solver         =  'CTQMC'   # impurity solver
DCs            =  'nominal' # double counting scheme

max_dmft_iterations = 1     # number of iteration of the dmft-loop only
max_lda_iterations  = 100   # number of iteration of the LDA-loop only
finish              =  30   # number of iterations of full charge loop (1 = no charge self-consistency)

ntail          =  300       # on imaginary axis, number of points in the tail of the logarithmic mesh

cc             =  2e-4      # the charge density precision to stop the LDA+DMFT run
ec             =  2e-4      # the energy precision to stop the LDA+DMFT run

recomputeEF    =  0         # Recompute EF in dmft2 step.

# Impurity problem number 0
iparams0={"exe"                : ["ctqmc"              , "# Name of the executable"],
          "U"                  : [8.0                  , "# Coulomb repulsion (F0)"],
          "J"                  : [0.8                  , "# Coulomb repulsion (F0)"],
          "beta"               : [50                   , "# Inverse temperature"],
	  "CoulombF"           : ["'Ising'"            , "# Form of Coulomb repulsion"],
          "svd_lmax"           : [25                   , "# We will use SVD basis to expand G, with this cutoff"],
          "M"                  : [10e6                 , "# Total number of Monte Carlo steps"],
          "mode"               : ["SH"                 , "# We will use self-energy sampling, and Hubbard I tail"],
          "nom"                : [200                  , "# Number of Matsubara frequency points sampled"],
          "tsample"            : [200                  , "# How often to record measurements"],
          "GlobalFlip"         : [1000000              , "# How often to try a global flip"],
          "warmup"             : [1e6                  , "# Warmup number of QMC steps"],
          "nf0"                : [2                    , "# Double counting parameter"],
}