diff --git a/doc/basicnotions/first.rst b/doc/basicnotions/first.rst index 18235d01..c06771f1 100644 --- a/doc/basicnotions/first.rst +++ b/doc/basicnotions/first.rst @@ -49,7 +49,7 @@ Learn how to use :ref:`TRIQS ` (and the :ref:`CTHYB ` based application it is beneficial to invest a few hours to become familiar with the :ref:`TRIQS ` basics first. The -`TRIQS tutorial `_ covers +:ref:`TRIQS tutorial ` covers the most important aspects of :ref:`TRIQS `. We recommend downloading our hands-on training in the form of ipython notebooks from the `tutorials repository on GitHub `_. diff --git a/doc/conf.py.in b/doc/conf.py.in index 2a8f2bb6..4fc5b7a1 100644 --- a/doc/conf.py.in +++ b/doc/conf.py.in @@ -29,7 +29,7 @@ html_theme = 'triqs' html_theme_path = ['@TRIQS_THEMES_PATH@'] html_show_sphinx = False html_context = {'header_title': 'dft tools', - 'header_subtitle': 'connecting TRIQS to DFT packages', + 'header_subtitle': 'connecting TRIQS to DFT packages', 'header_links': [['Install', 'install'], ['Documentation', 'documentation'], ['Issues', 'issues'], @@ -39,4 +39,4 @@ html_sidebars = {'index': ['sideb.html', 'searchbox.html']} htmlhelp_basename = 'TRIQSDftToolsdoc' -intersphinx_mapping = {'python': ('http://docs.python.org/2.7', None), 'triqslibs': ('http://ipht.cea.fr/triqs', None), 'triqscthyb': ('http://ipht.cea.fr/triqs/applications/cthyb', None)} +intersphinx_mapping = {'python': ('http://docs.python.org/2.7', None), 'triqslibs': ('http://triqs.ipht.cnrs.fr/1.x', None), 'triqscthyb': ('https://triqs.ipht.cnrs.fr/1.x/applications/cthyb/', None)} diff --git a/doc/guide/dftdmft_selfcons.rst b/doc/guide/dftdmft_selfcons.rst index 47198c7d..95bc7f3e 100644 --- a/doc/guide/dftdmft_selfcons.rst +++ b/doc/guide/dftdmft_selfcons.rst @@ -16,7 +16,7 @@ Wien2k + dmftproj In order to do charge self-consistent calculations, we have to tell the band structure program about the changes in the charge density due to correlation effects. In the following, we discuss how to use the -:ref:`TRIQS ` tools in combination with the :program:`Wien2k` program. +:ref:`TRIQS ` tools in combination with the :program:`Wien2k` program. We can use the DMFT script as introduced in section :ref:`singleshot`, with just a few simple diff --git a/doc/guide/dftdmft_singleshot.rst b/doc/guide/dftdmft_singleshot.rst index f02841ad..5afcc80e 100644 --- a/doc/guide/dftdmft_singleshot.rst +++ b/doc/guide/dftdmft_singleshot.rst @@ -33,7 +33,7 @@ The next step is to setup an impurity solver. There are different solvers available within the :ref:`TRIQS ` framework. E.g. for :ref:`SrVO3 `, we will use the hybridization expansion :ref:`CTHYB solver `. Later on, we will -see also the example of the `Hubbard-I solver `_. +see also the example of the `Hubbard-I solver `_. They all have in common, that they are called by an uniform command:: S.solve(params) diff --git a/python/sumk_dft_tools.py b/python/sumk_dft_tools.py index 21a92be8..b685f9c9 100644 --- a/python/sumk_dft_tools.py +++ b/python/sumk_dft_tools.py @@ -854,7 +854,7 @@ class SumkDFTTools(SumkDFT): def transport_coefficient(self, direction, iq, n, beta, method=None): r""" Calculates the transport coefficient A_n in a given direction for a given :math:`\Omega`. The required members (Gamma_w, directions, Om_mesh) have to be obtained first - by calling the function :meth:`transport_distribution `. For n>0 A is set to NaN if :math:`\Omega` is not 0.0. + by calling the function :meth:`transport_distribution `. For n>0 A is set to NaN if :math:`\Omega` is not 0.0. Parameters ---------- @@ -918,9 +918,9 @@ class SumkDFTTools(SumkDFT): def conductivity_and_seebeck(self, beta, method=None): r""" Calculates the Seebeck coefficient and the optical conductivity by calling - :meth:`transport_coefficient `. + :meth:`transport_coefficient `. The required members (Gamma_w, directions, Om_mesh) have to be obtained first by calling the function - :meth:`transport_distribution `. + :meth:`transport_distribution `. Parameters ----------