Orbit Fit and Astrometric record for 15GC58

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: 15GC58    
# Created Wed May  8 01:17:05 2024
# Orbit generated from Bernstein formalism
# Fitting     36 observations of     36
# Arc:   2.34y
# First observation: 2015/02/17
#  Last observation: 2017/06/22
Preliminary a, adot, b, bdot, g, gdot:
  -0.000093   0.021273   0.000003  -0.000351   0.022653   0.000000
# Chi-squared of fit:     6.46 DOF:     66 RMS:  0.07
# Min/Max residuals:    -0.19    0.19
# Exact a, adot, b, bdot, g, gdot:
  1.508837E-05  2.122244E-02 -3.306239E-07 -3.513033E-04  2.270290E-02  8.552545E-04
# Covariance matrix:
  1.5773E-13  6.2361E-15 -9.1891E-16 -9.5234E-16  1.2550E-13  2.3318E-12
  6.2361E-15  2.5596E-13 -2.9383E-16 -4.5609E-15  1.7312E-13  7.8030E-12
 -9.1891E-16 -2.9383E-16  8.3509E-14 -5.9566E-14 -1.2732E-15 -2.8927E-15
 -9.5234E-16 -4.5609E-15 -5.9566E-14  8.2777E-14 -3.6104E-15 -2.1532E-13
  1.2550E-13  1.7312E-13 -1.2732E-15 -3.6104E-15  2.4546E-13  7.0293E-12
  2.3318E-12  7.8030E-12 -2.8927E-15 -2.1532E-13  7.0293E-12  3.5939E-10
#      lat0       lon0       xBary       yBary       zBary        JD0
    2.826139 -157.280727    0.801275    0.028410   -0.572672  2457071.081158
# Heliocentric elements and errors
Epoch:              2457070.5000  =  2015/02/17
Mean Anomaly:          104.99479 +/-     0.668
Argument of Peri:        0.05778 +/-     0.662
Long of Asc Node:       93.82108 +/-     0.014
Inclination:             2.93030 +/-     0.000
Eccentricity:         0.02542773 +/-    0.0008
Semi-Major Axis:     44.31167353 +/-    0.0033
Time of Perihelion: 2425647.9878 +/-     200.0
Perihelion:          43.18492808 +/-    0.0371
Aphelion:            45.43841899 +/-    0.0371
Period (y)              294.9752 +/-      0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -41.42124020 +/-    0.0009
Ecliptic Y          -16.47343304 +/-    0.0004
Ecliptic Z            2.17175568 +/-    0.0000
Ecliptic XDOT         0.00088785 +/-    0.0000
Ecliptic YDOT        -0.00240690 +/-    0.0000
Ecliptic ZDOT        -0.00003714 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   44.62969481 +/-    0.0008
Geocenter to KBO     44.04724086 +/-    0.0010
# Hcoef:  7.68

The following table shows the complete astrometric record for 15GC58. 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 (15GC58) followed by the observatory code and reference code for the source of the astrometry.

2015 02  17.58038  13 28 16.728  -06 12 42.53  24.2r 15GC58    568  C~2nvY      
2015 02  17.62132  13 28 16.638  -06 12 42.03  24.1r 15GC58    568  C~2nvY      
2015 02  20.61441  13 28 10.053  -06 11 53.17  24.1r 15GC58    568  C~2nvY      
2015 03  18.55881  13 26 49.298  -06 02 49.58  24.3r 15GC58    568  C~2nvY      
2015 03  18.59998  13 26 49.141  -06 02 48.52  24.3r 15GC58    568  C~2nvY      
2015 03  20.56294  13 26 41.642  -06 02 00.95  24.0r 15GC58    568  C~2nvY      
2015 04  11.49722  13 25 10.899  -05 52 44.32  24.4r 15GC58    568  C~2nvY      
2015 04  13.36151  13 25 02.908  -05 51 56.64  24.5r 15GC58    568  C~2nvY      
2015 04  13.40245  13 25 02.732  -05 51 55.63  24.3r 15GC58    568  C~2nvY      
2015 04  13.48799  13 25 02.347  -05 51 53.72  23.2r 15GC58    568  C~2nvY      
2015 04  13.50003  13 25 02.293  -05 51 53.28  24.1r 15GC58    568  C~2nvY      
2015 04  13.50498  13 25 02.286  -05 51 53.07  24.2r 15GC58    568  C~2nvY      
2015 04  19.40228  13 24 36.973  -05 49 24.82  24.7r 15GC58    568  C~2nvY      
2015 04  19.51922  13 24 36.471  -05 49 22.07  23.9r 15GC58    568  C~2nvY      
2015 05  18.27664  13 22 43.557  -05 38 55.31  24.2r 15GC58    568  C~2nvY      
2015 05  18.32493  13 22 43.390  -05 38 54.48  24.1r 15GC58    568  C~2nvY      
2015 06  20.27498  13 21 24.559  -05 32 54.75  24.2r 15GC58    568  C~2nvY      
2015 06  20.31583  13 21 24.504  -05 32 54.58  24.3r 15GC58    568  C~2nvY      
2015 06  22.31959  13 21 22.182  -05 32 48.74  24.2r 15GC58    568  C~2nvY      
2015 07  14.27191  13 21 17.673  -05 33 54.55  23.8r 15GC58    568  C~2nvY      
2016 02  04.54302  13 33 08.029  -06 43 25.80  24.4w 15GC58    568  C~2nvY      
2016 02  04.56329  13 33 08.008  -06 43 25.72  24.5w 15GC58    568  C~2nvY      
2016 02  10.53099  13 33 00.915  -06 42 22.07  24.4w 15GC58    568  C~2nvY      
2016 03  11.53218  13 31 45.443  -06 33 31.08  24.7w 15GC58    568  C~2nvY      
2016 04  03.42104  13 30 16.266  -06 24 14.95  24.4w 15GC58    568  C~2nvY      
2016 04  09.40077  13 29 50.801  -06 21 42.85  24.2w 15GC58    568  C~2nvY      
2016 05  01.36453  13 28 17.701  -06 12 48.10  24.0w 15GC58    568  C~2nvY      
2016 05  02.30717  13 28 13.895  -06 12 27.06  23.9w 15GC58    568  C~2nvY      
2016 05  06.31695  13 27 57.924  -06 10 59.31  24.3w 15GC58    568  C~2nvY      
2016 05  28.27195  13 26 42.311  -06 04 26.16  24.1w 15GC58    568  C~2nvY      
2016 06  27.27271  13 25 46.681  -06 00 47.03  24.7w 15GC58    568  C~2nvY      
2016 07  06.30847  13 25 43.315  -06 01 05.14  24.7w 15GC58    568  C~2nvY      
2017 02  24.63168  13 37 03.799  -07 06 33.83        15GC58    568  C~2nvY      
2017 03  29.44523  13 35 12.424  -06 54 38.18  24.6w 15GC58    568  C~2nvY      
2017 06  22.26639  13 30 21.989  -06 28 53.80  24.5w 15GC58    568  C~2nvY      
2017 06  22.27110  13 30 21.989  -06 28 53.71  23.5w 15GC58    568  C~2nvY      

