VLA calibrator information for 0541-0541

This page summarizes the information for 0541-0541 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
 ===================================================================
 0541-056   J2000  A 05h41m38.083384s -05d41'49.428390"  Aug01         
 0539-057   B1950  A 05h39m10.994600s -05d43'15.028000"
 -----------------------------------------------------
 BAND        A B C D    FLUX(Jy)    UVMIN(kL)  UVMAX(kL)
 =====================================================
  20cm    L  S S S S       1.05
   6cm    C  P P P P       1.25
 3.7cm    X  P P P P       0.98
   2cm    U  P P P P       1.30
 0.7cm    Q  W W W W       0.7

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)
201907260.839J0541-0541
201909111.065J0541-0541
S-band data (filled triangles)
201712151.011J0541-0541
C-band data (open squares)
202101180.587J0541-0541
202109290.653J0541-0541
202204150.617J0541-0541
202207010.755J0541-0541
202207020.751J0541-0541
X-band data (X-crosses)
201802251.894J0541-0541
201802252.466J0541-0541
201803210.881J0541-0541
202101040.601J0541-0541
202101150.504J0541-0541
202203160.650J0541-0541
U-band data (filled squares)
202012280.505J0541-0541
202203310.770J0541-0541
202204020.795J0541-0541
202303140.506J0541-0541
202304020.565J0541-0541
202304170.520J0541-0541
K-band data (open circles)
201706110.297J0541-0541
201708170.582J0541-0541
201809100.432J0541-0541
201809130.429J0541-0541
201809140.420J0541-0541
201809150.403J0541-0541
201809160.415J0541-0541
201809170.457J0541-0541
201809180.472J0541-0541
201809210.442J0541-0541
201809230.442J0541-0541
201809240.452J0541-0541
201810020.419J0541-0541
201810040.417J0541-0541
201810050.447J0541-0541
201810060.482J0541-0541
201810080.487J0541-0541
201810250.466J0541-0541
201811300.618J0541-0541
201903110.452J0541-0541
201903230.481J0541-0541
201903300.432J0541-0541
201904200.444J0541-0541
201904230.450J0541-0541
201906090.390J0541-0541
201906110.377J0541-0541
201906160.407J0541-0541
201906230.401J0541-0541
201907150.414J0541-0541
201907200.382J0541-0541
202203150.753J0541-0541
A-band data (6-pointed stars)
201708170.458J0541-0541
202012270.411J0541-0541
202101030.462J0541-0541
202101050.481J0541-0541
202101120.447J0541-0541
Q-band data (filled circles)
201708170.434J0541-0541
201811270.549J0541-0541
201811270.531J0541-0541
201811280.504J0541-0541
202102070.435J0541-0541
202102240.461J0541-0541
202110040.504J0541-0541
202110110.518J0541-0541
202110210.539J0541-0541
202208140.539J0541-0541