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dft_tools/pytriqs/gf/local/descriptors.py

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################################################################################
#
# TRIQS: a Toolbox for Research in Interacting Quantum Systems
#
# Copyright (C) 2011 by M. Ferrero, O. Parcollet
#
# TRIQS is free software: you can redistribute it and/or modify it under the
# terms of the GNU General Public License as published by the Free Software
# Foundation, either version 3 of the License, or (at your option) any later
# version.
#
# TRIQS is distributed in the hope that it will be useful, but WITHOUT ANY
# WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS
# FOR A PARTICULAR PURPOSE. See the GNU General Public License for more
# details.
#
# You should have received a copy of the GNU General Public License along with
# TRIQS. If not, see <http://www.gnu.org/licenses/>.
#
################################################################################
r""" """
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from descriptor_base import *
from gf import MeshImFreq, MeshReFreq
#######################################
class OneFermionInTime(Base):
def __init__ (self, l =0):
Base.__init__(self, L=l)
def __call__(self,G):
L = self.L
if G.mesh.TypeGF not in [GF_Type.Imaginary_Time]:
raise TypeError, "This initializer is only correct in frequency"
Id = numpy.identity(G.N1)
G.tail.zero()
G.tail[1][:,:] = 1*Id
G.tail[2][:,:] = L*Id
G.tail[3][:,:] = L*L*Id
G.tail.mask.fill(3)
fact = -1/(1+exp(-L*G.beta))
Function(lambda t: fact* exp(-L*t) *Id, None)(G)
return G
##################################################
def _SemiCircularDOS(half_bandwidth):
"""
Semi_Circular DOS function
Input: the 1/2 bandwidth
Returns: a function omega-> dos(omega)
"""
from math import sqrt,pi
larg = half_bandwidth
def semi(x):
if (abs(x)<larg): return sqrt( 1 - (x/larg)**2 )*2/pi/larg
else: return 0.0
return semi
def semi(x):
return _SemiCircularDOS(x)
##################################################
class SemiCircular (Base):
r"""Hilbert transform of a semicircular density of states, i.e.
.. math::
g(z) = \int \frac{A(\omega)}{z-\omega} d\omega
where :math:`A(\omega) = \theta( D - |\omega|) 2 \sqrt{ D^2 - \omega^2}/(\pi D^2)`.
(Only works in combination with frequency Green's functions.)
"""
def __init__ (self, half_bandwidth):
""":param half_bandwidth: :math:`D`, the half bandwidth of the
semicircular density of states"""
Base.__init__(self, half_bandwidth=half_bandwidth)
def __str__(self): return "SemiCircular(%s)"%self.half_bandwidth
def __call__(self,G):
D= self.half_bandwidth
Id = numpy.identity(G.N1,numpy.complex_)
if type(G.mesh) == MeshImFreq:
f = lambda om: (om - 1j*copysign(1,om.imag)*sqrt(abs(om)**2 + D*D))/D/D*2*Id
elif type(G.mesh) == MeshReFreq:
def f(om_):
om = om_.real
if (om > -D) and (om < D):
return (2.0/D**2) * (om - 1j* sqrt(D**2 - om**2))
else:
return (2.0/D**2) * (om - copysign(1,om) * sqrt(om**2 - D**2))
else:
raise TypeError, "This initializer is only correct in frequency"
# Let's create a new tail
Id = numpy.identity(G.N1)
G.tail.zero()
G.tail[1][:,:] = 1.0*Id
G.tail[3][:,:] = D**2/4.0*Id
G.tail[5][:,:] = D**4/8.0*Id
G.tail.mask.fill(6)
Function(f,None)(G)
return G
##################################################
class Wilson (Base):
r"""The Hilbert transform of a flat density of states, with cut-off
.. math::
g(z) = \int \frac{A(\omega)}{z-\omega} d\omega
where :math:`A(\omega) = \theta( D^2 - \omega^2)/(2D)`.
(Only works in combination with frequency Green's functions.)
"""
def __init__ (self, half_bandwidth):
""":param half_bandwidth: :math:`D`, the half bandwidth """
Base.__init__(self, half_bandwidth=half_bandwidth)
def __str__(self): return "Wilson(%s)"%half_bandwidth
def __call__(self,G):
D = self.half_bandwidth
Id = numpy.identity(G.N1,numpy.complex_)
if type(G.mesh) == MeshImFreq:
f = lambda om: (-1/(2.0*D)) * numpy.log((om-D)/(om+D)) * Id
elif type(G.mesh) == MeshReFreq:
def f(om):
if (om.real > -D) and (om.real < D):
return -numpy.log(abs(om-D)/abs(om+D))*Id/(2*D) - 1j*pi*Id/(2*D)
else:
return -numpy.log(abs(om-D)/abs(om+D))*Id/(2*D)
else:
raise TypeError, "This initializer is only correct in frequency"
# Let's create a new tail
Id = numpy.identity(G.N1)
G.tail.zero()
G.tail[1][:,:] = 1.0*Id
G.tail[3][:,:] = D**2/3.0*Id
G.tail[5][:,:] = D**4/5.0*Id
G.tail.mask.fill(6)
Function(f,None)(G)
return G
##################################################
class Fourier (Base):
r"""
The Fourier transform as a lazy expression
"""
def __init__ (self, G):
""":param G: :math:`G`, the function to be transformed. Must in the time domain"""
Base.__init__(self, G = G)
def __str__(self): return "Fourier(%s)"%self.G.name
def __call__(self,G2):
G2.set_from_fourier(self.G)
return G2
class InverseFourier (Base):
r"""
The Inverse Fourier transform as a lazy expression
"""
def __init__ (self, G):
""":param G: :math:`G`, the function to be transformed. Must in the frequency domain"""
Base.__init__(self, G = G)
def __str__(self): return "InverseFourier(%s)"%self.G.name
def __call__(self,G2):
G2.set_from_inverse_fourier(self.G)
return G2
class LegendreToMatsubara (Base):
r"""
The transformation from Legendre to Matsubara as a lazy expression
"""
def __init__ (self, G):
""":param G: :math:`G`, the function to be transformed. Must in the Legendre domain"""
Base.__init__(self, G = G)
def __str__(self): return "LegendreToMatsubara(%s)"%self.G.name
def __call__(self,G2):
G2.set_from_legendre(self.G)
return G2
class MatsubaraToLegendre (Base):
r"""
The transformation from Legendre to Matsubara as a lazy expression
"""
def __init__ (self, G):
""":param G: :math:`G`, the function to be transformed. Must in the Matsubara domain"""
Base.__init__(self, G = G)
def __str__(self): return "MatsubaraToLegendre(%s)"%self.G.name
def __call__(self,G2):
G2.set_from_imfreq(self.G)
return G2