[py3] Run port_to_triqs3 script

cmake/sitecustomize.py

@@ -1,8 +1,8 @@
-def application_pytriqs_import(name,*args,**kwargs):
+def application_triqs_import(name,*args,**kwargs):
   if name.startswith('@package_name@'):
     name = name[len('@package_name@')+1:]
   return builtin_import(name,*args,**kwargs)
 
 import builtins
-builtins.__import__, builtin_import = application_pytriqs_import, builtins.__import__
+builtins.__import__, builtin_import = application_triqs_import, builtins.__import__
 

doc/guide/analysis.rst

@@ -37,7 +37,7 @@ class::
 Note that all routines available in :class:`SumkDFT <dft.sumk_dft.SumkDFT>` are also available here.
 
 If required, we have to load and initialise the real-frequency self energy. Most conveniently,
-you have your self energy already stored as a real-frequency :class:`BlockGf <pytriqs.gf.BlockGf>` object
+you have your self energy already stored as a real-frequency :class:`BlockGf <triqs.gf.BlockGf>` object
 in a hdf5 file::
 
   with HDFArchive('case.h5', 'r') as ar:
@@ -45,10 +45,10 @@ in a hdf5 file::
 
 You may also have your self energy stored in text files. For this case the :ref:`TRIQS <triqslibs:welcome>` library offers
 the function :meth:`read_gf_from_txt`, which is able to load the data from text files of one Green function block
-into a real-frequency :class:`ReFreqGf <pytriqs.gf.ReFreqGf>` object. Loading each block separately and
+into a real-frequency :class:`ReFreqGf <triqs.gf.ReFreqGf>` object. Loading each block separately and
-building up a :class:´BlockGf <pytriqs.gf.BlockGf>´ is done with::
+building up a :class:´BlockGf <triqs.gf.BlockGf>´ is done with::
 
-  from pytriqs.gf.tools import *
+  from triqs.gf.tools import *
   # get block names
   n_list = [n for n,nl in SK.gf_struct_solver[0].iteritems()]
   # load sigma for each block - in this example sigma is composed of 1x1 blocks

doc/guide/dftdmft_singleshot.rst

@@ -80,8 +80,8 @@ for :emphasis:`use_dc_formula` are:
 
 At the end of the calculation, we can save the Green function and self energy into a file::
 
-    from pytriqs.archive import HDFArchive
+    from h5 import HDFArchive
-    import pytriqs.utility.mpi as mpi
+    import triqs.utility.mpi as mpi
     if mpi.is_master_node():
         ar = HDFArchive("YourDFTDMFTcalculation.h5",'w')
         ar["G"] = S.G_iw

doc/tutorials/ce-gamma-fscs_wien2k.rst

@@ -96,7 +96,7 @@ In order to run DFT+DMFT calculations within Hubbard-I we need the corresponding
 with the CT-QMC solver (see :ref:`singleshot`), however there are also some differences. First
 difference is that we import the Hubbard-I solver by::
 
-   from pytriqs.applications.impurity_solvers.hubbard_I.hubbard_solver import Solver
+   from triqs.applications.impurity_solvers.hubbard_I.hubbard_solver import Solver
 
 The Hubbard-I solver is very fast and we do not need to take into account the DFT block structure
 or use any approximation for the *U*-matrix. We load and convert the :program:`dmftproj` output

doc/tutorials/images_scripts/Ce-gamma.py

@@ -1,6 +1,6 @@
 from triqs_dft_tools.sumk_dft import *
 from triqs_dft_tools.converters.wien2k_converter import *
-from pytriqs.applications.impurity_solvers.hubbard_I.hubbard_solver import Solver
+from triqs.applications.impurity_solvers.hubbard_I.hubbard_solver import Solver
 
 import os
 dft_filename = os.getcwd().rpartition('/')[2]

doc/tutorials/images_scripts/Ce-gamma_DOS.py

@@ -1,6 +1,6 @@
 from triqs_dft_tools.sumk_dft_tools import *
 from triqs_dft_tools.converters.wien2k_converter import *
-from pytriqs.applications.impurity_solvers.hubbard_I.hubbard_solver import Solver
+from triqs.applications.impurity_solvers.hubbard_I.hubbard_solver import Solver
 
