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author | Karl Berry <karl@freefriends.org> | 2012-08-15 23:11:00 +0000 |
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committer | Karl Berry <karl@freefriends.org> | 2012-08-15 23:11:00 +0000 |
commit | da0e0b99c435f4dbdf0423f98a795ea6410b05e7 (patch) | |
tree | 2f467c1f7e0f2f88c02bda2ab0c6e00f7ae22bcd /Master/texmf-dist/doc/latex/classicthesis/Chapters | |
parent | 4b94812ec8dc518960017e3e9cd77ab3774fc0f1 (diff) |
classicthesis (15aug12)
git-svn-id: svn://tug.org/texlive/trunk@27416 c570f23f-e606-0410-a88d-b1316a301751
Diffstat (limited to 'Master/texmf-dist/doc/latex/classicthesis/Chapters')
-rw-r--r-- | Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter01.tex | 37 | ||||
-rw-r--r-- | Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter03.tex | 26 |
2 files changed, 49 insertions, 14 deletions
diff --git a/Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter01.tex b/Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter01.tex index a76ffc66892..1b1765ed6b6 100644 --- a/Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter01.tex +++ b/Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter01.tex @@ -316,10 +316,45 @@ Spanish languages need an extra option in order to work with this template: Thanks to an unknown person for this information (via Google Code issue reporting). +\paragraph{Further information for using \texttt{classicthesis} with Spanish (in addition to the above)} +In the file \texttt{ClassicThesis.tex} activate the language: +\begin{verbatim} + \selectlanguage{spanish} +\end{verbatim} + +In order to get the bibliography style right, you can use the following: +\begin{verbatim} + \bibliographystyle{babplain} +\end{verbatim} + +For this, it is necessary to load the package: +\begin{verbatim} + \usepackage[spanish,fixlanguage]{babelbib} + \selectbiblanguage{spanish} +\end{verbatim} + +If there are issues changing \verb|\tablename|, \eg, using this: +\begin{verbatim} + \renewcommand{\bibname}{Referencias} + \renewcommand{\tablename}{Tabla} +\end{verbatim} + +This can be solved by passing \texttt{es-tabla} parameter to \texttt{babel}: +\begin{verbatim} + \PassOptionsToPackage{es-tabla,spanish,es-lcroman,english}{babel} + \usepackage{babel} +\end{verbatim} + +But it is also necessary set \texttt{spanish} in the \verb|\documentclass|. + +Thanks to Alvaro Jaramillo Duque for this information. + + \subsection*{Compatibility with the \texttt{pdfsync} Package} Using the \texttt{pdfsync} package leads to linebreaking problems with the \texttt{graffito} command. Thanks to Henrik Schumacher for this information. - + + \section{Future Work} So far, this is a quite stable version that served a couple of people diff --git a/Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter03.tex b/Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter03.tex index c06b7e5d58a..d7fdeeec58e 100644 --- a/Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter03.tex +++ b/Master/texmf-dist/doc/latex/classicthesis/Chapters/Chapter03.tex @@ -23,30 +23,30 @@ energy transfer in a single collision with an atomic electron: \graffito{You might get unexpected results using math in chapter or section heads. Consider the \texttt{pdfspacing} option.} \begin{equation} -\kappa =\frac{\xi}{E_{\mathrm{max}}} %\mathbb{ZNR} +\kappa =\frac{\xi}{E_{\textrm{max}}} %\mathbb{ZNR} \end{equation} -$E_{\mathrm{max}}$ is the maximum transferable energy in a single +$E_{\textrm{max}}$ is the maximum transferable energy in a single collision with an atomic electron. \[ -E_{\mathrm{max}} =\frac{2 m_{\mathrm{e}} \beta^2\gamma^2 }{1 + -2\gamma m_{\mathrm{e}}/m_{\mathrm{x}} + \left ( m_{\mathrm{e}} -/m_{\mathrm{x}}\right)^2}\ , +E_{\textrm{max}} =\frac{2 m_{\textrm{e}} \beta^2\gamma^2 }{1 + +2\gamma m_{\textrm{e}}/m_{\textrm{x}} + \left ( m_{\textrm{e}} +/m_{\textrm{x}}\right)^2}\ , \] -where $\gamma = E/m_{\mathrm{x}}$, $E$ is energy and -$m_{\mathrm{x}}$ the mass of the incident particle, -$\beta^2 = 1 - 1/\gamma^2$ and $m_{\mathrm{e}}$ is the electron mass. +where $\gamma = E/m_{\textrm{x}}$, $E$ is energy and +$m_{\textrm{x}}$ the mass of the incident particle, +$\beta^2 = 1 - 1/\gamma^2$ and $m_{\textrm{e}}$ is the electron mass. $\xi$ comes from the Rutherford scattering cross section and is defined as: -\begin{eqnarray*} \xi = \frac{2\pi z^2 e^4 N_{\mathrm{Av}} Z \rho -\delta x}{m_{\mathrm{e}} \beta^2 c^2 A} = 153.4 \frac{z^2}{\beta^2} +\begin{eqnarray*} \xi = \frac{2\pi z^2 e^4 N_{\textrm{Av}} Z \rho +\delta x}{m_{\textrm{e}} \beta^2 c^2 A} = 153.4 \frac{z^2}{\beta^2} \frac{Z}{A} - \rho \delta x \quad\mathrm{keV}, + \rho \delta x \quad\textrm{keV}, \end{eqnarray*} where \begin{tabular}{ll} $z$ & charge of the incident particle \\ -$N_{\mathrm{Av}}$ & Avogadro's number \\ +$N_{\textrm{Av}}$ & Avogadro's number \\ $Z$ & atomic number of the material \\ $A$ & atomic weight of the material \\ $\rho$ & density \\ @@ -54,7 +54,7 @@ $ \delta x$ & thickness of the material \\ \end{tabular} $\kappa$ measures the contribution of the collisions with energy -transfer close to $E_{\mathrm{max}}$. For a given absorber, $\kappa$ +transfer close to $E_{\textrm{max}}$. For a given absorber, $\kappa$ tends towards large values if $\delta x$ is large and/or if $\beta$ is small. Likewise, $\kappa$ tends towards zero if $\delta x $ is small |