VLA calibrator information for 1035+5628

This page summarizes the information for 1035+5628 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
 ===================================================================
 1035+564   J2000  A 10h35m07.0399s    56d28'46.792"
 1031+567   B1950  A 10h31m55.9547s    56d44'18.174"
 -----------------------------------------------------
 BAND        A B C D    FLUX(Jy)    UVMIN(kL)  UVMAX(kL)
 =====================================================
  20cm    L  P P P S       1.85
   6cm    C  P P P P       1.22
 3.7cm    X  S P P P       0.80                      400
   2cm    U  S S S S       0.40
 0.7cm    Q  W W W W       0.11

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

WARNING: multiple positions found, using first one 158.7792917 +56.4796639 158.7793329 +56.4796644 Results from CASA pipeline flux density mining:
Observing date (UT)Flux density (Jy/bm)Source name used
C-band data (open squares)
201709040.976J1035+5628
X-band data (X-crosses)
201709040.602J1035+5628
201705291.818J1035+5628
201706041.799J1035+5628
201706041.802J1035+5628
201706051.786J1035+5628
201706071.865J1035+5628
201706111.837J1035+5628
201706111.826J1035+5628
201706111.816J1035+5628
201706121.819J1035+5628
201706171.797J1035+5628
201706191.801J1035+5628
201706221.8191035+564
201706241.778J1035+5628
201707031.805J1035+5628
201707041.790J1035+5628
201707061.823J1035+5628
201707081.809J1035+5628
201707151.799J1035+5628
201707151.811J1035+5628
201707161.807J1035+5628
201707171.813J1035+5628
201707181.810J1035+5628
201707201.793J1035+5628
201707231.801J1035+5628
201707311.794J1035+5628
201708011.801J1035+5628
201708031.794J1035+5628
201708051.799J1035+5628
201708071.793J1035+5628
201708071.792J1035+5628
201709181.826J1035+5628
201709291.792J1035+5628
201709291.785J1035+5628
201710071.787J1035+5628
201710131.792J1035+5628
201801021.804J1035+5628
201801041.799J1035+5628
201801111.796J1035+5628
201801121.788J1035+5628
201801271.766J1035+5628
201802191.771J1035+5628
201802261.762J1035+5628
201802281.783J1035+5628
201803201.777J1035+5628
201804161.778J1035+5628
201804161.776J1035+5628
201805021.797J1035+5628
201805021.784J1035+5628
201809152.478J1035+5628
201809171.779J1035+5628
201810252.077J1035+5628
201902261.785J1035+5628
201903271.792J1035+5628
201904261.901J1035+5628
201905061.794J1035+5628
201905111.791J1035+5628
201905121.804J1035+5628
201905131.811J1035+5628
201907231.786J1035+5628
201908101.744J1035+5628
201908311.785J1035+5628
201909081.784J1035+5628
201909101.806J1035+5628
202111211.812J1035+5628
202305211.781J1035+5628
201706221.5261035+564
201708201.477J1035+5628
201709181.516J1035+5628
201709221.490J1035+5628
201709231.500J1035+5628
201709261.515J1035+5628
201710061.514J1035+5628
201711271.523J1035+5628
201811181.510J1035+5628
201901031.506J1035+5628
201901201.506J1035+5628
201901301.507J1035+5628
201902091.508J1035+5628
201902171.517J1035+5628
201902191.517J1035+5628
201902191.521J1035+5628
201904271.520J1035+5628
201907231.509J1035+5628
201909101.535J1035+5628
201709021.009J1035+5628
201711140.995J1035+5628
201801030.913J1035+5628
201801230.982J1035+5628
201803210.985J1035+5628
201804010.878J1035+5628
201805141.000J1035+5628
201809210.964J1035+5628
201809270.989J1035+5628
201811170.945J1035+5628
201902280.948J1035+5628
201903080.953J1035+5628
201903230.976J1035+5628
201904230.939J1035+5628
201907231.015J1035+5628
201908030.937J1035+5628
201909081.057J1035+5628
201909151.018J1035+5628
201909240.994J1035+5628
201910200.919J1035+5628
201910210.928J1035+5628
201910210.934J1035+5628
201910210.940J1035+5628
201910210.960J1035+5628
202103220.991J1035+5628
202206220.985J1035+5628
202206270.993J1035+5628
202208090.981J1035+5628
201711040.562J1035+5628
201907230.628J1035+5628
201908290.540J1035+5628
202006260.581J1035+5628
202103250.608J1035+5628
202104040.615J1035+5628
202104100.614J1035+5628
202104200.612J1035+5628
202104210.640J1035+5628
202104240.612J1035+5628
202104260.627J1035+5628
202106220.610J1035+5628
202108160.605J1035+5628
202203040.536J1035+5628
202203060.623J1035+5628
U-band data (filled squares)
201705310.401J1035+5628
201706110.400J1035+5628
201801230.394J1035+5628
201811180.404J1035+5628
202203060.391J1035+5628
202206100.388J1035+5628
K-band data (open circles)
201706170.256J1035+5628
202204220.253J1035+5628_cal