Changeset 552 in ETALON for papers/2016_IPAC/IPAC16_SP_CTR/MOPMB003.tex

Timestamp:

Apr 26, 2016, 5:54:12 PM (8 years ago)

Author:

hodnevuc

Message:

 

File:

• papers/2016_IPAC/IPAC16_SP_CTR/MOPMB003.tex (modified) (6 diffs)

papers/2016_IPAC/IPAC16_SP_CTR/MOPMB003.tex

@@ -33 +33 @@
 \title{Comparison of Coherent Smith-Purcell radiation and Coherent Transition Radiation\thanks{The authors are grateful for the funding received from the French ANR (contract ANR-12-JS05-0003-01) and the IDEATE International Associated Laboratory (LIA) between France and Ukraine.}}
 
-\author{Vitalii Khodnevych~\thanks{hodnevuc@lal.in2p3.fr} (LAL, Orsay;  Taras Shevchenko National University of Kyiv, Kyiv),\\ Nicolas Delerue~\thanks{delerue@lal.in2p3.fr} (LAL, Orsay), Oleg Bezshyyko ( Taras Shevchenko National University of Kyiv, Kyiv) }
+\author{Vitalii Khodnevych\textsuperscript{1}\thanks{hodnevuc@lal.in2p3.fr}, Nicolas Delerue~\thanks{delerue@lal.in2p3.fr} 
+\\(LAL, Orsay),
+\\ Oleg Bezshyyko
+\\ ( Taras Shevchenko National University of Kyiv, Kyiv)
+\\ \textsuperscript{1}also at National Taras Shevchenko University of Kyiv, Kyiv, Ukraine
+  }
+
+
+
+
 \maketitle
 
@@ -84 +93 @@
 \begin{figure}[htb]
   \centering
-  \includegraphics[width=0.9\linewidth]{plots/SEY2.eps}
-  \caption{Single electron yield for TR and SP. The screen diameter for TR is 40mm. SP SEY is presented for different beam-grating separation (3,6,9 mm). The grating used here is  $40\mbox{mm}\times180\mbox{mm}$ with 8 mm pitch and $30^o$ blaze angle.  }
+  \includegraphics[width=0.9\linewidth]{plots/SEY1488.eps}
+  \caption{Single electron yield for TR and SP. The screen diameter for TR is 40mm. SP SEY is presented for different beam-grating separation (3,6,9 mm). The grating used here is   $40\times180$ \si{mm^2}with 8 mm pitch and $30^o$ blaze angle.  }
   \label{sey}
 \end{figure}
@@ -93 +102 @@
   \centering
   \includegraphics[width=0.9\linewidth]{plots/SP2d.eps}
-  \caption{SEY for SP effect. Grating $40mm\times180mm$  with 8~mm pitch and $30^o$ blaze angle.  }
+  \caption{SEY for SP effect. Grating  $40\times180$ \si{mm^2}  with 8~mm pitch and $30^o$ blaze angle.  }
   \label{sey2d}
 \end{figure}
@@ -134 +143 @@
   \centering
   \includegraphics[width=0.9\linewidth]{plots/MAE.eps}
-  \caption{Maximum angle of emission for SP effect as function of pulsewidth and grating pitch.  Grating $40mm\times180mm$ with  $30^o$ blaze angle. The beam-grating separation is 3~mm.}
+  \caption{Maximum angle of emission for SP effect as function of pulsewidth and grating pitch.  Grating  $40\times180$ \si{mm^2} with  $30^o$ blaze angle. The beam-grating separation is 3~mm.}
   \label{mae}
 \end{figure}
@@ -152 +161 @@
   \centering
   \includegraphics[width=0.9\linewidth]{plots/TE.eps}
-  \caption{Total energy for SP effect presented as function of pulsewidth and grating pitch. Grating is $40mm\times180mm$ with  $30^o$ blaze angle. }
+  \caption{Total energy for SP effect presented as function of pulsewidth and grating pitch. Grating is  $40\times180$ \si{mm^2} with  $30^o$ blaze angle. }
   \label{Epp}
 \end{figure}
@@ -197 +206 @@
 \begin{figure}[!htb]
   \centering
-  \includegraphics[width=0.9\linewidth]{plots/SP.eps}
+  \includegraphics[width=0.9\linewidth]{plots/SP1488.eps}
   \caption{CSPR and CTR energy density as function of wavelength. The CSPR spectrum is presented for  beam-grating separations of \SIlist{3;6;9}{mm}. The grating dimensions are $40\times180$ \si{mm^2} with \SI{8}{mm} pitch and \ang{30} blaze angle. The screen diameter for TR is \SI{40}{mm}. The signal is measured as integrated with a \SI{50}{mm} diameter parabolic mirror located \SI{300}{mm} from the beam axis.}
   \label{spctr}