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\title{CLIC\\
  Continuum and Line Interferometer Calibration}%
\author{V. Pi\'etu$^{1}$}%
\date{Dec 18th, 2020}%
\makeindex{}

%
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$ b_{ik}$%
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$ I,Q,U,V$%
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$ P_{hot}$%
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$ \cos(El)$%
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$ ~130$%
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$ f$%
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$\displaystyle a$%
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\lthtmlinlinemathA{tex2html_wrap_indisplay7249}%
$\displaystyle b\xi$%
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$\displaystyle \phi_3 (\xi,\eta)$%
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{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_indisplay7255}%
$\displaystyle c\eta$%
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$\displaystyle \phi_4 (\xi,\eta)$%
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\lthtmlinlinemathA{tex2html_wrap_indisplay7261}%
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{\newpage\clearpage
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$\displaystyle \phi_5 (\xi,\eta)$%
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$\displaystyle \delta x\frac{\xi}{f}\left(1-\frac{1}{\sqrt{\frac{r^2}{f^2}
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{\newpage\clearpage
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$\displaystyle \phi_6 (\xi,\eta)$%
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{\newpage\clearpage
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$\displaystyle \delta y\frac{\eta}{f}\left(1-\frac{1}{\sqrt{\frac{r^2}{f^2}
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{\newpage\clearpage
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$\displaystyle \phi_7 (\xi,\eta)$%
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{\newpage\clearpage
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{\newpage\clearpage
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$\displaystyle \phi_8 (\xi,\eta)$%
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{\newpage\clearpage
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$ a$%
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{\newpage\clearpage
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$ b$%
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{\newpage\clearpage
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$ c$%
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{\newpage\clearpage
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$ \delta x$%
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{\newpage\clearpage
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$ \delta y$%
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{\newpage\clearpage
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$ \delta z$%
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{\newpage\clearpage
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$ a_{+}$%
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{\newpage\clearpage
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$ a_{\times}$%
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{\newpage\clearpage
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$ ^\circ$%
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{\newpage\clearpage
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$ \psi_a$%
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{\newpage\clearpage
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$\displaystyle \psi_a = \frac{\arctan{(a_{\times},a_{+})}}{2}$%
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{\newpage\clearpage
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$ \eta_A$%
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{\newpage\clearpage
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$ \eta_I$%
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{\newpage\clearpage
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$\displaystyle \frac{\lvert \int_A A(\xi,\eta)\exp(i \phi (\xi,\eta))d\xi d\eta
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{\newpage\clearpage
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{\newpage\clearpage
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$\displaystyle \frac{\lvert \int_A A(\xi,\eta)d\xi d\eta
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{\newpage\clearpage
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$\displaystyle J=\frac{2k}{\eta_A \pi r^2}$%
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{\newpage\clearpage
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$\displaystyle \delta p = \delta \phi \times \frac{\lambda}{4\pi}\times\sqrt{1+\frac{r^2} {4f^2}}$%
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$ \phi_j-\phi_i$%
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{\newpage\clearpage
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$\displaystyle \tau_g$%
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{\newpage\clearpage
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$\displaystyle \frac{{\bf b_{\cdot} s}}{c}$%
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{\newpage\clearpage
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$\displaystyle \frac{1}{c}\left(X_{ij}\cos h\cos\delta - Y_{ij}\sin h\cos \delta 
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\stepcounter{subsubsection}
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$ F_{rest}^{ref}$%
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{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline7362}%
$ v$%
\lthtmlinlinemathZ
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{\newpage\clearpage
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$ F_{IF}^{ref}$%
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{\newpage\clearpage
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$ F_{rest}$%
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{\newpage\clearpage
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$ F_{topo}$%
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{\newpage\clearpage
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$\displaystyle F_{topo}  = F_{rest} \left(1+\delta-\frac{v}{c} \right)$%
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{\newpage\clearpage
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$ \delta$%
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{\newpage\clearpage
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$ F_{IF} = \pm(F_{topo}-F_{LO1})$%
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{\newpage\clearpage
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$\displaystyle F_{IF} = \pm \left(F_{rest} \left(1+\delta-\frac{v}{c}\right) - F_{LO1}\right)$%
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{\newpage\clearpage
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$\displaystyle F_{LO1} = F_{rest}^{ref}\left(1+\delta-\frac{v}{c}\right)\mp F_{IF}^{ref}$%
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{\newpage\clearpage
\lthtmlinlinemathA{tex2html_wrap_inline7386}%
$ F_{LO1}$%
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{\newpage\clearpage
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$ i_{IF}$%
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$ T$%
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$ K_{p}$%
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$\displaystyle P_{hot}$%
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$ C_{ii}$%
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$ T_{emi}$%
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$ T_{sys,s}$%
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$ T_{sys,i}$%
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{\newpage\clearpage
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$ T_{ijk}$%
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$ T_i$%
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{\newpage\clearpage
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$ \nu_1$%
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{\newpage\clearpage
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$ \nu_2$%
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$ \nu_3$%
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$ \nu^2$%
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$\displaystyle T_{triple} = \frac{1-\left(\frac{\nu_1}{\nu_2}\right)^2}{1-\left(\frac{\nu_2}{\nu_3}\right)^2}\left(T_2-T_3\left(\frac{\nu_2}{\nu_3}\right)^2\right)-\left(T_1-T_2\left(\frac{\nu_1}{\nu_2}\right)^2\right)$%
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$ (u,v)$%
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\end{document}
