===== EFFECTIVITY CORRECTION - HED 3X HIT LEVELS ===== **Format(s): f10** ERNE Effectivity Coefficients for HED 3x Hit Levels Version 1.0 (TM format f10) Usage: multiply lev-3 intensity values for measurement periods with HED 3x hit levels by the tabulated numbers below. Version history: 1.2 - 2003-01-29 New values based on f10 measurements during 1996. Two 1x/3x hit level period pairs were considered: 2.6 - 17.6 1x 19.6 - 31.7 3x 1.11 - 1.12 3x 3.12 - 19.12 1x Results: 1) The LED channels and lower HED channels had higher average intensities during 3x-hit level periods resulting in correction factors smaller than 1.0. This was presumably due to small particle events that were present during the (longer) 3x integration times. 2) HED channel 11 was empty as anticipated. 3) It seems that only HED channels 6-10 were affected by the hit level changes. This conforms also with the earlier understanding. The corresponding correction factors between the two periods are also in good agreement. This is in contrast to other energies, where the differences tend to be much bigger. This seems to indicate also that the small particle events had no effect in the higher HED energies. The correction factors for the HED channels 6-10 in the table are set to average values attained from the two periods. Other factors are set to 1.0. 1.1 - 2002-06-18 New values based on format-40 values (hedx3eff.4.0) The f10 coefficients are calculated from the f40 proton values by weighting the f40 coefficients with the GdE-values of the contributing f40 energy channels. In other words, these values are weighted sums of the f40 values, weight factor being the corresponding GdE-values. 1.0 - 2002-05-08 Original version with dymmy coefficients, ER --------------------------------------- p He --------------------------------------- 1.0 1.0 ; 0 LED 0 1.0 1.0 ; 1 1 1.0 1.0 ; 2 2 1.0 1.0 ; 3 3 1.0 1.0 ; 4 4 1.0 1.0 ; 5 5 1.0 1.0 ; 6 6 1.0 1.0 ; 7 7 1.0 1.0 ; 8 8 1.0 1.0 ; 9 9 1.0 1.0 ; 10 10 1.0 1.0 ; 11 11 1.0 1.0 ; 12 HED 0 1.0 1.0 ; 13 1 1.0 1.0 ; 14 2 1.0 1.0 ; 15 3 1.0 1.0 ; 16 4 1.0 1.0 ; 17 5 1.14090 1.0 ; 18 6 2.40213 1.0 ; 19 7 24.5816 1.0 ; 20 8 5.90016 1.0 ; 21 9 3.25230 1.0 ; 22 10 1.0 1.0 ; 23 11