IMPORTANT NOTE: To derive irradiance from XRT signals after May-2012(when the stray light started to appear), two types of corrections are required:
(1) Subtraction of stray light image from each X-ray images.
(2) Modify XRT response functions so that it reflects the
appearance of the stray light.
This study only handles the correction (1), because we don't have the confident method yet for the correction (2).
-- Contents Summary of Generic File: /disk/yla/takeda/xrt_irradiance/teemirrad_v4_hybrid_201606.genx-- ..... Data Section ..... ** Structure MS_290034151011, 9 tags, length=506224, data length=502396: INDEX_AM STRUCT -> MS_290034151010 Array[58] TE DOUBLE Array[58] EM DOUBLE Array[58] IRRAD1_8 DOUBLE Array[58] IRRAD1_10 DOUBLE Array[58] IRRAD1_12 DOUBLE Array[58] IRRAD04_20 DOUBLE Array[58] IRRAD5_60 DOUBLE Array[58] IRRAD4_200 DOUBLE Array[58] -----------------------------------------------------------
Al_mesh | Ti_poly | Al_poly |
Al_poly/Al_mesh | Ti_poly/Al_mesh |
The calcualtion of model solar spectra was done with CHIANTI atomic DB & SW ver. 8.0.7.
The elemental abundance files used in the calculation are as follows:
Year | 1-8A | 1-10A | 1-12A | 0.4-20A | 5-60A | 4-200A |
2008 | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM |
2009 | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM |
2010 | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM |
2011 | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM |
2012 | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM |
2013 | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM | TP_AM |
2014 | TP_AM AP_AM |
TP_AM AP_AM |
TP_AM AP_AM |
TP_AM AP_AM |
TP_AM AP_AM |
TP_AM AP_AM |
2015 | TP_AM AP_AM |
TP_AM AP_AM |
TP_AM AP_AM |
TP_AM AP_AM |
TP_AM AP_AM |
TP_AM AP_AM |
2016 | AP_AM | AP_AM | AP_AM | AP_AM | AP_AM | AP_AM |
2017 | AP_AM | AP_AM | AP_AM | AP_AM | AP_AM | AP_AM |
2018 | AP_AM | AP_AM | AP_AM | AP_AM | AP_AM | AP_AM |
2019 | AP_AM | AP_AM | AP_AM | AP_AM | AP_AM | AP_AM |