VI. Analysis of the 2MASS Second Incremental Release Catalogs


1. Comparison of Achieved Performance of Second Incremental Release Catalogs with Level 1 Science Specification

m. 2MASS Seasonal Effects

This page is frequently revised, so the reader is strongly encouraged to consult the online version of the Explanatory Supplement for updates. The figures below are based upon the calibrator scans from the full production processing. All dates are given by Survey Night Number. The following table may help translate Night Number to calendar dates.

Night NumberDateNotes
1001997 June 8 
1541997 August 1Monsoon Start
1871997 August 31Monsoon End
2501997 November 5 
3001997 December 25 
3841998 March 19CTIO Start
4501998 May 24 
5071998 July 20Monsoon Start
5651998 September 16Monsoon End
6021998 October 23Leach Electronics at Hopkins
7001999 January 29 
7291999 February 27Leach Electronics at CTIO
8721999 July 20Monsoon Start
9271999 September 13Monsoon End
10372000 January 1Y2K
12442000 July 26Monsoon Start
12932000 September 13Monsoon End

Nightly Averages

Average Backgrounds: The backgrounds, shown in Figures 1 and 2, are such that the Ks background, presumably dominated by the thermal contribution, is highest in the summer -- as a result, the airglow-dominated H background was worse than Ks in the winter. Starting with 1999 September, H background data have been multiplied by 1.3 to (roughly) account for the decreased sensitivity of the new array.

Figure 1Figure 2

Average FWHM: As shown in Figures 3 and 4, our best images in the north are about 2.7´´-2.8´´ FWHM. The southern seeing values are better. It appears that the telescope adjustments in early 1998 September improved the image quality in the north, but over time these improvements were lost. The 1999 September adjustments resulted in better images than ever seen before in the north. The better images have been sustained through the winter and summer of 2000.

Figure 3Figure 4

Average Limiting Magnitude: The signal-to-noise ratio (S/N) for faint stars depends upon both the background and the "seeing". The Level 1 specifications for 2MASS limiting magnitudes at S/N=10 are 14.3 mag at Ks, 15.1 mag at H, and 15.8 mag at J. The actual limiting magnitudes are shown in Figures 5 and 6. Since the calibrator fields are observed six times consecutively, the observed scatter gives a measure of the S/N. R. Cutri has found that the limiting magnitude can be parameterized in terms of the backgrounds and seeing, and this parameterization is one of the factors used to grade the quality of science scans. The figures below are based upon the parameterization, transformed into the magnitude at which S/N=10 is achieved. We have rederived new relations for the southern camera and the new northern H array, and these relations are now used in these figures.

Figure 5Figure 6

Average 2nd Image Moment Ratio: Figures 7 and 8 have been updated to use the new elongation statistic, for which elongation appears as values<1.0. For some nights, only the old "Second Image Moment ratio" was available. In this case, we plot any values >1.0 as 1/old_statistic. This will underestimate the elongation, as is obvious in the southern plots (nights 520-580) where the elongation is along position angle 45°. Note the bad data from the northern summers, particularly 1997. At high temperatures, J,H and Ks cannot be focused at the same time, resulting in worse Ks second image moment ratios in September and June.

Figure 7Figure 8

Zero-Points: The zero-point, shown in Figures 9 and 10, measures the relationship between flux and camera counts (DN). More positive zero-points are more sensitive, in the sense that there are more counts for a given flux. The J zero-point varies more strongly than H or Ks. This is no surprise, as the J zero-point often varies during the course of a night. The huge jump at CTIO night 729 can be attributed to the change in electronics, since the gain was expected to change. Also, the mirror was cleaned at that point, which may also have helped. The jump at CTIO night 685 is due to the camera window being cleaned. The recent zero-point improvements at night 1124 (000325n) and 1129 (000402s) coincide with mirror cleanings. Note that CTIO has just returned to normal zero-points.

Figure 9Figure 10

[Last updated 2000 Sep 20 by J. Gizis. Modified 2000 Sep 21 by S. Van Dyk.]


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