# 
# ALPS Project: Algorithms and Libraries for Physics Simulations
# 
# ALPS Libraries
# 
# Copyright (C) 2010      by Brigitte Surer <surerb@phys.ethz.ch> 
#               2012-2013 by Jakub Imriska  <jimriska@phys.ethz.ch>
# 
# This software is part of the ALPS libraries, published under the ALPS
# Library License; you can use, redistribute it and/or modify it under
# the terms of the license, either version 1 or (at your option) any later
# version.
#  
# You should have received a copy of the ALPS Library License along with
# the ALPS Libraries; see the file LICENSE.txt. If not, the license is also
# available from http://alps.comp-phys.org/.
# 
# THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR 
# IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY, 
# FITNESS FOR A PARTICULAR PURPOSE, TITLE AND NON-INFRINGEMENT. IN NO EVENT 
# SHALL THE COPYRIGHT HOLDERS OR ANYONE DISTRIBUTING THE SOFTWARE BE LIABLE 
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# DEALINGS IN THE SOFTWARE.
# 
# ****************************************************************************

import pyalps
import numpy as np
import matplotlib.pyplot as plt
import pyalps.plot


#prepare the input parameters
parms=[]
for u in [4.,5.,6.,8.]: 
    parms.append(
            { 
              'ANTIFERROMAGNET'         : 0,
              'CONVERGED'               : 0.001,
              'FLAVORS'                 : 2,
              'H'                       : 0,
              'H_INIT'                  : 0.,
              'MAX_IT'                  : 20,
              'MAX_TIME'                : 600,
              'MU'                      : 0,
              'N'                       : 500,
              'NMATSUBARA'              : 500, 
              'N_MEAS'                  : 1000,
              'N_HISTOGRAM_ORDERS'                 : 50,
              'OMEGA_LOOP'              : 1,
              'SEED'                    : 0, 
              'SITES'                   : 1,              
              'SOLVER'                  : 'hybridization',
              'SC_WRITE_DELTA'          : 1,
              'SYMMETRIZATION'          : 1,
              't'                       : 1,
              'SWEEPS'                  : 1500*u,
              'BETA'                    : 20.0,
              'THERMALIZATION'          : 500,
              'U'                       : u
            }
        )
     
# For more precise calculations change the parameters
#   enlarge SWEEPS,
#   CONVERGED (to 0.0002-0.001),
#   raise N and NMATSUBARA (to 1000)

#write the input file and run the simulation
for p in parms:
    input_file = pyalps.writeParameterFile('parm_u_'+str(p['U']),p)
    res = pyalps.runDMFT(input_file)

listobs=['0']   # we look at only one flavor, as they are SYMMETRIZED
    
data = pyalps.loadMeasurements(pyalps.getResultFiles(pattern='parm_u_*h5'), respath='/simulation/results/G_tau', what=listobs, verbose=True)

for d in pyalps.flatten(data):
    d.x = d.x*d.props["BETA"]/float(d.props["N"])
    d.y = -d.y
    d.props['label'] = r'$U=$'+str(d.props['U'])
plt.figure()
plt.yscale('log')
plt.xlabel(r'$\tau$')
plt.ylabel(r'$G_{flavor=0}(\tau)$')
plt.title('DMFT-04: Mott-insulator transition for the Hubbard model on the Bethe lattice')
pyalps.plot.plot(data)
plt.legend()
plt.show()