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   0.0001     -1.43    -0.03      -0.03    -0.12
     3   0.0083   -110.73     0.02       9.13    -0.02
     4   0.0793  -1430.78    -0.03      69.34    -0.06
     5   0.0795  -1433.35    -0.04      69.46     0.01
     6   0.0848  -1554.88    -0.02      72.30    -0.14
     7   0.1449  -3018.74    -0.04      88.39    -0.04
     8   0.1500  -3147.18     0.03      88.51     0.19
     9   0.1501  -3150.00     0.09      88.47     0.18
    10   0.1503  -3156.04     0.04      88.12    -0.13
    11   0.1504  -3156.95    -0.03      88.23    -0.01
    12   0.1504  -3157.13     0.14      88.39     0.15
    13   0.1665  -3563.00    -0.12      86.12    -0.00
    14   0.1668  -3570.98     0.03      85.90    -0.11
    15   0.2456  -5369.33    -0.04      42.65     0.08
    16   0.2457  -5371.95    -0.02      42.50     0.06
    17   0.3359  -6599.21     0.02     -60.98    -0.02
    18   0.3360  -6600.04    -0.01     -61.12     0.00
    19   0.3415  -6634.42     0.05     -68.60     0.03
    20   0.4016  -6672.47    -0.02    -154.77    -0.03
    21   0.9636   4716.16     0.09    -116.27     0.09
    22   0.9637   4715.84     0.12    -116.31    -0.01
    23   0.9800   4594.13    -0.12     -95.86     0.12
    24   1.0622   3352.73    -0.04     -14.89     0.00
    25   1.1248   1912.00     0.01      13.34    -0.05
    26   1.1412   1503.03     0.10      14.94    -0.09
    27   1.2013     15.54    -0.19       0.18    -0.02
    28   1.2039    -44.97     0.03      -1.21    -0.08
    29   1.2149   -298.71     0.03      -7.58    -0.05
    30   1.2750  -1491.91     0.02     -58.94    -0.04
    31   1.3571  -2343.99     0.07    -162.36     0.11
    32   1.3819  -2383.94    -0.05    -197.77    -0.01
    33   2.0207   8495.36     0.01    -123.44    -0.11
    34   2.1105   6687.93    -0.02     -63.11     0.02
    35   2.3427   2094.00    -0.03    -214.53    -0.01
    36   2.3428   2093.96     0.02    -214.45     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.

15GC58    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        43.903    43.915    43.892
ecceobj         0.028     0.030     0.027
incobj          2.930     2.930     2.930
qmin           41.878    41.827    41.923
qmax           46.653    46.734    46.569
amean          44.175    44.186    44.165
amin           43.834    43.841    43.817
amax           44.529    44.540    44.516
emean           0.033     0.034     0.032
emin            0.017     0.018     0.016
emax            0.048     0.049     0.047
imean           1.287     1.288     1.286
imin            0.626     0.628     0.624
imax            1.859     1.862     1.859
excite_mean     0.040     0.041     0.039
fracstop        1.000     1.000     1.000
cjmean          3.102     3.102     3.102

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       173.2     173.5     173.2
kozaiamp        180.0     179.9     180.0