The tuning of the active deblending parameters is discussed in the Ken Marsh's page. Figures presented here provide some statistical results on active deblending. Figures 1 to 5 contains all scans from the night 971116n.
I. Analysis
a. Initial chi2, improved chi2:
Figure 1 is a color-magnitude diagram obtained for actively deblended
sources. The Y axis corresponds to a reconstruction of the original magnitude
by adding the flux of the deblended components. These two figures are generated
for a different chi2 minimum improvement (dchi) during the deblending
process.
For Figure
1a and Figure
1b, dchi=0.5 and dchi=1.0, respectively. Diamonds correspond to successful
deblends, crosses to inconsistent deblends. The inconsistency refers
to the case when the secondary source for each band cannot be cross-identified
by the bandmerge process.
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| Figure 1a | Figure 1b |
Figure 2a represent deblended H-Ks vs the
initial chi2 (before deblending) for sources with dchi=0.5. It shows that
inconsistent deblends (crosses) occur for all chi2 values.
Figure
2b gives the dchi distribution of the successfully deblended sources.
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| Figure 2a | Figure 2b |
The optimal value for the dchi parameter is derived from the Figure
3. Between dchi=0.5 to 1.0 the fraction successful deblends increase
to 88% to 94% and remains at this fraction for larger dchi.
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| Figure 3 |
b. Color-color diagrams:
Color-color diagrams are shown in Figures 4:
4a) version 2 of the pipeline, before
the active deblending implementation, for sources that corresponds to Figure
4c. Extremely blue objects were identified as the result of an inadequate
design of the passive deblending algorithm in Ks (see Laurent's
page).
4b) version 3 of the pipeline, dchi=0.5,
successful deblends only.
4c) dchi=1.0, successful deblends only.
One sigma error bars are indicated for objects far from the normal main
sequence star locus.
4d) version 3 with the active deblending
turned OFF for sources corresponding to those represented in Figure 4c.
Extremely blue objects of the v2 pipeline (Figure 4a) do not exist in the
v3 pipeline with improved PSFs.
4e) version 3 with the active
deblending turned ON but with remerged magnitudes by adding fluxes from
each deblended component.
4f) version 3 for sources actively deblended
in less than 3 bands. For non-deblended bands, the large aperture photometry
gives the upper limit.
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| Figure 4a | Figure 4b | Figure 4c |
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| Figure 4d | Figure 4e | Figure 4f |
Figure 5 represents the density color-color
diagram for deblended sources (same as Figure 4c) and non-deblended sources
(i.e. blend flag = 1 in all bands). Contours are normalized to the number
of objects in each plot and begin at a value of 2 with a step of 2 (units
are arbitrary). The lowest contour is in agreement for the two plots but
the maxima are 21 and 9 for the deblended and non-deblended sources, respectively.
The statistic for the deblended sources is still low (1228 objects) but
this figure suggests that the stellar population is different with an excess
of sources around J-H=0.2 H-K=0.05 that would correspond to F5 type stars.
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| Figure 5 |
c. Relative numbers of deblended sources
Figures 6 (dchi=1.0) compare the number of deblended sources (active
successful, active inconsistent, passive) with the total number of deblended
source in JHKs simultaneously (6a), the total number of sources (6b), the
total number of sources deblended in at least one band (6c). Figures 6d
give the fraction of deblended sources with respect to the total number
of sources in a scan.
Each point corresponds to a science scan, 6 full nights are
used in these figures (971116n, 980319s, 980403n, 990523n, 990723s, 990923s)
which cover fields from high Galactic latitudes to the Baade's window close
to the Galactic center.
Plots generated with the new version of the pipeline (April, 5th :
new nl.prophot? parms and new galworks with fits header fix).
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| Figure 6a | Figure 6b | Figure 6c | Figure 6d |
II. Optimized version of prophot (4/20/01)
Figure 7a is the new version of Figure
4c (same night: 971116n). Figures 7b and 7c are for the primary and
secondary components and the active deblending, respectively. Figures 7d
and 7e are for the 6 nights (971116n, 980319s, 980403n, 990523n, 990723s,
990923s) and include very high density fields.
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| Figure 7a | Figure 7b | Figure 7c |
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| Figure 7d | Figure 7e |
Number of deblended sources for two different versions of prophot (night 971116n):
| Date | march, 28 | april, 20 |
| Active | 1865 | 180 |
| Passive | 383 | 399 |
The evolution of color-color diagrams for different delta(mag) between
the primary and the secondary components, or for different separation distances
between the two components is represented in these two animations:
delta(mag),
distance
separation.
6 nights are used (971116n, 980319s, 980403n, 990523n, 990723s, 990923s).
Figures 8 are the new version of figures 6. The number of active deblends
has strongly decreased and is now close to the number of passive deblends.
Arcs for low density fields (N<1000 stars/scan) in Figure 8d are hyperbolae
that correspond to a small integer number of deblends.
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| Figure 8a | Figure 8b | Figure 8c | Figure 8d |