Orbit Fit and Astrometric record for 15GX56

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: 15GX56    
# Created Wed May  8 01:17:04 2024
# Orbit generated from Bernstein formalism
# Fitting     35 observations of     35
# Arc:   2.11y
# First observation: 2015/02/17
#  Last observation: 2017/03/29
Preliminary a, adot, b, bdot, g, gdot:
  -0.000114   0.023521   0.000000  -0.000845   0.023797   0.000000
# Chi-squared of fit:     6.64 DOF:     64 RMS:  0.08
# Min/Max residuals:    -0.18    0.16
# Exact a, adot, b, bdot, g, gdot:
  1.514301E-05  2.342404E-02 -4.663065E-07 -8.429450E-04  2.387224E-02  1.982706E-03
# Covariance matrix:
  1.9066E-13  5.6112E-15  7.8068E-16 -4.3327E-15  1.5871E-13  3.2057E-12
  5.6112E-15  2.9347E-13  2.0363E-15 -1.1390E-14  1.8509E-13  8.3942E-12
  7.8068E-16  2.0363E-15  8.7605E-14 -7.8215E-14  2.0523E-15  1.1183E-13
 -4.3327E-15 -1.1390E-14 -7.8215E-14  1.3361E-13 -1.1444E-14 -6.2622E-13
  1.5871E-13  1.8509E-13  2.0523E-15 -1.1444E-14  2.7846E-13  8.4472E-12
  3.2057E-12  8.3942E-12  1.1183E-13 -6.2622E-13  8.4472E-12  4.6124E-10
#      lat0       lon0       xBary       yBary       zBary        JD0
   -0.007438 -155.200721    0.822314    0.000077   -0.542766  2457071.002878
# Heliocentric elements and errors
Epoch:              2457070.5000  =  2015/02/17
Mean Anomaly:           51.06625 +/-     0.240
Argument of Peri:      121.38039 +/-     0.334
Long of Asc Node:       23.48183 +/-     0.001
Inclination:             2.05339 +/-     0.001
Eccentricity:         0.08170817 +/-    0.0008
Semi-Major Axis:     44.53540551 +/-    0.0068
Time of Perihelion: 2441671.6612 +/-      72.2
Perihelion:          40.89649922 +/-    0.0372
Aphelion:            48.17431180 +/-    0.0374
Period (y)              297.2120 +/-      0.07
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -38.86709642 +/-    0.0008
Ecliptic Y          -17.05138051 +/-    0.0004
Ecliptic Z           -0.00546332 +/-    0.0000
Ecliptic XDOT         0.00091674 +/-    0.0000
Ecliptic YDOT        -0.00253965 +/-    0.0000
Ecliptic ZDOT        -0.00009661 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   42.44291214 +/-    0.0008
Geocenter to KBO     41.88966474 +/-    0.0009
# Hcoef:  7.89

The following table shows the complete astrometric record for 15GX56. 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 (15GX56) followed by the observatory code and reference code for the source of the astrometry.

2015 02  17.50210  13 31 52.897  -09 36 40.64  24.0r 15GX56    568  C~2nvU      
2015 02  17.54344  13 31 52.800  -09 36 40.23  24.3r 15GX56    568  C~2nvU      
2015 02  20.47426  13 31 46.302  -09 36 03.75  24.1r 15GX56    568  C~2nvU      
2015 03  18.47063  13 30 22.936  -09 28 11.35  24.4r 15GX56    568  C~2nvU      
2015 03  18.47537  13 30 22.927  -09 28 11.31  24.0r 15GX56    568  C~2nvU      
2015 03  18.52182  13 30 22.731  -09 28 10.23  24.4r 15GX56    568  C~2nvU      
2015 03  20.52388  13 30 14.760  -09 27 24.61  23.9r 15GX56    568  C~2nvU      
2015 04  11.41445  13 28 39.827  -09 18 20.24  24.2r 15GX56    568  C~2nvU      
2015 04  12.36711  13 28 35.507  -09 17 55.43  24.1r 15GX56    568  C~2nvU      
2015 04  12.40803  13 28 35.317  -09 17 54.33  24.3r 15GX56    568  C~2nvU      
2015 04  12.45503  13 28 35.105  -09 17 53.14  23.8r 15GX56    568  C~2nvU      
2015 04  14.46499  13 28 26.004  -09 17 00.88  23.8r 15GX56    568  C~2nvU      
2015 04  18.42564  13 28 08.074  -09 15 17.49  24.0r 15GX56    568  C~2nvU      
2015 04  18.47335  13 28 07.865  -09 15 16.39  24.0r 15GX56    568  C~2nvU      
2015 05  16.27210  13 26 10.776  -09 04 01.33  24.0r 15GX56    568  C~2nvU      
2015 05  25.37637  13 25 39.117  -09 00 59.14  24.0r 15GX56    568  C~2nvU      
2015 05  25.43418  13 25 38.916  -09 00 58.02  24.0r 15GX56    568  C~2nvU      
2015 06  21.32593  13 24 37.293  -08 55 06.74  24.2r 15GX56    568  C~2nvU      
2015 06  22.28249  13 24 36.120  -08 55 00.18  24.3r 15GX56    568  C~2nvU      
2015 07  12.27649  13 24 29.172  -08 54 28.49  24.2r 15GX56    568  C~2nvU      
2015 07  15.26670  13 24 31.086  -08 54 40.99  24.3r 15GX56    568  C~2nvU      
2015 07  19.26636  13 24 34.859  -08 55 05.30  24.2r 15GX56    568  C~2nvU      
2016 03  11.58783  13 35 48.334  -10 02 43.84  24.2w 15GX56    568  C~2nvU      
2016 03  11.63454  13 35 48.169  -10 02 43.05  24.6w 15GX56    568  C~2nvU      
2016 03  12.48427  13 35 45.127  -10 02 26.02  24.4w 15GX56    568  C~2nvU      
2016 04  03.46148  13 34 15.350  -09 53 59.65  24.3w 15GX56    568  C~2nvU      
2016 04  09.44264  13 33 48.585  -09 51 27.82  24.2w 15GX56    568  C~2nvU      
2016 05  02.32341  13 32 06.368  -09 41 46.14  24.2w 15GX56    568  C~2nvU      
2016 05  06.33319  13 31 49.417  -09 40 09.51  24.4w 15GX56    568  C~2nvU      
2016 05  28.31243  13 30 28.738  -09 32 29.27  24.5w 15GX56    568  C~2nvU      
2016 05  29.31935  13 30 25.663  -09 32 11.73  24.5w 15GX56    568  C~2nvU      
2016 06  04.38178  13 30 08.563  -09 30 34.56  24.3w 15GX56    568  C~2nvU      
2016 06  27.29699  13 29 28.537  -09 26 49.78  24.3w 15GX56    568  C~2nvU      
2016 07  07.29960  13 29 24.488  -09 26 30.32  24.6w 15GX56    568  C~2nvU      
2017 03  29.46402  13 39 41.524  -10 28 18.29        15GX56    568  C~2nvU      

