Cong Xu and Jarrett briefly explored the issue of galaxy symmetry. GALWORKS computes several "symmetry" measures, including CHI^2 fits to the ellipse modeling, flux ratios across the semi-major axis, and cross-corration (across semi-major axis). Symmetry details can be found here.
Our goal was to find galaxy pairs and "disturbed" galaxies, as well
as take a census of artifacts, in particular those generated from bright stars.
Our qualitative study did reveal asymmetric galaxies (no surprise) and did
bring to the fore sources generated from bright stars. The brighter the
asymmetric source, the more likely it is an artifact. The most annoying
artifacts are the "edge flares". These derive from bright star located
just beyond the scan edge.
Here is an example of an
edge flare. Jarrett modified GALWORKS to better deal with
edge flares based on this work. The module edge_flare
is designed to eliminate these artifacts without killing inclined galaxies.
This work has been suspended until Cong returns from China.
The original bright star masking method
relied upon PIPELINE V2 photometry for bright stars.
Very bright stars that saturate in R1 will not have reliable mags (nor by
association, masking radii) for V2 reduction. The improved PIPELINE V3
estimates the integrated flux of R1-saturated stars by integrating and
extrapolating the radial profile with a functional fit (work by Cong Xu
and Gene Kopan).
Very bright stars will have reliable mags under
most conditions. Analysis of the bright star masking for these types of stars
reveals underestimation of the halo radius. A slight scaling adjust is therefore
made for the bright end of the halo-radius masking scale. The results
look very good. See
for some details.
The Abell 3558 repeat data sets and RTB tests are detailed in Repeatibility Tests. The tables below represents the latest (mostly stable) GALWORKS V3, and comparison with V2 repeatibility. Note: these tests were carried out on data sets generated by the V2 pipeline (but with V3 GALWORKS) and hence are not a comprehensive test of the V3 pipeline. These tests will come later when the RTBs have been generated.
ABELL 3558 Repeatibility, GALWORKS V3
-- | -- | -- | non-contaminated | ... | | | contaminated | ... | | |
---|---|---|---|---|---|---|---|---|
fname | mag- | mag+ | #r | #p | C | #r | #p | C |
J7_comp_1.tbl | 14.00 | 15.00 | 2518 | 2676 | 0.94 | 814 | 969 | 0.840 |
H7_comp_1.tbl | 13.70 | 14.20 | 1190 | 1374 | 0.87 | 452 | 518 | 0.873 |
K7_comp_1.tbl | 13.00 | 13.50 | 1415 | 1398 | 1.01 | 200 | 233 | 0.858 |
J7_comp_2.tbl | 14.00 | 15.00 | 20 | 239 | 0.08 | 16 | 197 | 0.081 |
H7_comp_2.tbl | 13.70 | 14.20 | 10 | 135 | 0.07 | 1 | 11 | 0.091 |
K7_comp_2.tbl | 13.00 | 13.50 | 5 | 13 | 0.38 | 0 | 0 | 0.000 |
fname | val- | val+ | # | valbar | RMS | # | valbar | RMS |
J7_repeats_1.tbl | 14.00 | 15.00 | 118 | 14.45 | 0.068 | 35 | 14.58 | 0.093 |
H7_repeats_1.tbl | 13.70 | 14.20 | 53 | 13.95 | 0.104 | 18 | 14.04 | 0.118 |
K7_repeats_1.tbl | 13.00 | 13.50 | 75 | 13.23 | 0.092 | 10 | 13.22 | 0.094 |
Jf20e_repeats_1.tbl | 14.00 | 15.00 | 110 | 14.48 | 0.079 | 36 | 14.57 | 0.101 |
Hf20e_repeats_1.tbl | 13.70 | 14.20 | 52 | 13.94 | 0.098 | 14 | 14.04 | 0.111 |
Kf20e_repeats_1.tbl | 13.00 | 13.50 | 71 | 13.24 | 0.111 | 10 | 13.18 | 0.112 |
