Changeset 24993
- Timestamp:
- Aug 4, 2009, 8:43:20 AM (17 years ago)
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- 1 edited
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trunk/psphot/doc/notes.20090523.txt (modified) (2 diffs)
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trunk/psphot/doc/notes.20090523.txt
r24583 r24993 1 1 2 20090 523 : extended source analysis -- further development2 20090725 : extended source radial profiles 3 3 4 issues to address:4 I need to fix the Petrosian and similar code. There are several issues: 5 5 6 * quality of moments used for initial psf selection 7 - what is the behavior of moments with Gaussian windowing as function of S/N & size? 8 - can we choose a sigma value that will give reliable moments for an expected range of seeing? 6 1) correct implementation of the actual Petrosian radius / Petrosian flux measurement: 9 7 10 * moments for galaxy model guesses 11 - trade-off between Gaussian windowing, tophat windowing, and S/N windowing in footprint area 8 R_p : Given F(R) : F(0) / F(R_p) = 0.9 ?? (something like this...) 12 9 13 initial dev work:10 Actually implemented by calculating the average surface brightness in annullii: 14 11 15 * add Gaussian windowing, S/N windowing, (tophat windowing) and options to select 12 R_p : Given F(R) -> define f(R) = \sum_{R-dR}^{R+dR}F(R) / 4\pi R dR 13 R_p : f(dR) / F(R_p) = P_ratio 16 14 17 * check visualization of moments 15 2) need to construct a clean, normalized radial profile to make this measurement 16 17 * generate radial profiles for each of N annular wedges 18 * find R_50 : f(0) / f(R_50) = 0.5 19 $ fit the ellipse of R_50 to Rmaj sin(T) + Rmin cos(T) 20 21 22 cos(a+b) = cos(a) cos(b) - sin(a) sin(b) 23 sin(a+b) = cos(a) sin(b) + cos(b) sin(a) 24 25 cos(theta+To) = cos(theta) cos(To) - sin(theta) sin(To) 26 sin(theta+To) = cos(theta) sin(To) + sin(theta) cos(To) 27 28 R_x = R_maj cos(theta + theta_o) = R_maj cos(theta) cos(theta_o) - Rmaj sin(theta) sin(theta_o) 29 R_y = R_min sin(theta + theta_o) = R_min cos(theta) sin(theta_o) + Rmin sin(theta) cos(theta_o) 30 31 R_X = R_x cos(phi) - R_y sin(phi) 32 R_Y = R_x sin(phi) + R_y cos(phi) 33 34 R_X = R_maj cos(phi) cos(theta + To) - R_min sin(phi) sin(theta + To) 35 R_Y = R_maj sin(phi) cos(theta + To) + R_min cos(phi) sin(theta + To) 36 37 R_X = (R_maj cos(phi) cos (To) - R_min sin(phi) sin(To)) cos(theta) - (Rmaj cos(phi) sin(To) + Rmin sin(phi) cos(To)) sin(theta) 38 R_Y = (R_maj sin(phi) cos (To) + R_min cos(phi) sin(To)) cos(theta) - (Rmaj cos(phi) sin(To) + Rmin sin(phi) cos(To)) sin(theta) 39 40 41 R_X = Ax cos(theta) + Bx sin(theta) 42 R_Y = Ay cos(theta) + By sin(theta) 43 44 Ax = \sum (R_X * cos(theta)) 45 Bx = \sum (R_X * sin(theta)) 46 Ay = \sum (R_Y * cos(theta)) 47 By = \sum (R_Y * sin(theta)) 48 49 R_maj = sqrt(Ax^2 + Ay^2) 50 R_min = sqrt(Bx^2 + By^2) 51 52 phi = atan2(Bx + By, Ax + Ay) 53 54 *** get rest of math from my notebook... 55 56 18 57 19 58 20090525 : some clarity of issues: … … 40 79 41 80 * QGAUSS with see 81 82 20090523 : extended source analysis -- further development 83 84 issues to address: 85 86 * quality of moments used for initial psf selection 87 - what is the behavior of moments with Gaussian windowing as function of S/N & size? 88 - can we choose a sigma value that will give reliable moments for an expected range of seeing? 89 90 * moments for galaxy model guesses 91 - trade-off between Gaussian windowing, tophat windowing, and S/N windowing in footprint area 92 93 initial dev work: 94 95 * add Gaussian windowing, S/N windowing, (tophat windowing) and options to select 96 97 * check visualization of moments 98
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