diff --git a/README.rst b/README.rst index 0997e9bc97ff11be477955163c44f5099358c543..0940247b080c8f37832b70ba875d6b9422119a22 100644 --- a/README.rst +++ b/README.rst @@ -1,5 +1,7 @@ -.. image:: https://gitlab.mpcdf.mpg.de/mjr/bfps/badges/develop/build.svg - :target: https://gitlab.mpcdf.mpg.de/mjr/bfps/commits/develop +.. only:: html + + .. image:: https://gitlab.mpcdf.mpg.de/mjr/bfps/badges/develop/build.svg + :target: https://gitlab.mpcdf.mpg.de/mjr/bfps/commits/develop ========================================= Turbulence Tools: Lagrangian and Eulerian diff --git a/cpp/kspace.cpp b/cpp/kspace.cpp index 213fbcbb48e229c4217a1c61d109121ae47e843c..d759219872b7fd9efb1bf6ca98909aa766881649 100644 --- a/cpp/kspace.cpp +++ b/cpp/kspace.cpp @@ -352,25 +352,33 @@ void kspace<be, dt>::Gauss_filter( * a Gaussian filter and a sharp real space spherical filter. * * Filter expressions in real space are as follows: - * \f{eqnarray*}{ - * \phi^b_\ell(r) &=& - * \frac{1}{\ell^3}\frac{6}{\pi} H(\ell/2 - r) \\ - * \phi^g_\ell(r) &=& + * \f[ + * \phi^b_\ell(r) = + * \frac{1}{\ell^3}\frac{6}{\pi} H(\ell/2 - r) + * \f] + * \f[ + * \phi^g_\ell(r) = * \frac{1}{\sigma_\ell^3}\frac{1}{(2\pi)^{3/2}} - * \exp\left(-\frac{1}{2}\left(\frac{r}{\sigma_\ell}\right)^2\right) \\ - * \phi^s_\ell(r) &=& + * \exp\left(-\frac{1}{2}\left(\frac{r}{\sigma_\ell}\right)^2\right) + * \f] + * \f[ + * \phi^s_\ell(r) = * \frac{1}{2 \pi^2 r^3} * \left(\sin k_\ell r - k_\ell r \cos k_\ell r\right) - * \f} + * \f] * and the corresponding expressions in Fourier space are: - * \f{eqnarray*}{ - * \hat{\phi^b_\ell}(k) &=& + * \f[ + * \hat{\phi^b_\ell}(k) = * \frac{3}{2(k\ell/2)^3} - * \left(2\sin (k \ell/2) - k \ell \cos (k \ell/2)\right) \\ - * \hat{\phi^g_\ell}(k) &=& - * \exp\left(-\frac{1}{2}k^2 \sigma_\ell^2\right) \\ - * \hat{\phi^s_\ell}(k) &=& H(k_\ell - k) - * \f} + * \left(2\sin (k \ell/2) - k \ell \cos (k \ell/2)\right) + * \f] + * \f[ + * \hat{\phi^g_\ell}(k) = + * \exp\left(-\frac{1}{2}k^2 \sigma_\ell^2\right) + * \f] + * \f[ + * \hat{\phi^s_\ell}(k) = H(k_\ell - k) + * \f] * * \f$ k_\ell \f$ is given as a parameter, and then we use * \f[ @@ -425,7 +433,7 @@ int kspace<be, dt>::filter( * a Gaussian filter and a sharp real space spherical filter. * * Filter expressions in real space are as follows: - * \f{eqnarray*}{ + * \begin{eqnarray*} * \phi^b_\ell(r) &=& * \frac{1}{\ell^3}\frac{6}{\pi} H(\ell/2 - r) \\ * \phi^g_\ell(r) &=& @@ -434,16 +442,16 @@ int kspace<be, dt>::filter( * \phi^s_\ell(r) &=& * \frac{1}{2 \pi^2 r^3} * \left(\sin k_\ell r - k_\ell r \cos k_\ell r\right) - * \f} + * \end{eqnarray*} * and the corresponding expressions in Fourier space are: - * \f{eqnarray*}{ + * \begin{eqnarray*} * \hat{\phi^b_\ell}(k) &=& * \frac{3}{2(k\ell/2)^3} * \left(2\sin (k \ell/2) - k \ell \cos (k \ell/2)\right) \\ * \hat{\phi^g_\ell}(k) &=& * \exp\left(-\frac{1}{2}k^2 \sigma_\ell^2\right) \\ * \hat{\phi^s_\ell}(k) &=& H(k_\ell - k) - * \f} + * \end{eqnarray*} * * \f$\sigma_\ell\f$ and \f$k_\ell\f$ are calibrated such that the energy of * the large scales is approximately the same (within the inertial range) diff --git a/documentation/conf.py b/documentation/conf.py index e37f8e523e2039897c993372686bc0c15ef0ccdf..be67c310772ab154210d7bb5c348b0e594d11e8b 100644 --- a/documentation/conf.py +++ b/documentation/conf.py @@ -225,7 +225,7 @@ latex_elements = { #'pointsize': '10pt', # Additional stuff for the LaTeX preamble. -#'preamble': '', +'preamble': '\usepackage{amssymb,amsmath,amsfonts}', # Latex figure (float) alignment #'figure_align': 'htbp',