Orbit Fit and Astrometric record for 13SK106

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: 13SK106   
# Created Thu Apr 25 01:15:03 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     36 observations of     36
# Arc:  16.25y
# First observation: 2000/08/28
#  Last observation: 2016/11/26
# Chi-squared of fit:     7.01 DOF:     66 RMS:  0.08
# Min/Max residuals:    -0.18    0.18
# Exact a, adot, b, bdot, g, gdot:
  1.543408E-05  2.255047E-02 -1.167414E-08  2.495484E-04  2.343387E-02  1.290209E-07
# Covariance matrix:
  7.3419E-13 -1.0135E-13  1.3342E-15 -6.6293E-16 -5.6031E-14 -1.4721E-13
 -1.0135E-13  3.7381E-14 -7.4148E-16  3.6542E-16  5.0165E-14  8.2372E-14
  1.3342E-15 -7.4148E-16  6.2381E-13 -4.1677E-14 -8.6340E-16 -1.8053E-15
 -6.6293E-16  3.6542E-16 -4.1677E-14  2.9643E-15  4.0127E-16  8.9313E-16
 -5.6031E-14  5.0165E-14 -8.6340E-16  4.0127E-16  2.1170E-13  1.0040E-13
 -1.4721E-13  8.2372E-14 -1.8053E-15  8.9313E-16  1.0040E-13  1.9991E-13
#      lat0       lon0       xBary       yBary       zBary        JD0
   -1.002110   -7.809090    0.298888   -0.016968   -0.961314  2451784.795313
# Heliocentric elements and errors
Epoch:              2451784.5000  =  2000/08/28
Mean Anomaly:          340.85535 +/-     0.042
Argument of Peri:      322.86630 +/-     0.045
Long of Asc Node:       49.19924 +/-     0.005
Inclination:             1.16323 +/-     0.000
Eccentricity:         0.02882557 +/-    0.0001
Semi-Major Axis:     44.85791052 +/-    0.0032
Time of Perihelion: 2457620.3195 +/-      17.1
Perihelion:          43.56485553 +/-    0.0039
Aphelion:            46.15096552 +/-    0.0040
Period (y)              300.4462 +/-      0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           43.18869799 +/-    0.0008
Ecliptic Y           -6.21901262 +/-    0.0001
Ecliptic Z           -0.74634634 +/-    0.0000
Ecliptic XDOT         0.00035120 +/-    0.0000
Ecliptic YDOT         0.00261543 +/-    0.0000
Ecliptic ZDOT         0.00002930 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   43.64054691 +/-    0.0008
Geocenter to KBO     42.67330741 +/-    0.0008
# Hcoef:  6.76

The following table shows the complete astrometric record for 13SK106. 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 (13SK106) followed by the observatory code and reference code for the source of the astrometry.

2000 08  28.29457  23 32 53.94   -04 01 07.9   22.6R 13SK106   807  C~3clG      
2000 08  28.36825  23 32 53.64   -04 01 09.8         13SK106   807  C~3clG      
2013 09  28.11390  00 32 13.591  +02 37 50.05  23.6g 13SK106   W84  C~4yR3      
2013 09  30.15357  00 32 04.771  +02 36 53.84  23.3r 13SK106   W84  C~4yR3      
2013 09  30.15357  00 32 04.77   +02 36 53.8   23.2r 13SK106   W84  C~3clG      
2013 09  30.15656  00 32 04.751  +02 36 53.64  22.8i 13SK106   W84  C~4yR3      
2013 09  30.15656  00 32 04.75   +02 36 53.6   22.8i 13SK106   W84  C~3clG      
2013 10  13.09336  00 31 09.143  +02 31 00.89  22.8z 13SK106   W84  C~4yR3      
2013 10  13.09336  00 31 09.14   +02 31 00.9   22.9z 13SK106   W84  C~3clG      
2013 10  13.12065  00 31 09.026  +02 31 00.23  23.1i 13SK106   W84  C~4yR3      
2013 10  13.12065  00 31 09.03   +02 31 00.2   23.3i 13SK106   W84  C~3clG      
2013 11  22.09809  00 28 50.468  +02 16 43.47  24.3g 13SK106   W84  C~4yR3      
2013 11  22.09947  00 28 50.471  +02 16 43.33  23.2r 13SK106   W84  C~4yR3      
2013 11  22.09947  00 28 50.47   +02 16 43.3   23.3r 13SK106   W84  C~3clG      
2013 11  22.13497  00 28 50.389  +02 16 42.95  22.9i 13SK106   W84  C~4yR3      
2013 11  22.13497  00 28 50.39   +02 16 42.9   22.9i 13SK106   W84  C~3clG      
2014 11  14.05019  00 33 54.433  +02 50 24.83  22.6z 13SK106   W84  C~4yR3      
2014 11  15.10387  00 33 51.319  +02 50 05.73  22.9z 13SK106   W84  C~4yR3      
2016 09  09.28605  00 47 42.458  +04 20 32.87  23.0i 13SK106   W84  C~4yR3      
2016 09  09.28605  00 47 42.46   +04 20 32.9   23.1i 13SK106   W84  C~3clG      
2016 09  09.28743  00 47 42.454  +04 20 32.91  23.0r 13SK106   W84  C~4yR3      
2016 09  09.28743  00 47 42.45   +04 20 32.9   23.1r 13SK106   W84  C~3clG      
2016 09  09.28881  00 47 42.437  +04 20 32.73  24.0g 13SK106   W84  C~4yR3      
2016 09  10.31721  00 47 38.501  +04 20 07.62  22.3z 13SK106   W84  C~4yR3      
2016 09  10.31721  00 47 38.50   +04 20 07.6   22.4z 13SK106   W84  C~3clG      
2016 11  08.11301  00 43 37.074  +03 54 57.40  22.4i 13SK106   W84  C~4yR3      
2016 11  08.11301  00 43 37.08   +03 54 57.4   22.5i 13SK106   W84  C~3clG      
2016 11  08.11440  00 43 37.054  +03 54 57.51  23.0z 13SK106   W84  C~4yR3      
2016 11  18.08408  00 43 05.440  +03 51 46.01  23.3r 13SK106   W84  C~4yR3      
2016 11  18.08408  00 43 05.44   +03 51 46.0   23.5r 13SK106   W84  C~3clG      
2016 11  18.12288  00 43 05.326  +03 51 45.26  23.1i 13SK106   W84  C~4yR3      
2016 11  18.12426  00 43 05.309  +03 51 45.43  22.8z 13SK106   W84  C~4yR3      
2016 11  26.10593  00 42 44.520  +03 49 41.66  22.9r 13SK106   W84  C~4yR3      
2016 11  26.10593  00 42 44.52   +03 49 41.7   22.8r 13SK106   W84  C~3clG      
2016 11  26.10730  00 42 44.522  +03 49 41.58  23.8g 13SK106   W84  C~4yR3      
2016 11  26.10730  00 42 44.52   +03 49 41.6   23.7g 13SK106   W84  C~3clG      