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     0.08       0.00    -0.02
     2   0.0001     -1.49     0.01      -0.14    -0.12
     3   0.0081   -104.27     0.09      -1.40     0.03
     4   0.0793  -1424.83     0.00     -14.24    -0.04
     5   0.0793  -1424.97     0.16     -14.25    -0.05
     6   0.0795  -1428.06     0.02     -14.31    -0.07
     7   0.0849  -1554.52    -0.02     -15.20     0.04
     8   0.1449  -3061.40     0.06     -25.82     0.06
     9   0.1475  -3130.01    -0.13     -26.32     0.00
    10   0.1476  -3133.03    -0.17     -26.33     0.03
    11   0.1477  -3136.38    -0.09     -26.38     0.03
    12   0.1532  -3280.92     0.01     -27.44    -0.05
    13   0.1641  -3565.86    -0.12     -29.18     0.12
    14   0.1642  -3569.14     0.07     -29.30     0.05
    15   0.2403  -5430.70     0.11     -42.43     0.05
    16   0.2652  -5934.19     0.11     -46.79    -0.02
    17   0.2654  -5937.37    -0.06     -46.85    -0.03
    18   0.3390  -6916.54     0.06     -59.02    -0.08
    19   0.3416  -6935.14     0.05     -59.38    -0.03
    20   0.3964  -7042.63     0.05     -68.16    -0.07
    21   0.4046  -7011.62    -0.09     -69.24     0.13
    22   0.4155  -6950.61    -0.16     -71.08     0.01
    23   1.0625   3810.62    -0.18    -185.74     0.10
    24   1.0626   3808.06    -0.05    -185.89    -0.01
    25   1.0650   3760.00     0.04    -186.36    -0.08
    26   1.1251   2340.03     0.00    -197.62     0.00
    27   1.1415   1916.33    -0.06    -200.52     0.09
    28   1.2042    297.23     0.03    -211.34     0.05
    29   1.2151     28.61    -0.02    -213.21     0.01
    30   1.2753  -1250.27     0.03    -222.62    -0.01
    31   1.2781  -1299.02    -0.04    -223.01     0.02
    32   1.2947  -1570.01    -0.05    -225.55    -0.03
    33   1.3574  -2203.42     0.15    -234.23     0.10
    34   1.3848  -2266.30     0.02    -238.17    -0.16
    35   2.1108   7577.58     0.06    -369.82    -0.05

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.

15GX56    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        44.102    44.125    44.081
ecceobj         0.075     0.078     0.073
incobj          2.062     2.062     2.063
qmin           39.906    39.850    40.006
qmax           49.133    49.271    48.995
amean          44.387    44.410    44.365
amin           44.024    44.059    44.013
amax           44.766    44.789    44.751
emean           0.082     0.084     0.079
emin            0.066     0.068     0.064
emax            0.098     0.100     0.095
imean           2.174     2.176     2.173
imin            1.397     1.393     1.398
imax            2.812     2.822     2.806
excite_mean     0.090     0.093     0.088
fracstop        1.000     1.000     1.000
cjmean          3.096     3.096     3.096

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       167.9     168.3     168.1
kozaiamp        180.0     180.0     180.0