Jf20c_repeats_1.tbl | 14.00 | 15.00 | 113 | 14.44 | 0.072 | 38 | 14.60 | 0.117 |
Hf20c_repeats_1.tbl | 13.70 | 14.20 | 53 | 13.94 | 0.107 | 21 | 14.04 | 0.143 |
Kf20c_repeats_1.tbl | 13.00 | 13.50 | 71 | 13.23 | 0.101 | 12 | 13.19 | 0.137 |
RKf0e_repeats_1.tbl | 10.00 | 20.00 | 31 | 12.78 | 1.297 | 27 | 13.62 | 2.210 |
RKf0c_repeats_1.tbl | 10.00 | 20.00 | 11 | 12.38 | 1.073 | 19 | 13.03 | 2.259 |
J_ba_repeats_1.tbl | 0.20 | 0.80 | 30 | 0.58 | 0.072 | 106 | 0.57 | 0.073 |
K_ba_repeats_1.tbl | 0.20 | 0.80 | 32 | 0.59 | 0.070 | 110 | 0.59 | 0.082 |
S_ba_repeats_1.tbl | 0.20 | 0.80 | 26 | 0.55 | 0.073 | 107 | 0.57 | 0.076 |
J20e_Jext_repeats_1. | 0.01 | 0.80 | 192 | 0.18 | 0.089 | 96 | 0.22 | 0.096 |
H20e_Hext_repeats_1. | 0.01 | 0.80 | 204 | 0.18 | 0.104 | 90 | 0.20 | 0.113 |
K20e_Kext_repeats_1. | 0.01 | 0.80 | 210 | 0.16 | 0.096 | 89 | 0.18 | 0.097 |
RkronE_repeats_1.tbl | 10.00 | 20.00 | 80 | 12.51 | 1.947 | 71 | 13.20 | 2.292 |
JkronE_repeats_1.tbl | 14.00 | 15.00 | 94 | 14.41 | 0.088 | 49 | 14.56 | 0.127 |
JkronE_repeats_1.tbl | 13.70 | 14.20 | 41 | 14.01 | 0.072 | 23 | 14.01 | 0.093 |
JkronE_repeats_1.tbl | 13.00 | 13.50 | 17 | 13.25 | 0.049 | 16 | 13.27 | 0.076 |
RkronC_repeats_1.tbl | 10.00 | 20.00 | 25 | 12.01 | 1.707 | 40 | 13.02 | 2.006 |
JkronC_repeats_1.tbl | 14.00 | 15.00 | 99 | 14.41 | 0.089 | 49 | 14.52 | 0.119 |
JkronC_repeats_1.tbl | 13.70 | 14.20 | 39 | 14.01 | 0.070 | 22 | 13.98 | 0.090 |
JkronC_repeats_1.tbl | 13.00 | 13.50 | 19 | 13.27 | 0.059 | 16 | 13.25 | 0.086 |
J20e_Jkron_repeats_1 | 0.01 | 0.50 | 174 | 0.08 | 0.043 | 92 | 0.11 | 0.050 |
H20e_Hkron_repeats_1 | 0.01 | 0.50 | 181 | 0.08 | 0.050 | 86 | 0.11 | 0.051 |
K20e_Kkron_repeats_1 | 0.01 | 0.50 | 175 | 0.08 | 0.061 | 80 | 0.11 | 0.064 |
-- | -- | -- | non-contaminated | ... | | | contaminated | ... | | |
---|---|---|---|---|---|---|---|---|
fname | mag- | mag+ | #r | #p | C | #r | #p | C |
J7_comp_1.tbl | 14.00 | 15.00 | 2518_2023 | 2676_2180 | 0.940_0.930 | 814_1269 | 969_1536 | 0.840_0.826 |
H7_comp_1.tbl | 13.70 | 14.20 | 1190_1075 | 1374_1193 | 0.870_0.900 | 452_658 | 518_795 | 0.873_0.828 |
K7_comp_1.tbl | 13.00 | 13.50 | 1415_1277 | 1398_1276 | 1.010_1.000 | 200_449 | 233_514 | 0.858_0.874 |
fname | val- | val+ | # | valbar | RMS | # | valbar | RMS |
J7_repeats_1.tbl | 14.00 | 15.00 | 118_93 | 14.450_14.470 | 0.068_0.069 | 35_52 | 14.580_14.480 | 0.093_0.076 |
H7_repeats_1.tbl | 13.70 | 14.20 | 53_51 | 13.950_13.970 | 0.104_0.105 | 18_25 | 14.040_13.940 | 0.118_0.110 |
K7_repeats_1.tbl | 13.00 | 13.50 | 75_62 | 13.230_13.240 | 0.092_0.095 | 10_18 | 13.220_13.240 | 0.094_0.098 |
Jf20e_repeats_1.tbl | 14.00 | 15.00 | 110_83 | 14.480_14.500 | 0.079_0.079 | 36_55 | 14.570_14.480 | 0.101_0.098 |
Hf20e_repeats_1.tbl | 13.70 | 14.20 | 52_44 | 13.940_13.970 | 0.098_0.105 | 14_24 | 14.040_13.950 | 0.111_0.122 |
Kf20e_repeats_1.tbl | 13.00 | 13.50 | 71_59 | 13.240_13.240 | 0.111_0.123 | 10_18 | 13.180_13.200 | 0.112_0.132 |
Jf20c_repeats_1.tbl | 14.00 | 15.00 | 113_83 | 14.440_14.470 | 0.072_0.075 | 38_58 | 14.600_14.460 | 0.117_0.089 |
Hf20c_repeats_1.tbl | 13.70 | 14.20 | 53_44 | 13.940_13.960 | 0.107_0.110 | 21_31 | 14.040_13.940 | 0.143_0.116 |
Kf20c_repeats_1.tbl | 13.00 | 13.50 | 71_55 | 13.230_13.240 | 0.101_0.113 | 12_22 | 13.190_13.210 | 0.137_0.130 |
