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fnevgeny committed Nov 29, 2016
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26 changes: 13 additions & 13 deletions doc/sfaclang.tex
Original file line number Diff line number Diff line change
Expand Up @@ -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}
Expand All @@ -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}}
Expand All @@ -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}}
Expand Down Expand Up @@ -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
Expand Down Expand Up @@ -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}
Expand All @@ -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}
Expand Down Expand Up @@ -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}
Expand Down Expand Up @@ -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}}
Expand Down Expand Up @@ -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}


Expand All @@ -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}


Expand All @@ -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}
Expand Down Expand Up @@ -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}

Expand Down Expand Up @@ -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}{}
Expand Down

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