\contentsline {figure}{\numberline {2.1}{\ignorespaces ploty, '15-nov-91 22:30','15-nov-91 23:50' }}{7}
\contentsline {figure}{\numberline {3.2}{\ignorespaces bcs\_24hr\_plot, '11-dec-91'}}{18}
\contentsline {figure}{\numberline {3.3}{\ignorespaces An example of a one-component fit of BCS channel 3 data by FIT\_BSC. }}{24}
\contentsline {figure}{\numberline {3.4}{\ignorespaces Time series plot of results from FIT\_BSC using FIT\_BSC\_PLOT. }}{26}
\contentsline {figure}{\numberline {4.5}{\ignorespaces plott\_hda, '15-nov-91 22:35', 10,psym=10}}{28}
\contentsline {figure}{\numberline {5.6}{\ignorespaces Coordinate definition for COAL\_IMAGE}}{41}
\contentsline {figure}{\numberline {5.7}{\ignorespaces The effective area of the SXT: The thick curve shows gives the effective area for the indicated filter. The thin curve is the open filter case (no analysis filter) effective area over-plotted for comparison. }}{45}
\contentsline {figure}{\numberline {5.8}{\ignorespaces The total SXT signal as a function of $\mathop {\mathgroup \symoperators log}\nolimits _{10}(T_e)$ for the open filter and the analysis filters as indicated. NOTE: Be and Al12 are mistakenly reversed in Tsuneta {\it et al.}, (1991). }}{46}
\contentsline {figure}{\numberline {5.9}{\ignorespaces Ratios of the SXT response functions. For the curve marked ``Be119/(2$\times $Al12)'' the effective observing time with the Al12 filter has been doubled with respect to the Be119 filter. For the curve marked ``$2\times $Al12/Al.1'' the effective observing time with the Al12 filter has again been doubled, this time with respect to the Al.1 filter. }}{47}
\contentsline {figure}{\numberline {6.10}{\ignorespaces plott\_wda, '15-nov-91 22:35', 10,psym=10}}{53}
\contentsline {figure}{\numberline {7.11}{\ignorespaces Roll Angle Offset for the SXT}}{65}
\contentsline {figure}{\numberline {7.12}{\ignorespaces Sign Convention for the SXT Roll Angle}}{66}
\contentsline {figure}{\numberline {B.13}{\ignorespaces Yohkoh Data File Format}}{81}