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    -0.06       0.00     0.02
     2   0.0002      0.00     0.01       0.00     0.06
     3  13.0837      0.00     0.14       0.00     0.04
     4  13.0893      0.00     0.09       0.00     0.05
     5  13.0893      0.00     0.08       0.00     0.01
     6  13.0893      0.00    -0.03       0.00    -0.11
     7  13.0893      0.00    -0.01       0.00    -0.07
     8  13.1247      0.00    -0.07       0.00    -0.05
     9  13.1247      0.00    -0.03       0.00    -0.06
    10  13.1248      0.00     0.04       0.00    -0.02
    11  13.1248      0.00    -0.02       0.00     0.01
    12  13.2342      0.00    -0.06       0.00     0.00
    13  13.2342      0.00     0.02       0.00    -0.15
    14  13.2342      0.00     0.03       0.00    -0.12
    15  13.2343      0.00     0.09       0.00    -0.00
    16  13.2343      0.00     0.10       0.00    -0.05
    17  14.2115      0.00    -0.15       0.00     0.16
    18  14.2144      0.00    -0.05       0.00    -0.05
    19  16.0328      0.00     0.00       0.00     0.07
    20  16.0328      0.00    -0.03       0.00     0.04
    21  16.0328      0.00    -0.07       0.00     0.11
    22  16.0328      0.00    -0.01       0.00     0.12
    23  16.0328      0.00    -0.18       0.00    -0.03
    24  16.0357      0.00     0.03       0.00     0.04
    25  16.0357      0.00     0.04       0.00     0.06
    26  16.1966      0.00     0.18       0.00    -0.05
    27  16.1966      0.00     0.09       0.00    -0.05
    28  16.1966      0.00    -0.14       0.00     0.09
    29  16.2239      0.00     0.09       0.00     0.04
    30  16.2239      0.00     0.09       0.00     0.05
    31  16.2240      0.00     0.09       0.00    -0.03
    32  16.2240      0.00    -0.10       0.00     0.17
    33  16.2459      0.00    -0.04       0.00    -0.00
    34  16.2459      0.00    -0.04       0.00    -0.04
    35  16.2459      0.00     0.01       0.00    -0.08
    36  16.2459      0.00     0.04       0.00    -0.10

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.

13SK106    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        44.942    44.942    44.942
ecceobj         0.030     0.030     0.030
incobj          1.163     1.163     1.163
qmin           42.693    42.694    42.693
qmax           46.815    46.817    46.812
amean          44.689    44.690    44.689
amin           44.343    44.342    44.345
amax           45.049    45.049    45.049
emean           0.027     0.027     0.027
emin            0.013     0.013     0.013
emax            0.040     0.040     0.040
imean           1.224     1.224     1.224
imin            0.613     0.613     0.613
imax            1.639     1.639     1.639
excite_mean     0.035     0.035     0.035
fracstop        1.000     1.000     1.000
cjmean          3.108     3.108     3.108

libcent 0      -180.0    -180.0    -180.0
libamp  0      -180.0    -180.0    -180.0
libcent 1      -180.0    -180.0    -180.0
libamp  1      -180.0    -180.0    -180.0
libcent 2      -180.0    -180.0    -180.0
libamp  2      -180.0    -180.0    -180.0
libcent 3      -180.0    -180.0    -180.0
libamp  3      -180.0    -180.0    -180.0
libcent 4      -180.0    -180.0    -180.0
libamp  4      -180.0    -180.0    -180.0

kozaimean       218.4     218.4     218.4
kozaiamp        180.0     180.0     180.0