Flux Density Calibration

Accurate Flux Density Bootstrapping

Introduction

Because of source variability, it is impossible to compile an accurate listing of flux densities for most VLA calibrators. The values given in Chapter 4 of this manual are only approximate. We strongly recommend bootstrapping the flux density of a calibrator by comparing the calibrator observations with one or several observations of 3C286, 3C48 or 3C147. Careful observations have allowed the following set of rules to be established for accurate bootstrapping of flux densities using 3C286, 3C48 or 3C147.

3C286 is partially resolved to most combinations of configuration and band. Its resolution occurs on two different scales - there is a weak secondary located 2.5" from the core, and the core itself is partially resolved on longer baselines. Nevertheless, 3C286 can be used as a flux calibrator for all VLA observations providing the rules laid down below are followed.

3C48 and 3C147 are heavily resolved to some combinations of configuration and frequency and exhibit some variability on timescales of months to years (see section 2.2), but nevertheless may be preferable as a flux calibrator over 3C286 since they contain no extended structure on scales greater than 1".

When 3C48, 3C147 and 3C286 can be used directly

The following combinations of array configuration and band have no restrictions in number of antennas or UV range:

3C48/3C147 90cm All configurations
20cm C and D configurations
6 cm D configuration
3.6 cm D configuration
3C286 90cm B, C, D configurations
20cm C and D configurations
6 cm D configuration
2 cm D configuration
1.3cm D configuration

 

When 3C48 and 3C147 require a model

The following combinations of configuration and band should not be calibrated with 3C48 or 3C147 without supplying a good model.

2 cm A configuration
1.3 cm A configuration
0.7 cm A, B configurations

Some FITS format images, along with clean component models for 3C48 and 3C286 can be found at

http://www.aoc.nrao.edu/~cchandle/cal/cal.html.

or

http://www.aoc.nrao.edu/~smyers/calibration/

(look for the latest links therein).

If a model is used then no (u,v) restrictions or limitations on the number of antennas are needed. Note that it is still necessary to run SETJY on the primary flux density calibrator even when supplying a model to CALIB.

When special restrictions are necessary for flux calibration

The following rules must be carefully followed to ensure proper flux bootstrapping in the combinations of array scale and band noted below. For the hybrid configurations (BnA, CnB, DnC) the rule for the more compact configuration should be adopted (i.e. follow B config rules for BnA). When specifying inner antennas to be used for the calibration solution, no antenna on the North arm further out than on the East or West arms should be used. Finally, it is a good idea to set WTUV = 0.1 in CALIB to ensure a stable solution.

Source

Band

(cm)

uvrange

k lambda

config

number of inner

antennas per arm

Notes
3C48/3C147 90 0-40 All All
3C48/3C147 20 0-40 A 7
0-40 B,C,D All
3C48/3C147 6 0-40 A 3
0-40 B,C,D All
3C48/3C147 3,6 0-40 A 2
0-40 B 6
0-40 C,D All
3C48/3C147 2 0-60 A 1 Not recommended
0-60 B 5
0-60 C,D All
3C48/3C147 1.3 0-80 A 1 Not recommended
0-80 B 5
0-80 C,D All
3C48/3C147 0.7 0-100 A 1,* Not recommended
0-100 B 3,* See note below
0-100 C,D All,* See note below

 

Source

band

(cm)

uvrange

k lambda

Config

Number of Inner

Antennas per arm

Notes
3C286 90 0-18 A 7
0-18 B,C,D All
3C286 20 0-18 A 4
0-18 B,C,D All
90-180 A All Reduce flux by 6%
3C286 6 0-25 A 1 Not recommended
0-25 B 4
0-25 C,D All
150-300 A All Reduce flux by 2%
3C286 3.6 50-300 A 3 Reduce flux by 1%
50-300 B 7 Reduce flux by 1%
50-300 C All Reduce flux by 1%
0-15 D All
3C286 2 0-150 A 3
0-150 B,C,D All
3C286 1.3 0-185 A 2
0-185 B 7
0-185 C,D All
3C286 0.7 0-300 A 2,* See note below
0-300 B 6,* See note below
0-300 C,D All

* NOTE: We are also investigating additional sources that may be suitable as primary flux density calibrators 1.3 and 0.7 cm. The latest information concerning absolute flux calibration at 0.7 cm can be found in the relevant section of the VLA Guide to Observing.

Due to its (u,v) restrictions, low flux density, and evidence suggesting that 3C48 is variable at this wavelength, it is not recommended for flux calibration at 0.7 cm.

If one were to ignore the guidelines, and blindly calibrate the data on the basis of the available data, the flux error obtained would vary according roughly to how much resolution occurs but would not exceed 5% for 3C286. Bear in mind that there will occur a differential error as well, as the antennas at the ends of the array will be over-calibrated with respect to those at the center. If these guidelines are followed, the bootstrap accuracy should be 1 or 2 percent at 20, 6, and 3.6 cm, and perhaps 3 to 5 percent at 2, 1.3 and 0.7 cm. At 2cm and 1.3cm bands, other effects, such as dish efficiency, pointing and atmospheric absorption (1.3cm and 0.7cm) are probably more important.

