Photo Object Lists

1. File Naming Conventions

The principal output of the photometric pipeline (photo) is a list of detected objects with parameters in 5 bands. These outputs, expressed in instrumental units, are stored in files with the naming convention

o_0311.fit

where the prefix o is short for objc (the SDSS nomenclature for a detected object) and 0311 is the field number within a particular run and scanline. Calibrated versions of these files are stored in files with the naming convention

t_0311.fit

where the prefix t is short for tsObjc (the SDSS nomenclature for a calibrated object used by target selection algorithms). The astrometric and photometric conventions are described in data.htm: positions are for equinox J2000, and magnitudes are on the AB sytem.

For convenience of users, a subset of the outputs in this file are written out in plain ascii text in the files with the naming convention

t_0311.txt.

Several fields in the outputs contain flags. These are described briefly here, but for a fuller description, see document flags.htm and t.htm.



2. Description

The photometric pipeline processes 5 frames (one for each filter) per field simultaneously. An object detected in at least one frame is measured in all other frames, even if just to establish upper limits.

The first set of outputs describe the object as a whole:

The next set of outputs are reported for each band.




3. Petrosian Quantities

Let I(r) be (a spline fit to or other smooth representation of) the measured azimuthally averaged surface brightness of an object in r'.

The profMean profile will be used. The profile used for calculating Petrosian quantities is cutoff at the first radial bin for which the S/N is below 1.0. To avoid the necessity of interpolating to determine fluxes, the actual radial profile will be recorded out to the adopted Petrosian radius.


Define the Petrosian ratio RP(r) as the ratio of the local surface brightness at radius r to the mean within r:

Petrosian radius

Mark all the radii ri, i = 1,..., N where RP falls to a specified value f1, and for which I(r) > f2.

If there is at least one such radius (N > 0), the largest of the ri will be taken as the Petrosian radius rP; If no such radius exists, there are two possibilities: that the lowest surface brightness in the object is above a specified value f3 (in which case we adopt rP = rmax}, the largest "good" radius in the profile), or that the highest surface brightness is below f3 (in which case we take rP = f5).

The Petrosian flux FP is defined as the total flux as measured within a certain number of Petrosian radii:

Petrosian flux

The Petrosian half-light r50 is defined by the implicit equation:

Petrosian half-light  radius

The Petrosian 90% radius is defined by the implicit equation:

Petrosian 90% radius

The adjustable parameters used for the data sets on the CD-ROM are:

f1Petrosian Ratio0.25
f2Minimum Surface Brightness at rP26.7
f3Fallback surface brightness25.7
f4Multiple of rP for Petrosian flux3
f5Fallback Radius3"