 # Creates the data directory, cd into it:
 #Prepare_Run_Directory(DirectoryName = "Ce-Gamma") 

doc/tutorials/images_scripts/NiO_local_lattice_GF.py

@@ -1,12 +1,12 @@
 from itertools import *
 import numpy as np
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 from h5 import *
-from pytriqs.gf import *
+from triqs.gf import *
 from triqs_dft_tools.sumk_dft import *
 from triqs_dft_tools.sumk_dft_tools import *
-from pytriqs.operators.util.hamiltonians import *
+from triqs.operators.util.hamiltonians import *
-from pytriqs.operators.util.U_matrix import *
+from triqs.operators.util.U_matrix import *
 from triqs_cthyb import *
 import warnings
 warnings.filterwarnings("ignore", category=FutureWarning)

doc/tutorials/images_scripts/dft_dmft_cthyb.py

@@ -1,8 +1,8 @@
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
-from pytriqs.operators.util import *
+from triqs.operators.util import *
 from h5 import HDFArchive
 from triqs_cthyb import *
-from pytriqs.gf import *
+from triqs.gf import *
 from triqs_dft_tools.sumk_dft import *
 from triqs_dft_tools.converters.wien2k_converter import *
 

doc/tutorials/images_scripts/maxent.py

@@ -1,4 +1,4 @@
-from pytriqs.gf import *
+from triqs.gf import *
 from h5 import *
 from triqs_maxent import *
 
@@ -43,7 +43,7 @@ for orb in orbs:
 
 
     # you may be interested in the details of the line analyzer:
-    # from pytriqs.plot.mpl_interface import oplot
+    # from triqs.plot.mpl_interface import oplot
     #plt.figure(2)
     #result.analyzer_results['LineFitAnalyzer'].plot_linefit()
     #plt.savefig('ana'+str(orb[0])+'.pdf',fmt='pdf')

doc/tutorials/images_scripts/nio.py

@@ -1,13 +1,13 @@
 from itertools import *
 import numpy as np
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 from h5 import *
-from pytriqs.gf import *
+from triqs.gf import *
-import sys, pytriqs.version as triqs_version
+import sys, triqs.version as triqs_version
 from triqs_dft_tools.sumk_dft import *
 from triqs_dft_tools.sumk_dft_tools import *
-from pytriqs.operators.util.hamiltonians import *
+from triqs.operators.util.hamiltonians import *
-from pytriqs.operators.util.U_matrix import *
+from triqs.operators.util.U_matrix import *
 from triqs_cthyb import *
 import triqs_cthyb.version as cthyb_version
 import triqs_dft_tools.version as dft_tools_version

doc/tutorials/images_scripts/nio_csc.py

@@ -1,13 +1,13 @@
 from itertools import *
 import numpy as np
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 from h5 import *
-from pytriqs.gf import *
+from triqs.gf import *
-import sys, pytriqs.version as triqs_version
+import sys, triqs.version as triqs_version
 from triqs_dft_tools.sumk_dft import *
 from triqs_dft_tools.sumk_dft_tools import *
-from pytriqs.operators.util.hamiltonians import *
+from triqs.operators.util.hamiltonians import *
-from pytriqs.operators.util.U_matrix import *
+from triqs.operators.util.U_matrix import *
 from triqs_cthyb import *
 import triqs_cthyb.version as cthyb_version
 import triqs_dft_tools.version as dft_tools_version

doc/tutorials/srvo3.rst

@@ -77,11 +77,11 @@ Loading modules
 First, we load the necessary modules::
 
   from triqs_dft_tools.sumk_dft import *
-  from pytriqs.gf import *
+  from triqs.gf import *
-  from pytriqs.archive import HDFArchive
+  from h5 import HDFArchive
-  from pytriqs.operators.util import *
+  from triqs.operators.util import *
   from triqs_cthyb import *
-  import pytriqs.utility.mpi as mpi
+  import triqs.utility.mpi as mpi
 
 The last two lines load the modules for the construction of the
 :ref:`CTHYB solver <triqscthyb:welcome>`.
@@ -271,7 +271,7 @@ and perform only one DMFT iteration. The resulting self energy can be tail fitte
     Sigma_iw_fit << tail_fit(S.Sigma_iw, fit_max_moment = 4, fit_min_n = 40, fit_max_n = 160)[0]
 
 Plot the self energy and adjust the tail fit parameters such that you obtain a
-proper fit. The :meth:`fit_tail function <pytriqs.gf.tools.tail_fit>` is part
+proper fit. The :meth:`fit_tail function <triqs.gf.tools.tail_fit>` is part
 of the :ref:`TRIQS <triqslibs:welcome>` library.
 
