTQMC solver uses a Fourier transform, the time grid dmftqmc_l in imaginary space must be chosen so that the Nyquist frequency, defined by πdmftqmc_l tsmear, is around 2 or 3 Ha. A convergence study should be performed on this variable. Moreover, the number of imaginary frequencies (dmft_nwlo) has to be set to at least twice the value of dmftqmc_l. Typical numbers of steps for the thermalization (dmftqmc_therm) and for the Monte carlo runs (dmftqmc_n) are 106 and 109 respectively. The random number generator can be initialized with the variable dmftqmc_seed. Several other variables are available. dmftctqmc_order gives a histogram of the perturbation orders during the simulation, dmftctqmc_gmove customizes the global move tries (mainly useful for systems with high/low spin configurations), and dmftctqmc_meas sets the frequency of measurement of quantities.
Related Input Variables¶
compulsory:
 dmft_iter Dynamical Mean Field Theory: number of ITERation
 dmft_nwli Dynamical Mean Field Theory: Number of frequency omega (W) in the LInear mesh
 dmft_nwlo Dynamical Mean Field Theory: Number of frequency omega (W) in the LOg mesh
 dmftbandf Dynamical Mean Field Theory: BAND: Final
 dmftbandi Dynamical Mean Field Theory: BAND: Initial
 dmftqmc_l Dynamical Mean Field Theory: Quantum Monte Carlo time sLices
 dmftqmc_n Dynamical Mean Field Theory: Quantum Monte Carlo Number of sweeps
 dmftqmc_therm Dynamical Mean Field Theory: Quantum Monte Carlo THERMalization
 usedmft USE Dynamical Mean Field Theory
basic:
 dmft_rslf Dynamical Mean Field Theory: Read SeLF energy
 dmft_solv Dynamical Mean Field Theory: choice of SOLVer
useful:
 dmft_dc Dynamical Mean Field Theory: Double Counting
 dmft_mxsf Dynamical Mean Field Theory: MiXing parameter for the SelF energy
 dmft_tollc Dynamical Mean Field Theory: TOLerance on Local Charge for convergence of the DMFT loop
 dmftcheck Dynamical Mean Field Theory: CHECKs
 dmftctqmc_check Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo CHECK
 dmftctqmc_gmove Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo Global MOVEs
 dmftctqmc_order Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo perturbation ORDER
 dmftqmc_seed Dynamical Mean Field Theory: Quantum Monte Carlo SEED
expert:
 dmft_entropy Dynamical Mean Field Theory: ENTROPY
 dmft_nlambda Dynamical Mean Field Theory: Number of LAMBDA points
 dmft_read_occnd Dynamical Mean Field Theory: READ OCCupations (Non Diagonal)
 dmft_t2g Dynamical Mean Field Theory: t2g orbitals
 dmft_tolfreq Dynamical Mean Field Theory: TOLerance on DFT correlated electron occupation matrix for the definition of the FREQuency grid
 dmftctqmc_basis Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo BASIS
 dmftctqmc_correl Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo CORRELations
 dmftctqmc_grnns Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo GReeNs NoiSe
 dmftctqmc_meas Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo MEASurements
 dmftctqmc_mov Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo MOVie
 dmftctqmc_mrka Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo MARKov Analysis
 dmftctqmc_triqs_nleg Dynamical Mean Field Theory: Continuous Time Quantum Monte Carlo perturbation of TRIQS, Number of LEGendre polynomials
Selected Input Files¶
paral:
v6:
v7:
Tutorials¶
 The tutorial on DFT+DMFT shows how to perform a DFT+DMFT calculation on SrVO3 using projected Wannier functions. Prerequisite: DFT+U.