Changeset 287 in ETALON for reconstruction/long_paper3/phase_reconstruction_paper.tex
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- Oct 15, 2015, 9:21:49 AM (9 years ago)
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reconstruction/long_paper3/phase_reconstruction_paper.tex
r284 r287 190 190 \begin{figure}[htbp] 191 191 \centering 192 \includegraphics*[width=70mm]{plot s/31.eps} \\193 \includegraphics*[width=70mm]{plot s/32.eps}192 \includegraphics*[width=70mm]{plot1510/31.eps} \\ 193 \includegraphics*[width=70mm]{plot1510/32.eps} 194 194 %\includegraphics*[width=70mm]{newFig/lin27e203line203.eps} 195 195 \caption{Comparison of different samplings with $\chi^2$ criterium (top) and $\Delta_{FWHM}$ (bottom).}%VH add picture … … 327 327 \rho_{HF}(\omega)=A\omega^B 328 328 \end{equation} 329 where the A and B coefficient are selected from the boundary conditions. 329 where the A and B coefficient are selected from the boundary conditions. But assumption of finite bunch size set boundary condition on B. So even if $B>-2$ from crosslinking conditions, we use B=-2. 330 330 Two other extrapolation methods have also been investigated: 331 331 \begin{itemize} … … 335 335 336 336 These HF extrapolation methods are compared on figure~\ref{hf} and~\ref{hf2}.\par 337 Thus, by virtue of the above arguments and simulations, It's naturally to choose the high-frequency extrapolation by power function. Constants of extrapolation functions are selected from crosslinking conditions above .337 Thus, by virtue of the above arguments and simulations, It's naturally to choose the high-frequency extrapolation by power function. Constants of extrapolation functions are selected from crosslinking conditions above and $B<=-2$ condition is also used. 338 338 339 339 … … 402 402 \begin{figure}[htbp] 403 403 \centering 404 \includegraphics*[width=70mm]{plot s/131.eps} \\405 \includegraphics*[width=70mm]{plot s/132.eps}404 \includegraphics*[width=70mm]{plot1510/131.eps} \\ 405 \includegraphics*[width=70mm]{plot1510/132.eps} 406 406 \caption{{$\Delta_{FWHM}$ (top) and $\chi^2$ (bottom) distribution of 1000 simulations reconstructed using the Hilbert transform method (black line) and Kramers-Kronig reconstruction method (red line). }}% VH change name of picture and unite with other 407 407 \label{profiles_stats_hilbert} … … 423 423 \begin{figure}[htbp] 424 424 \centering 425 \includegraphics*[width=70mm]{plot s/15.eps}425 \includegraphics*[width=70mm]{plot1510/15.eps} 426 426 \caption{$\Delta_{FWXM}$ for 1000 profiles with both methods.}%VH add picture 427 427 \label{fwxm} … … 442 442 \begin{figure}[htbp] 443 443 \centering 444 \includegraphics*[width=70mm]{plot s/171.eps} \\445 \includegraphics*[width=70mm]{plot s/172.eps} \\444 \includegraphics*[width=70mm]{plot1510/171.eps} \\ 445 \includegraphics*[width=70mm]{plot1510/172.eps} \\ 446 446 % \includegraphics*[width=75mm]{THPME088f10.eps} 447 447 \caption{Distribution of the $\chi^2$ in the case of a lorenzian distribution. }
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