 For a self energy which is going to zero for :math:`i\omega \rightarrow 0` our suggestion is

python/block_structure.py

@@ -1,8 +1,8 @@
 import copy
 import numpy as np
-from pytriqs.gf import GfImFreq, BlockGf
+from triqs.gf import GfImFreq, BlockGf
 from ast import literal_eval
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 from warnings import warn
 
 class BlockStructure(object):

python/converters/converter_tools.py

@@ -19,7 +19,7 @@
 # TRIQS. If not, see <http://www.gnu.org/licenses/>.
 #
 ##########################################################################
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 
 class ConverterTools:
 

python/converters/hk_converter.py

@@ -23,7 +23,7 @@
 from types import *
 import numpy
 from h5 import *
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 from math import sqrt
 from .converter_tools import *
 

python/converters/plovasp/sc_dmft.py

@@ -30,7 +30,7 @@ import re
 import time
 import signal
 import sys
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 from . import converter
 from shutil import copyfile
 

python/sumk_dft.py

@@ -22,10 +22,10 @@
 
 from types import *
 import numpy
-import pytriqs.utility.dichotomy as dichotomy
+import triqs.utility.dichotomy as dichotomy
-from pytriqs.gf import *
+from triqs.gf import *
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
-from pytriqs.utility.comparison_tests import assert_arrays_are_close
+from triqs.utility.comparison_tests import assert_arrays_are_close
 from h5 import *
 from .symmetry import *
 from .block_structure import BlockStructure
@@ -36,7 +36,7 @@ from scipy.optimize import minimize
 
 
 class SumkDFT(object):
-    """This class provides a general SumK method for combining ab-initio code and pytriqs."""
+    """This class provides a general SumK method for combining ab-initio code and triqs."""
 
     def __init__(self, hdf_file, h_field=0.0, use_dft_blocks=False,
                  dft_data='dft_input', symmcorr_data='dft_symmcorr_input', parproj_data='dft_parproj_input',

python/sumk_dft_tools.py

@@ -21,8 +21,8 @@
 import sys
 from types import *
 import numpy
-from pytriqs.gf import *
+from triqs.gf import *
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 from .symmetry import *
 from .sumk_dft import SumkDFT
 from scipy.integrate import *

python/symmetry.py

@@ -23,9 +23,9 @@
 import copy
 import numpy
 from types import *
-from pytriqs.gf import *
+from triqs.gf import *
 from h5 import *
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 
 
 class Symmetry:

python/trans_basis.py

@@ -1,8 +1,8 @@
 from triqs_dft_tools.sumk_dft import *
 from triqs_dft_tools.converters import Wien2kConverter
-from pytriqs.gf import *
+from triqs.gf import *
 from h5 import *
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 import numpy
 import copy
 

test/analyse_block_structure_from_gf.py

@@ -1,8 +1,8 @@
-from pytriqs.gf import *
+from triqs.gf import *
 from triqs_dft_tools.sumk_dft import SumkDFT
 from scipy.linalg import expm
 import numpy as np
-from pytriqs.utility.comparison_tests import assert_gfs_are_close, assert_arrays_are_close, assert_block_gfs_are_close
+from triqs.utility.comparison_tests import assert_gfs_are_close, assert_arrays_are_close, assert_block_gfs_are_close
 from h5 import *
 import itertools
 

test/analyse_block_structure_from_gf2.py

@@ -1,7 +1,7 @@
-from pytriqs.gf import *
+from triqs.gf import *
 from triqs_dft_tools.sumk_dft import SumkDFT
 import numpy as np
-from pytriqs.utility.comparison_tests import assert_block_gfs_are_close
+from triqs.utility.comparison_tests import assert_block_gfs_are_close
 
