From fcf95f4bd4c4191e944e9eacc77fd597377d8483 Mon Sep 17 00:00:00 2001 From: Evgeny Stambulchik Date: Tue, 29 Nov 2016 10:32:08 -0500 Subject: [PATCH] Trailing spaces removed. --- doc/sfaclang.tex | 26 +++++++++++++------------- 1 file changed, 13 insertions(+), 13 deletions(-) diff --git a/doc/sfaclang.tex b/doc/sfaclang.tex index 100c129..330b60c 100644 --- a/doc/sfaclang.tex +++ b/doc/sfaclang.tex @@ -81,7 +81,7 @@ \subsection{Electron Shell Configuration} occupation number(s), separated by ``;'', e.g., $3*10;3s>0;3p>5$ generate configurations that have at least 1 electron in the $3s$ shell and at least 6 electrons in the $3p$ shell. The logical relations allowed in conditions -include $=$, $>$, and $<$. +include $=$, $>$, and $<$. The third form of invoking this function allows for running calculations in the {\em experimental} \hyperref[subsec:mixed_mode]{mixed mode}, with the \var{uta} @@ -95,7 +95,7 @@ \subsection{Electron Shell Configuration} This functions returns a list of non-relativistic configurations corresponding to the supplied configuration strings, which may contain wild casts as in the \funcref{Config} function. It is useful, e.g., when one wants to know the -non-relativistic configurations of \key{1*2 2*2 3*1}. +non-relativistic configurations of \key{1*2 2*2 3*1}. \end{fundesc} \begin{fundesc}{ListConfig}{\opt{fn, g}} @@ -116,7 +116,7 @@ \subsection{Structure Calculations} arguments. Otherwise, the configurations given in that function are used to generate the mean configuration automatically. It is important that this function be called before \funcref{OptimizeRadial} and after -\funcref[0]{ConfigEnergy}, if the later is used. +\funcref[0]{ConfigEnergy}, if the latter is used. \end{fundesc} \begin{fundesc}{BasisTable}{fn\opt{,m}} @@ -174,7 +174,7 @@ \subsection{Structure Calculations} potential, $\lambda$ and $a$, in the formula \begin{equation} V_0(r) = -\frac{Z}{r} + \frac{N-1}{r}\left(1-\frac{\exp(-\lambda -r)}{1+ar}\right). +r)}{1+ar}\right). \end{equation} After that, the mean configuration used to generate the potential is printed in 3 columns representing the principal quantum number, the relativistic @@ -254,7 +254,7 @@ \subsection{Structure Calculations} Set the principal quantum number \var{n} and the orbital angular momentum \var{l}, beyond which, the hydrogenic approximation for the E1 multipole integrals should be used. If this routine is not called or the arguments are not -given, the default values of \var{n} = 20 and \var{l} = 10 are used. +given, the default values of \var{n} = 20 and \var{l} = 10 are used. \end{fundesc} \begin{fundesc}{SetMaxRank}{k} @@ -281,7 +281,7 @@ \subsection{Structure Calculations} printed out during the optimization. This routine does not need to be called. The default for \var{t} is $10^{-6}$, \var{s} is determined dynamically according to the type of ion, \var{m} is 128, and \var{p} is 0 for no printing -out of information. +out of information. \end{fundesc} \begin{fundesc}{SetOptimizeMaxIter}{m} @@ -411,7 +411,7 @@ \subsection{Radiative Transitions} \begin{fundesc}{SetTransitionGauge}{g} Set the gauge for radiative transition. 1 for Coulomb gauge (velocity form) and -2 for Babushkin gauge (length form, which is the default). +2 for Babushkin gauge (length form, which is the default). \end{fundesc} \begin{fundesc}{SetTransitionMaxE}{max\_e} @@ -537,7 +537,7 @@ \subsection{Collisional Excitation} the grid is given by a list \var{g}. In the second form, the grid is constructed with \var{n} points from \var{e0} to \var{e1}. This routine does not need to be called. A 3-point grid is constructed by default. Calling this function with -\var{n}=0 resets the grid to the system default. +\var{n}=0 resets the grid to the system default. \end{fundesc} \begin{fundesc}{SetUsrCEGrid}{g $\mid$ n\opt{, e0, e1}} @@ -623,7 +623,7 @@ \subsection{Collisional Ionization} \begin{fundesc}{SetUsrCIEGrid}{g $\mid$ n\opt{, e0, e1}} Set the user collision energy grid for collisional ionization. The collision -strengths on this grid are output. +strengths on this grid are output. \end{fundesc} @@ -644,7 +644,7 @@ \subsection{Radiative Recombination and Photoionization} radiative recombination and photoionization cross sections. The optional multipole type \var{m} is set to -1 (E1) by default. In almost all cases, no other multipole types should be important. The results are saved in file -\var{fn}. +\var{fn}. \end{fundesc} @@ -655,7 +655,7 @@ \subsection{Radiative Recombination and Photoionization} \var{e0} to \var{e1}. The energies are in units of eV. This function does not need to be called. A 6 point grid is constructed according to the transition array being considered by default. Calling this function with \var{n}=0 reset -the grid to system default. +the grid to system default. \end{fundesc} \begin{fundesc}{SetPEGridLimits}{e0, e1} @@ -734,7 +734,7 @@ \subsection{Data Storage and Manipulation} \begin{fundesc}{AppendTable}{fn} By default, when a new script is executed, existing binary files are -overwritten. If instead the new data should be appended to a file, use +overwritten. If instead the new data should be appended to a file, use this function to set the append flag. \end{fundesc} @@ -787,7 +787,7 @@ \subsection{Miscellaneous} \end{fundesc} \begin{fundesc}{Info}{} -Print out the version information of \cFAC. +Print out the version information of \cFAC. \end{fundesc} \begin{fundesc}{Pause}{}