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https://github.com/triqs/dft_tools
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for earlier commits, see TRIQS0.x repository.
180 lines
7.3 KiB
Python
180 lines
7.3 KiB
Python
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################################################################################
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#
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# TRIQS: a Toolbox for Research in Interacting Quantum Systems
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#
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# Copyright (C) 2011 by M. Ferrero, O. Parcollet
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#
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# TRIQS is free software: you can redistribute it and/or modify it under the
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# terms of the GNU General Public License as published by the Free Software
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# Foundation, either version 3 of the License, or (at your option) any later
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# version.
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#
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# TRIQS is distributed in the hope that it will be useful, but WITHOUT ANY
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# WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS
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# FOR A PARTICULAR PURPOSE. See the GNU General Public License for more
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# details.
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#
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# You should have received a copy of the GNU General Public License along with
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# TRIQS. If not, see <http://www.gnu.org/licenses/>.
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#
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################################################################################
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from pytriqs.gf.local import *
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import types, string, inspect, itertools
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from operator import isSequenceType
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from pytriqs.dos import DOS, DOSFromFunction
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import pytriqs.utility.mpi as mpi
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import numpy
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class HilbertTransform :
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r"""
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Computes the Hilbert Transform from a DOS object
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.. math::
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\int_{-\infty}^\infty d \epsilon \rho(\epsilon) \Bigl( (\omega + \mu +
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I\eta)\mathbf{1} - \hat\varepsilon(\epsilon) - \text{field} - \Sigma(\epsilon)
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\Bigr)^{-1}
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"""
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def __init__(self, rho):
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"""
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:param rho: a DOS object.
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"""
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self.dos = rho
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assert isinstance(rho, DOS), "See Doc. rho must be a DOS"
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self.__normalize()
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#-------------------------------------------------------------
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def __reduce__(self) :
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return self.__class__, (self.rho)
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#-------------------------------------------------------------
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def __normalize(self):
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# normalisation. dos is not the value of the function, is the weight of the integrals
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R = numpy.array(self.dos.rho, copy=True)
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self.rho_for_sum = R
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eps = self.dos.eps
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R[0] *= (eps[1] - eps[0])
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R[-1] *= (eps[-1] - eps[-2])
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for i in xrange(1, eps.shape[0] - 1) :
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R[i] *= (eps[i+1] - eps[i])/2+(eps[i] - eps[i-1])/2
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R /= numpy.sum(R)
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#-------------------------------------------------------------
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def __call__ (self, Sigma, mu=0, eta=0, field=None, epsilon_hat=None, result=None,
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n_points_integral=None, test_convergence=None):
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r"""
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Compute the Hilbert Transform
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Parameters
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-----------
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mu : float
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eta : float
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Sigma : a GFBloc or a function epsilon-> GFBloc
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field : anything that can added to the GFBloc Sigma, e.g. :
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* an Array_with_GFBloc_Indices (same size as Sigma)
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* a GBloc
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epsilon_hat : a function that takes a 1d array eps[i] and returns 3d-array eps[i, :, :]
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where the :, : has the matrix structure of Sigma. Default : eps[i] * Identity_Matrix
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Used only when DOS is a DOSFromFunction :
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n_points_integral : How many points to use. If None, use the Npts of construction
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test_convergence : If defined, it will refine the grid until CV is reached
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starting from n_points_integral and multiplying by 2
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Returns
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--------
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Returns the result. If provided, use result to compute the result locally.
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"""
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# we suppose here that self.eps, self.rho_for_sum such that
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# H(z) = \sum_i self.rho_for_sum[i] * (z- self.eps[i])^-1
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# Check Sigma and result
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assert Sigma.N1==Sigma.N2, "Sigma must be square"
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if result :
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assert result.N1 == Sigma.N1 and result.N2 == Sigma.N2, "Size of result and Sigma mismatch"
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else :
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result = Sigma.copy()
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if not( isinstance (self.dos, DOSFromFunction)):
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assert n_points_integral==None and test_convergence == None, " Those parameters can only be used with an dos_from_function"
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if field !=None :
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try :
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result += field
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except :
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assert 0, "field can not be added to the Green function blocks !. Cf Doc"
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def HT(res) :
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# First compute the eps_hat array
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eps_hat = epsilon_hat(self.dos.eps) if epsilon_hat else numpy.array( [ x* numpy.identity (Sigma.N1) for x in self.dos.eps] )
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assert eps_hat.shape[0] == self.dos.eps.shape[0], "epsilon_hat function behaves incorrectly"
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assert eps_hat.shape[1] == eps_hat.shape[2], "epsilon_hat function behaves incorrectly (result not a square matrix)"
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assert Sigma.N1 == eps_hat.shape[1], "Size of Sigma and of epsilon_hat mismatch"
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res.zero()
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Sigma_fnt = callable(Sigma)
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if Sigma_fnt : assert len(inspect.getargspec(Sigma)[0]) ==1, "Sigma function is not of the correct type. See Documentation"
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# Perform the sum over eps[i]
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tmp, tmp2 = res.copy(), res.copy()
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tmp <<= iOmega_n + mu + eta * 1j
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if not(Sigma_fnt) :
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tmp -= Sigma
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if field != None : tmp -= field
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# I slice all the arrays on the node. Cf reduce operation below.
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for d, e_h, e in itertools.izip (*[mpi.slice_array(A) for A in [self.rho_for_sum, eps_hat, self.dos.eps]]):
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tmp2.copy_from(tmp)
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tmp2 -= e_h
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if Sigma_fnt : tmp2 -= Sigma(e)
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tmp2.invert()
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tmp2 *= d
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res += tmp2
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# sum the res GF of all nodes and returns the results on all nodes...
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# Cf Boost.mpi.python, collective communicator for documentation.
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# The point is that res is pickable, hence can be transmitted between nodes without further code...
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res <<= mpi.all_reduce(mpi.world, res, lambda x, y : x+y)
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mpi.barrier()
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# END of HT
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def test_distance(G1, G2, dist) :
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def f(G1, G2) :
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dS = max(abs(G1.data - G2.data).flatten())
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aS = max(abs(G1.data).flatten())
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return dS <= aS*dist
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#return reduce(lambda x, y : x and y, [f(g1, g2) for (i1, g1), (i2, g2) in izip(G1, G2)])
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return f(G1, G2) # for block function, the previous one is for GF functions
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if isinstance (self.dos, DOSFromFunction):
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if not(n_points_integral) : # if not defined, use the defaults given at construction of the dos
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n_points_integral= len(self.dos.eps)
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else:
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self.dos._DOS__f(n_points_integral)
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self.__normalize()
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HT(result)
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nloop, test = 1, 0
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while test_convergence and nloop < 10 and (nloop == 1 or test > test_convergence):
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if nloop>1 :
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self.dos._DOS__f(n_points_integral)
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self.__normalize()
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result_old = result.copy()
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result = DOS.HilbertTransform(self, Sigma, mu, eta, epsilon_hat, result)
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test = test_distance(result, result_old, test_convergence)
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n_points_integral *=2
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else : # Ordinary DOS
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HT(result)
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return result
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