nohup: ignoring input mkdir: cannot create directory `n.1': File exists mkdir: cannot create directory `n.2': File exists mkdir: cannot create directory `n.3': File exists mkdir: cannot create directory `n.4': File exists mkdir: cannot create directory `n.5': File exists mkdir: cannot create directory `n.6': File exists mkdir: cannot create directory `n.7': File exists mkdir: cannot create directory `n.8': File exists mkdir: cannot create directory `n.9': File exists mkdir: cannot create directory `n.10': File exists -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.1 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.2 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.3 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.4 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.5 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.6 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.7 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.8 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.9 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range -b0 0.5 # Frequency mesh parameter -nom 200 # number of matsubara points used -p0 0.1 # how fast should the low energy function fall off -b 0.9 # b parameter to determin family of basis functions -alpha4 1.0 # weight for the low energy expansion in the functional to be minimized -alpha3 0.01 # weight for the normalization in functional to be minimized -ifit 4 # number of Matsubara points used to fit the lowe energy expansion -beta 40 # inverse temperature -rps 1 # The lowest lorentzian is usualy at pi*T. This factor can bring it closer to zero. -Ng 60 # number of basis functions -lcut 0.0 # the lowest frequency lorentzian position -a0 0.005 # Frequency mesh start -FermiLiquid True # Low energy expansion of a Fermi liquid of Mott insulator -sig Sig.10 # input self-energy on imaginary axis -L0 20 # High energy cut-off for plotting -Iwidth 0.01 # Width of the pole for the insulator -N0 400 # Number of frequency points for plotting -poles [] # additional poles -vunity 0.01 # value of low-energy function at unity -wexp 1.15 # wexp^i is position where basis functions are peaked Traceback (most recent call last): File "./ancont.py", line 539, in sinfty = sqmc0[-1][0] IndexError: list index out of range