Orbit Fit and Astrometric record for 19GH186

The following information shows the result of the orbit fit based on Gary Bernstein's method. Most of the information should be self-explanatory. Take special note that while the original Bernstein software works with barycentric coordinates, we convert these results into a heliocentric coordinate system.

# Object: 19GH186   
# Created Wed Nov 27 02:10:56 2024
# Orbit generated from Bernstein formalism
# Fitting     14 observations of     14
# Arc:  83.98d
# First observation: 2019/01/11
#  Last observation: 2019/04/05
Preliminary a, adot, b, bdot, g, gdot:
  -0.000001   0.017704  -0.000000   0.010352   0.022478   0.000000
# WARNING Fitting with energy constraint
# Chi-squared of fit:     3.42 DOF:     23 RMS:  0.09
# Min/Max residuals:    -0.15    0.17
# Exact a, adot, b, bdot, g, gdot:
  1.236130E-05  1.874067E-02  6.798830E-06  1.030279E-02  2.250534E-02 -2.157850E-03
# Covariance matrix:
  4.4164E-12  6.5018E-09  2.3613E-13  1.9456E-10  1.1598E-09  1.8895E-09
  6.5018E-09  1.0137E-05  3.6707E-10  3.0190E-07  1.8051E-06  2.3147E-06
  2.3613E-13  3.6707E-10  2.5733E-13  1.0353E-11  6.6325E-11  3.0302E-10
  1.9456E-10  3.0190E-07  1.0353E-11  9.6627E-09  5.5066E-08  3.6724E-07
  1.1598E-09  1.8051E-06  6.6325E-11  5.5066E-08  3.2402E-07  9.9941E-07
  1.8895E-09  2.3147E-06  3.0302E-10  3.6724E-07  9.9941E-07  1.3460E-04
#      lat0       lon0       xBary       yBary       zBary        JD0
   -6.445293  167.069864    0.825602   -0.061390   -0.544221  2458495.028731
# Heliocentric elements and errors
Epoch:              2458490.5000  =  2019/01/07
Mean Anomaly:          295.29457 +/-    72.356
Argument of Peri:       65.36383 +/-   107.682
Long of Asc Node:      177.45898 +/-     1.782
Inclination:            29.36272 +/-     3.827
Eccentricity:         0.12501935 +/-    0.5423
Semi-Major Axis:     46.84292649 +/-   10.0029
Time of Perihelion: 2479538.1050 +/-   22550.0
Perihelion:          40.98665418 +/-   26.8699
Aphelion:            52.69919881 +/-   27.7854
Period (y)              320.6079 +/-    102.69
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -43.38186411 +/-    1.0884
Ecliptic Y           10.79905143 +/-    0.2500
Ecliptic Z           -4.98763894 +/-    0.1262
Ecliptic XDOT        -0.00038513 +/-    0.0014
Ecliptic YDOT        -0.00225083 +/-    0.0004
Ecliptic ZDOT         0.00127471 +/-    0.0002
# Distances at JD0 (AU)
Heliocenter to KBO   44.98313226 +/-    1.0515
Geocenter to KBO     44.43390663 +/-    1.1239
# Hcoef:  8.52

The following table shows the complete astrometric record for 19GH186. The first three columns show the date of observation. The next six columns are RA and DEC. The next column (when provided) is the observed magnitude and filter. The next column is the object name (19GH186) followed by the observatory code and reference code for the source of the astrometry.

2019 01  11.52793  11 02 24.15   -00 50 00.5   24.5z 19GH186   T09  C~870l      
2019 01  11.54486  11 02 24.09   -00 50 00.3   25.1z 19GH186   T09  C~870l      
2019 01  11.57620  11 02 24.03   -00 50 00.0   24.8z 19GH186   T09  C~870l      
2019 01  11.61693  11 02 23.94   -00 49 59.6   24.5z 19GH186   T09  C~870l      
2019 01  11.61961  11 02 23.93   -00 49 59.3   24.9z 19GH186   T09  C~870l      
2019 01  11.66010  11 02 23.84   -00 49 59.0   25.0z 19GH186   T09  C~870l      
2019 04  04.39194  10 57 20.38   -00 12 34.1   25.9g 19GH186   T09  C~870l      
2019 04  04.41935  10 57 20.28   -00 12 33.1   25.4g 19GH186   T09  C~870l      
2019 04  04.42989  10 57 20.23   -00 12 32.7   25.5g 19GH186   T09  C~870l      
2019 04  05.42691  10 57 16.79   -00 12 00.2   25.0r 19GH186   T09  C~870l      
2019 04  05.43741  10 57 16.76   -00 12 00.0   25.1r 19GH186   T09  C~870l      
2019 04  05.46890  10 57 16.64   -00 11 59.0   24.8r 19GH186   T09  C~870l      
2019 04  05.47099  10 57 16.63   -00 11 58.8   25.1r 19GH186   T09  C~870l      
2019 04  05.50326  10 57 16.52   -00 11 58.0   25.3r 19GH186   T09  C~870l      

The following table shows the residuals to the orbit fit. The first coumn is the point number. The second column is the time, in years, measured from the first observation. The third and fifth columns are the regularized positions used in the orbit fit. The fourth and sixth columns are the residuals, in arc seconds, for RA and Dec respectively.

     1   0.0000      0.00     0.17       0.00     0.09
     2   0.0000     -0.91    -0.14      -0.16    -0.04
     3   0.0001     -1.85     0.02      -0.24    -0.04
     4   0.0002     -3.25     0.07      -0.39    -0.10
     5   0.0003     -3.51    -0.09      -0.17     0.12
     6   0.0004     -4.87    -0.02      -0.42    -0.04
     7   0.2269  -5071.97     0.12     303.48    -0.06
     8   0.2269  -5073.74     0.04     303.82     0.02
     9   0.2270  -5074.59    -0.15     303.90     0.00
    10   0.2297  -5134.79    -0.03     313.84     0.13
    11   0.2297  -5135.28     0.12     313.85     0.04
    12   0.2298  -5137.33    -0.01     314.07    -0.04
    13   0.2298  -5137.55    -0.10     314.20     0.06
    14   0.2299  -5139.38     0.03     314.30    -0.15

The following table comes from a 10My integration of the orbit of the object. Three columns are shown. The first column is the result of integrating the nominal orbit. The other two columns are based on clones of the nominal orbit that are +/- 3 sigma from the nominal orbit. If all three types agree then the classificiation is deemed secure. The basis for these calculations is described in more detail in AJ, 129, 1117 (2005). Any use made of these calculations should refer to and credit this publication and the Deep Ecliptic Survey Team.