RKf0e_repeats_1.tbl | 10.00 | 20.00 | 31_30 | 12.780_12.020 | 1.297_1.607 | 27_47 | 13.620_13.260 | 2.210_1.706 |
RKf0c_repeats_1.tbl | 10.00 | 20.00 | 11_9 | 12.380_12.420 | 1.073_1.452 | 19_35 | 13.030_12.690 | 2.259_1.632 |
J_ba_repeats_1.tbl | 0.20 | 0.80 | 30_28 | 0.580_0.490 | 0.072_0.061 | 106_75 | 0.570_0.550 | 0.073_0.075 |
K_ba_repeats_1.tbl | 0.20 | 0.80 | 32_30 | 0.590_0.520 | 0.070_0.068 | 110_84 | 0.590_0.570 | 0.082_0.096 |
S_ba_repeats_1.tbl | 0.20 | 0.80 | 26_27 | 0.550_0.470 | 0.073_0.054 | 107_77 | 0.570_0.550 | 0.076_0.061 |
J20e_Jext_repeats_1. | 0.01 | 0.80 | 192_89 | 0.180_0.320 | 0.089_0.115 | 96_104 | 0.220_0.350 | 0.096_0.114 |
H20e_Hext_repeats_1. | 0.01 | 0.80 | 204_76 | 0.180_0.310 | 0.104_0.119 | 90_83 | 0.200_0.320 | 0.113_0.119 |
K20e_Kext_repeats_1. | 0.01 | 0.80 | 210_49 | 0.160_0.290 | 0.096_0.116 | 89_52 | 0.180_0.270 | 0.097_0.106 |
A direct comparison between V2 photometry and the new V3 photometry can reveal potential problems, such as (1) systematics in the calibration, (2) background removal differences and (3) non-uniformities due to the new V3 methods (e.g., star removal). Star-removal non-uniformities are revealed by comparing the photometry across fields with different stellar number density. The first set of results will be separated according to the night (and hence, hardware and calibration period dependent).
M33 brings out the worst in GALWORKS. We detect the galaxy all right, but every piece of the galaxy. The chaff is extensive.
Two major changes to GALWORKS may significantly effect the disk usage. (1) GALWORKS V3 generates "coverage" maps; see Coverage Maps for some information. The image cubes are 6 planes deep, the first three planes are the GALWORKS masked areas and the last three planes are the PIXPHOT "coverage" maps. The images are 8-bits deep (i.e., short integers) to save space (they compress very efficiently). Here is an example of a GALWORKS coverage cube. The top three panels show the GALWORKS masking for J, H and Ks, respectively, of this Abell 3558 field (J-band coadd). The bottom three panels show the corresponding PIXPHOT coverage for J, H and Ks, respectively. The darkest grey scales correspond to a maximum coverage of 7. The typical coverage is 6. The lighter greyscales correspond to 5 and less coverages; (2) the galaxy postage stamp images are now 6 planes deep, the first three are nominal and the last three include star removal. Here is an example of a 3-color image showing the first three planes and the second three planes. Here is an example of a new postage stamp FITS header.
Coverage Maps
Gstamp Images: 1.5 to 2.5 Mb per scan * 70,000 scans == 105 to 175 Gb
We can expect about 120 Gb of compressed "coverage maps" from GALWORKS, assuming
a total of 70,000 scans. For galaxy stamps, we can expect between 100 and
200 Gb of compressed images. The low number corresponds to "typical" scans
(low density, field galaxies). The high number incorporates galaxy clusters
and fields full of nebulosity and complex structure (e.g., Orion). The actual
disk usage will fall somewhere between these two limits.
Low Density Fields
Abell 3558 Repeatibility from the OPS Testing Phase
Outstanding problems:
See OPS tests results below.
Report from Cong Xu:
I checked 2 most recently processed nights:
Abell 3558 Repeatibility from the OPS Testing Phase