Table 1: The shifts of the aberration patterns for the one-mirror optical system rotating at $\Omega =60 \hbox {$^{\prime \prime }$ }/{\rm s}$ after subtracting the mean value $\delta \overline{a}^{~\rm d}_{\rm L}+\delta \overline{a}^{~\rm r}_{\rm L}=18.3834$ $\mu$ as.
$\delta a_{\rm L}\ \times 10^{-3} ~\hbox{$\mu$ as}$ $\delta a_{\rm C}\ \times 10^{-3} ~\hbox{$\mu$ as}$

$_{\displaystyle{a_{\rm C}}}$ $\backslash$ $^{\displaystyle{a_{\rm L}}}$ $-30\hbox{$^\prime$ }$ $0\hbox{$^\prime$ }$ $+30\hbox{$^\prime$ }$ $-30\hbox{$^\prime$ }$ $0\hbox{$^\prime$ }$ $+30\hbox{$^\prime$ }$

$-30\hbox{$^\prime$ }$ 0.9 -1.2 0.9 1.4 0.0 -1.4

$0\hbox{$^\prime$ }$ 0.2 -1.9 0.2 0.0 0.0 0.0

$30 \hbox{$^\prime$ }$ 0.9 -1.2 0.9 -1.4 0.0 1.4

**Table 1:** The shifts of the aberration patterns for the one-mirror optical system rotating at $\Omega =60 \hbox {$^{\prime \prime }$ }/{\rm s}$ after subtracting the mean value $\delta \overline{a}^{~\rm d}_{\rm L}+\delta \overline{a}^{~\rm r}_{\rm L}=18.3834$ $\mu$ as.
	$\delta a_{\rm L}\ \times 10^{-3} ~\hbox{$\mu$ as}$	$\delta a_{\rm C}\ \times 10^{-3} ~\hbox{$\mu$ as}$
$_{\displaystyle{a_{\rm C}}}$ $\backslash$ $^{\displaystyle{a_{\rm L}}}$	$-30\hbox{$^\prime$ }$	$0\hbox{$^\prime$ }$	$+30\hbox{$^\prime$ }$	$-30\hbox{$^\prime$ }$	$0\hbox{$^\prime$ }$	$+30\hbox{$^\prime$ }$
$-30\hbox{$^\prime$ }$	0.9	-1.2	0.9	1.4	0.0	-1.4
$0\hbox{$^\prime$ }$	0.2	-1.9	0.2	0.0	0.0	0.0
$30 \hbox{$^\prime$ }$	0.9	-1.2	0.9	-1.4	0.0	1.4

Source LaTeX | All tables | In the text