Changeset 572 in ETALON


Ignore:
Timestamp:
Apr 28, 2016, 1:55:21 PM (8 years ago)
Author:
hodnevuc
Message:
 
Location:
papers/2016_IPAC/IPAC16_CLIO/poster
Files:
1 added
4 edited

Legend:

Unmodified
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  • papers/2016_IPAC/IPAC16_CLIO/poster/conference_poster_3.log

    r569 r572  
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    22entering extended mode
    33**E:/2016_IPAC/IPAC16_CLIO/poster/conference_poster_3.tex
     
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  • papers/2016_IPAC/IPAC16_CLIO/poster/conference_poster_3.tex

    r569 r572  
    9999}
    100100
    101 \headerbox{CTR}{name=ctr,column=0,row=0,below=introduction}{
     101\headerbox{CLIO installation}{name=ccc,column=0,row=0,below=introduction}{
    102102\begin{center}
    103 \includegraphics[width=\linewidth]{../MOPMB005f8.pdf}\\
    104 \smaller \textit{CTR spectrums of the different bunch profiles from CLIO simulation}
     103\includegraphics[width=\linewidth]{CLIO}\\
     104\smaller \textit{CLIO setup}
    105105\end{center}
    106 Unlike the case of CSPR, CTR will only be used to estimate the bunch length and no detailed profile reconstruction will be attempted. %The discrimination between pulse length will therefore be based primarily on CTR intensity but to enhance this phenomena we will also use band-pass filters in THz wavelength. %
     106
    107107}
     108
     109%\headerbox{CTR}{name=ctr,column=0,row=0,below=ccc}{
     110%\begin{center}
     111%\includegraphics[width=\linewidth]{../MOPMB005f8.pdf}\\
     112%\smaller \textit{CTR spectrums of the different bunch profiles from CLIO simulation}
     113%\end{center}
     114%Unlike the case of CSPR, CTR will only be used to estimate the bunch length and no detailed profile reconstruction will be attempted. %The discrimination between pulse length will therefore be based primarily on CTR intensity but to enhance this phenomena we will also use band-pass filters in THz wavelength. %
     115%}
    108116
    109117
     
    135143}
    136144
    137 \headerbox{Bunch length measurements (CSPR)}{name=results2,span=3,column=0,below=ctr}{ % To reduce this block to 1 column width, remove 'span=2'
     145\headerbox{Bunch length measurements}{name=results2,span=3,column=0,below=results1}{ % To reduce this block to 1 column width, remove 'span=2'
    138146 %The bunch length monitor will use two different radiative phenomenon:  Coherent Smith-Purcell Radiation (CSPR)~and Coherent Transition Radiation (CTR)~.
    139147 Energy distribution of Coherent Smith-Purcell spectrum as a function of the observation angle for different maximum field in the FB at left. The grating used for these simulations is $40 mm\times180 mm$ with a pitch of $8mm$ and a blaze angle of $30^o$.
    140148\begin{center}
    141 \includegraphics[width=0.40\linewidth]{../MOPMB005f6.pdf}
    142 \includegraphics[width=0.40\linewidth]{../MOPMB005f7.pdf}\\
    143 \smaller \textit{ CSPR spectrums with original (left) and normalized (right) amplitude}
     149\includegraphics[width=0.30\linewidth]{../MOPMB005f6.pdf}
     150\includegraphics[width=0.30\linewidth]{../MOPMB005f7.pdf}
     151\includegraphics[width=0.295\linewidth]{../MOPMB005f8.pdf}\\
     152\smaller \textit{ CSPR spectrums with original (left) and normalized (center) amplitude. At right CTR spectrums of the different bunch profiles from CLIO simulation.}
    144153\end{center}
    145 
     154Unlike the case of CSPR, CTR will only be used to estimate the bunch length and no detailed profile reconstruction will be attempted.
    146155
    147156}
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