Elevation-dependent gain corrections

At frequencies of 15 GHz and above, there are appreciable changes in the antenna gains as a function of elevation. Atmospheric opacity, especially at 22 GHz, also introduces an elevation-dependence on the observed visibility amplitudes. By calibrating the target source with a nearby calibrator, much of these variations can be removed. However, if the primary flux calibrator (e.g. 3C286) is observed at a different elevation from the secondary gain and phase calibrator, then the flux bootstrapping will be in error. Proper calibration of the flux densities at high frequencies requires knowledge of a gain curve for the antennas, and the atmospheric opacity as well. Software has been developed in AIPS to address these issues (see the task ELINT). If you don't have enough data to make your own gain curve, you can find gain curves at http://www.aoc.nrao.edu/~smyers/calibration/.

Monitoring of Flux Density Calibrators

Since the planet Mars and 3C295 are too heavily resolved for most VLA observing programs, the flux density of a small set of calibrators is carefully measured with respect to 3C295 and Mars in the 'D' configuration every few years. These more compact sources have been found to be only slowly variable (with some exceptions at the highest frequencies). Below we provide the current (1999.2) best analytic expression for their flux densities.

[display]{\rm Log}\: S = A + B \times {\rm Log}\: \nu + C \times ({\rm Log}\: \nu)^2 + D \times ({\rm Log}\: \nu)^3[/display]

 

where S is the flux density in Jy and v is the frequency in GHz. These expressions are valid between 300 MHz and 50 GHz.

 

SourceABCD
3C48 1.31752 -0.74090 -0.16708 +0.01525
3C138 1.00761 -0.55629 -0.11134 -0.01460
3C147 1.44856 -0.67252 -0.21124 +0.04077
3C286 1.23734 -0.43276 -0.14223 +0.00345
3C295 1.46744 -0.77350 -0.25912 +0.00752

 

The 31DEC99 version (with the proper patch installed) of AIPS program SETJY with OPTYP = 'CALC' will calculate and insert the flux densities based on the above expression and parameters into a VLA database. Alternatively SETJY can be told to use the old Baars et al (1977) expression and parameters (see previous section), or the 1995.2, or 1990 coefficients. AIPS Versions 15OCT89 through 15JAN96 use the 1989.9 coefficients or the Baars coefficients. With versions of AIPS prior to 15OCT89 the flux density of the calibrators must be set with OPTYP = ' ' for each IF. Do not use SETJY with optype 'CALC' if you are switching frequencies within the observing run. In this case you must calculate and insert the appropriate values for each frequency and IF with OPTYP = ' '. You may find it more convenient to split the databases into single FQid components.

Observations taken prior to 1990 may benefit from using the adjustments below when setting the flux density of 3C48, 3C147 or 3C286. Below are listed the RATIOS between the true and Baars et al. value for 3C48, 3C147 and 3C286 at the various frequency bands from 1983 to 1995. Multiply the Baars et al. value by this ratio to obtain the correct flux density. Contact R. Perley or G. Taylor if you need more information.

1983.51985.5
L C L C U
3C48 1.004 1.039 1.018 1.047 1.11
3C147 0.974 0.957 0.970 0.948 0.99
3C286 0.995 1.010 0.993 1.002 0.99

 

19871989.9
P L C X U L C X U
3C48 0.95 1.02 1.04 1.06 1.10 1.019 1.043 1.049 1.076
3C147 1.00 0.97 0.95 0.97 1.01 0.975 0.951 0.949 0.993
3C286 0.95 1.00 1.01 1.01 1.02 0.999 1.005 0.995 0.991

 

1995.21999.2
P L C X U P L C X U
3C48 0.948 1.017 1.023 1.034 1.034 0.966 1.016 1.008 1.009 1.004
3C147 0.990 0.983 0.974 0.999 1.046 0.998 0.984 0.987 0.975 1.002
3C286 0.971 0.999 1.008 1.006 0.988 0.967 0.999 1.008 1.007 0.989

The Flux Density Scale Used at the VLA

The flux density scale used by CASA and AIPS between 1 and 50 GHz is based on the Perley-Butler scale (ApJS, vol 204, 19, 2013). In turn, this scale is based on the absolute Wilkinson Microwave Anisotropy Probe (WMAP) measurements of the brightness of the planet Mars. The corresponding flux densities of Mars were then transferred to four stable calibrator sources (3C123, 3C196, 3C286 and 3C295) through careful VLA measurements of their ratios to Mars spanning more than one decade. The new scale is very close to the traditional Baars et al. (1977 Astron. Astrophys., 61, 99) scale between 1 and 15 GHz.

Below 1 GHz, AIPS and CASA have adopted the 'Scaife and Heald' scale. The VLA has made careful measurements of the ratios of a small set of standard calibrators to Cygnus A, whose absolute flux density is believed to be known to within ~3%.  Early results suggest the 'Scaife and Heald' scale is consistent with the known flux density of Cygnus A between 220 and 480 MHz.

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