 # here we test the SK.analyse_block_structure_from_gf function
 # with GfReFreq, GfReTime

test/blockstructure.py

@@ -1,7 +1,7 @@
 from triqs_dft_tools.sumk_dft import *
-from pytriqs.utility.h5diff import h5diff
+from triqs.utility.h5diff import h5diff
-from pytriqs.gf import *
+from triqs.gf import *
-from pytriqs.utility.comparison_tests import assert_block_gfs_are_close
+from triqs.utility.comparison_tests import assert_block_gfs_are_close
 from triqs_dft_tools.block_structure import BlockStructure
 
 SK = SumkDFT('blockstructure.in.h5',use_dft_blocks=True)

test/hk_convert.py

@@ -22,8 +22,8 @@
 
 
 from h5 import *
-from pytriqs.utility.h5diff import h5diff
+from triqs.utility.h5diff import h5diff
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 
 from triqs_dft_tools.converters import *
 

test/plovasp/converter/mytest.py

@@ -5,7 +5,7 @@ Module defining a custom TestCase with extra functionality.
 import unittest
 import numpy as np
 import difflib
-from pytriqs.utility.h5diff import h5diff
+from triqs.utility.h5diff import h5diff
 
 class MyTestCase(unittest.TestCase):
     """

test/plovasp/proj_group/mytest.py

@@ -5,7 +5,7 @@ Module defining a custom TestCase with extra functionality.
 import unittest
 import numpy as np
 import difflib
-from pytriqs.utility.h5diff import h5diff
+from triqs.utility.h5diff import h5diff
 
 class MyTestCase(unittest.TestCase):
     """

test/sigma_from_file.py

@@ -20,10 +20,10 @@
 ################################################################################
 
 from h5 import *
-from pytriqs.gf import *
+from triqs.gf import *
-from pytriqs.gf.tools import *
+from triqs.gf.tools import *
 from triqs_dft_tools.sumk_dft_tools import *
-from pytriqs.utility.comparison_tests import *
+from triqs.utility.comparison_tests import *
 import numpy as np
 
 # Read self energy from hdf file

test/srvo3_Gloc.py

@@ -20,12 +20,12 @@
 ################################################################################
 
 from h5 import *
-from pytriqs.gf import *
+from triqs.gf import *
 from triqs_dft_tools.sumk_dft import *
 from triqs_dft_tools.converters.wien2k_converter import *
-from pytriqs.operators.util import set_operator_structure
+from triqs.operators.util import set_operator_structure
-from pytriqs.utility.comparison_tests import *
+from triqs.utility.comparison_tests import *
-from pytriqs.utility.h5diff import h5diff
+from triqs.utility.h5diff import h5diff
 
 # Basic input parameters
 beta = 40

test/srvo3_transp.py

@@ -23,8 +23,8 @@ from numpy import *
 from triqs_dft_tools.converters.wien2k_converter import *
 from triqs_dft_tools.sumk_dft import *
 from triqs_dft_tools.sumk_dft_tools import *
-from pytriqs.utility.comparison_tests import *
+from triqs.utility.comparison_tests import *
-from pytriqs.utility.h5diff import h5diff 
+from triqs.utility.h5diff import h5diff 
 
 beta = 40
 

test/sumkdft_basic.py

@@ -22,9 +22,9 @@
 
 from h5 import *
 from triqs_dft_tools.sumk_dft_tools import SumkDFTTools
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
-from pytriqs.utility.comparison_tests import *
+from triqs.utility.comparison_tests import *
-from pytriqs.utility.h5diff import h5diff 
+from triqs.utility.h5diff import h5diff 
 
 SK = SumkDFTTools(hdf_file = 'SrVO3.h5')
 

test/w90_convert.py

@@ -23,8 +23,8 @@
 
 from triqs_dft_tools.converters import *
 from h5 import *
-from pytriqs.utility.h5diff import h5diff
+from triqs.utility.h5diff import h5diff
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 
 Converter = Wannier90Converter(seedname='LaVO3-Pnma',hdf_filename='w90_convert.out.h5')
 

test/wien2k_convert.py

@@ -20,9 +20,9 @@
 ################################################################################
 
 from h5 import *
-from pytriqs.utility.comparison_tests import *
+from triqs.utility.comparison_tests import *
-from pytriqs.utility.h5diff import h5diff 
+from triqs.utility.h5diff import h5diff 
-import pytriqs.utility.mpi as mpi
+import triqs.utility.mpi as mpi
 
 from triqs_dft_tools.converters import Wien2kConverter