VLA calibrator information for 0059+0006

This page summarizes the information for 0059+0006 as found in the original VLA calibrator list and, if found there, a link to search the NRAO VLA Archive Survey (NVAS) for calibrator data before 2010. Furthermore, a table with the most recent approximate flux densities, starting from 2017 as mined from the VLA CASA pipeline is presented.

If shown at the top, we have recovered the original, pre-WIDAR ANTSOL flux density solutions from the period roughly 2000-2007; symbols as explained next.
The mined data are plotted (gray, on the left hand side) as function of (log) frequency on the top and as function of time on the bottom. The frequency band symbols in the bottom panel follow the symbols as outlined in the top panel:

4-band  (~75 MHz) horizontal stripe       X-band (~10.0 GHz) cross
P-band (~350 MHz) open triangle        U/Ku-band (~15.0 GHz) filled square
L-band (~1.5 GHz) VLA-Y shape             K-band (~22.2 GHz) open circle
S-band (~3.0 GHz) filled triangle      A/Ka-band (~33.2 GHz) 6-pointed star
C-band (~6.0 GHz) open square             Q-band (~45.0 GHz) filled circle
Assume a 10% flux density error on each point, up to 30% for the higher frequency data points. The dashed lines in the frequency plot indicate the approximate spectral index in the frequency band (tied to the measured flux density).
Depending on the spectral behavior, different receiver observing bands (as indicated with the log-frequency axis) may have very different typical flux densities. Note that there can be significant flux density changes for different array configurations, which start date is indicated at the top of the time-line figure. Calendar years are separated by vertical dotted lines.
If shown, a curve depicts a fit to the (unweighted) average data for each band (if there are more than two bands with measured flux densities). The fit equation is listed at the top where the x-coordinate represents the base-10 log of the frequency (GHz) and the y-coordinate represents the base-10 log of the flux density (mJy/bm). The fit may use more data than shown and is using data with different time stamps, which means typically different flux densitities in a single band for genuine variable sources (and/or observed in different array configurations).
Depending on the variability of the source, array configuration and the quality of the data, this fit may, or may not, be representative for the data!

(Click on the figure for a larger view in a new tab/window)

Original (outdated) VLA calibrator list information:
 IAU NAME EQUINOX  PC RA(hh,mm,ss)    DEC(ddd,mm,ss)   POS.REF ALT.NAME
 ===================================================================
 0059+001   J2000  A 00h59m05.514924s  00d06'51.621710"  Aug01         
 0056-001   B1950  A 00h56m31.756700s -00d09'18.826000"
 -----------------------------------------------------
 BAND        A B C D    FLUX(Jy)    UVMIN(kL)  UVMAX(kL)
 =====================================================
  20cm    L  P P P P       2.50
   6cm    C  S P P P       1.35                      200
 3.7cm    X  X S P P       0.96                      200
   2cm    U  X X S S       0.70                      200
 0.7cm    Q  W W W W       0.42

Default NVAS search around this position (in new tab/window)

Results from CASA pipeline flux density mining:
Observing date (UT)Flux density (Jy/bm)Source name used
L-band data ("VLA Y-arm" symbols)
201706062.421J0059+0006
201706072.432J0059+0006
201706122.405J0059+0006
201706212.419J0059+0006
201706242.401J0059+0006
201707072.393J0059+0006
201707112.381J0059+0006
201707112.406J0059+0006
201707122.392J0059+0006
201707142.444J0059+0006
201707182.411J0059+0006
201707182.402J0059+0006
201707212.414J0059+0006
201707212.481J0059+0006
201707212.417J0059+0006
201707222.513J0059+0006
201707222.428J0059+0006
201707232.400J0059+0006
201707232.521J0059+0006
201707232.420J0059+0006
201707242.423J0059+0006
201707272.402J0059+0006
201707272.419J0059+0006
201707282.410J0059+0006
201707282.443J0059+0006
201707282.438J0059+0006
201707302.438J0059+0006
201707312.427J0059+0006
201708052.430J0059+0006
201708072.402J0059+0006
201708072.423J0059+0006
201708092.372J0059+0006
201708112.415J0059+0006
201708142.408J0059+0006
201708142.419J0059+0006
201708152.423J0059+0006
201708182.401J0059+0006
201708192.409J0059+0006
201708192.409J0059+0006
201708202.409J0059+0006
201708202.389J0059+0006
201708212.417J0059+0006
201708212.408J0059+0006
201708212.448J0059+0006
201708222.399J0059+0006
201708222.403J0059+0006
201708222.441J0059+0006
201708232.446J0059+0006
201708232.410J0059+0006
201708232.447J0059+0006
201708242.390J0059+0006
201708252.423J0059+0006
201708252.422J0059+0006
201708252.455J0059+0006
201708262.374J0059+0006
201708272.417J0059+0006
201708282.581J0059+0006
201708282.417J0059+0006
201708282.435J0059+0006
201904062.255J0059+0006
201904122.351J0059+0006
201905042.3130059+001cal
201905102.4510059+001cal
201905112.3460059+001cal
201905172.3270059+001cal
201909112.293J0059+0006
201909142.467J0059+0006
202201292.350J0059+0006
S-band data (filled triangles)
201706244.135J0059+0006
201811171.716J0059+0006
2018121717.588J0059+0006
201901021.665J0059+0006
K-band data (open circles)
201812060.602J0059+0006