Elsarticle - CAS: Difference between revisions

From STMDocs
Jump to navigation Jump to search
Line 10: Line 10:
and have an option <code>longmktitle</code> to handle long front matter.
and have an option <code>longmktitle</code> to handle long front matter.
===Front matter===
===Front matter===
 
[[File:cas-frontmatter.png|thumb|right|319|CAS Front matter]]
<syntaxhighlight lang="latex">
<syntaxhighlight lang="latex">



Revision as of 17:52, 24 September 2018

Elsarticle - CAS

Class files

Usage

There are two class files

  1. cas-sc.cls for single column journals.
    \documentclass[<options>]{cas-sc}
    
  2. cas-dc.cls for double column journals.
    \documentclass[<options>]{cas-dc}
    

and have an option longmktitle to handle long front matter.

Front matter

CAS Front matter
\title[mode = title]{This is a title}

\tnotemark[1,2]

\tnotetext[1]{Title notes}

\author[1,3]{Editor}
   [type=editor,
    auid=000,bioid=1,
    prefix=Sir,
    role=Researcher,
    orcid=0000-0001-7511-2910,
    facebook=Editor,
    twitter=Editor,
    linkedin=Editor,
    gplus=Editor]

\cormark[1]
\fnmark[1]
\ead{cvr_1@tug.org.in}
\ead[url]{www.cvr.cc, www.tug.org.in}

\credit{Conceptualization of this study, Methodology, Software}

\author[2,4]{Chinese Author}[style=chinese]

\author[1]{First Author}
  [role=Co-ordinator,
   suffix=Jr,
   facebook=Author,
   twitter=Author,
   gplus=Author,
   linkedin=Author
   ]
\fnmark[2]
\ead{rishi@sayahna.org}
\ead[URL]{www.sayahna.org}

\credit{Credit text}

\author[1,2]{Second Author}
\ead{karl@freefriends.org}
\ead[URL]{www.tug.org}

\address[2]{Unknown university, City, Country}

\cortext[cor1]{Corresponding author text}

\fntext[fn1]{This is a author footnote.}

\nonumnote{This note has no numbers.}


\begin{abstract}
 This is a abstract
\end{abstract}

\begin{keywords}
 First keyword \sep Second keyword \sep Third keyword \sep Fourth keyword
\end{keywords}

\maketitle

Tables

\begin{table*}[width=.9\textwidth,cols=4,pos=h]
  \caption{This is a test caption.}
  \begin{tabular*}{\tblwidth}{@{} LLLL@{} }
   \toprule
    Col 1 & Col 2 & Col 3 & Col4\\
   \midrule
    12345 & 12345 & 123 & 12345 \\
    12345 & 12345 & 123 & 12345 \\
    12345 & 12345 & 123 & 12345 \\
    12345 & 12345 & 123 & 12345 \\
    12345 & 12345 & 123 & 12345 \\
   \bottomrule
  \end{tabular*}
\end{table*}

Biography

\begin{biography}[tuglogo.png]{Biography}
The evanescent polariton provided by a single sphere gives the
time coherence necessary for the observable \BEC of the quadrupole
exciton. But the spatial coherence is limited to a small region
near the sphere. To improve the spatial coherence one has to
sacrifice the temporal coherence slightly by delocalizing the
corresponding \WGM. It can be done by using an array of spheres
aligned along the $z$ direction and separated by the distance
$\delta r_{0}$ (See Fig.\ref{FIG:2}).  
\end{biography}
\bio[width=10mm,pos=l]{tuglogo.png}
\textbf{Another Biography:}
Recent experimental \cite{HARA:2005} and theoretical
\cite{DEYCH:2006} studies have shown that the \WGM can travel
along the chain as "heavy photons". Therefore the \WGM acquires
the spatial dispersion, and the evanescent quadrupole polariton
has the form (See Fig.\ref{FIG:3}):
\endbio