Orbit Fit and Astrometric record for 13RE109

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: 13RE109   
# Created Fri Nov 22 02:09:29 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     68 observations of     68
# Arc:   5.13y
# First observation: 2013/09/02
#  Last observation: 2018/10/18
# Chi-squared of fit:    16.18 DOF:    130 RMS:  0.09
# Min/Max residuals:    -0.27    0.25
# Exact a, adot, b, bdot, g, gdot:
  1.463762E-05  2.297599E-02  5.601453E-07 -5.119201E-04  2.392873E-02  3.767066E-03
# Covariance matrix:
  1.5499E-13  5.6302E-15  3.9597E-16 -9.5453E-16  1.2578E-13  4.1478E-13
  5.6302E-15  1.3447E-13  1.8539E-15 -3.4275E-15  1.5155E-13  1.5357E-12
  3.9597E-16  1.8539E-15  7.8702E-14 -2.3461E-14  2.2049E-15  2.2780E-14
 -9.5453E-16 -3.4275E-15 -2.3461E-14  9.7523E-15 -4.3661E-15 -4.2301E-14
  1.2578E-13  1.5155E-13  2.2049E-15 -4.3661E-15  3.0180E-13  1.9394E-12
  4.1478E-13  1.5357E-12  2.2780E-14 -4.2301E-14  1.9394E-12  1.8942E-11
#      lat0       lon0       xBary       yBary       zBary        JD0
   -5.356424    9.047265    0.495652   -0.082072   -0.876268  2456537.788668
# Heliocentric elements and errors
Epoch:              2456538.5000  =  2013/09/03
Mean Anomaly:           72.70266 +/-     0.016
Argument of Peri:      165.69160 +/-     0.018
Long of Asc Node:      112.96430 +/-     0.003
Inclination:             5.41927 +/-     0.000
Eccentricity:         0.14975700 +/-    0.0002
Semi-Major Axis:     43.67302804 +/-    0.0026
Time of Perihelion: 2435248.9656 +/-       5.2
Perihelion:          37.13268632 +/-    0.0083
Aphelion:            50.21336976 +/-    0.0085
Period (y)              288.6212 +/-      0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           42.03738592 +/-    0.0009
Ecliptic Y            6.19486129 +/-    0.0001
Ecliptic Z           -3.90120218 +/-    0.0001
Ecliptic XDOT        -0.00000117 +/-    0.0000
Ecliptic YDOT         0.00266166 +/-    0.0000
Ecliptic ZDOT        -0.00009841 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   42.67000591 +/-    0.0009
Geocenter to KBO     41.79069799 +/-    0.0010
# Hcoef:  6.21

The following table shows the complete astrometric record for 13RE109. 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 (13RE109) followed by the observatory code and reference code for the source of the astrometry.

2013 09  02.28789  00 41 40.285  -01 20 21.05  23.6g 13RE109   W84  C~4yQo      
2013 09  02.28789  00 41 40.29   -01 20 21.1   23.7g 13RE109   W84  C~3cl7      
2013 09  12.15758  00 41 02.288  -01 25 01.32  21.6Y 13RE109   W84  C~4yQo      
2013 09  28.12146  00 39 54.527  -01 32 46.39  22.7g 13RE109   W84  C~4yQo      
2013 09  28.12146  00 39 54.52   -01 32 46.4   22.7g 13RE109   W84  C~3cl7      
2013 10  03.09214  00 39 32.635  -01 35 08.92  23.3g 13RE109   W84  C~4yQo      
2013 10  03.09214  00 39 32.64   -01 35 08.8   23.8g 13RE109   W84  C~3cl7      
2013 10  13.134074 00 38 48.52   -01 39 44.0   22.0i 13RE109   W84  C~35bW      
2013 10  13.13461  00 38 48.524  -01 39 43.97  22.3i 13RE109   W84  C~4yQo      
2013 10  13.13461  00 38 48.52   -01 39 44.0   22.2i 13RE109   W84  C~3cl7      
2013 10  13.17794  00 38 48.330  -01 39 45.14  21.8z 13RE109   W84  C~4yQo      
2013 10  13.17794  00 38 48.33   -01 39 45.1   21.8z 13RE109   W84  C~3cl7      
2013 11  23.119850 00 36 21.13   -01 52 35.9   22.8i 13RE109   W84  C~35bW      
2014 10  28.202280 00 42 39.64   -01 16 21.5   22.4r 13RE109   W84  C~35bW      
2014 10  28.20281  00 42 39.636  -01 16 21.51  22.5r 13RE109   W84  C~4yQo      
2014 10  28.20419  00 42 39.648  -01 16 21.76  22.4i 13RE109   W84  C~4yQo      
2014 10  28.20419  00 42 39.65   -01 16 21.8   22.4i 13RE109   W84  C~3cl7      
2014 11  13.13117  00 41 41.861  -01 21 19.39  21.7i 13RE109   W84  C~4yQo      
2014 11  13.13117  00 41 41.86   -01 21 19.4   22.0i 13RE109   W84  C~3cl7      
2014 11  14.15587  00 41 38.590  -01 21 34.45  22.0z 13RE109   W84  C~4yQo      
2014 11  14.15587  00 41 38.59   -01 21 34.5   22.1z 13RE109   W84  C~3cl7      
2014 11  15.15919  00 41 35.459  -01 21 49.00  21.9z 13RE109   W84  C~4yQo      
2014 11  15.15919  00 41 35.46   -01 21 49.0   21.9z 13RE109   W84  C~3cl7      
2014 11  18.09787  00 41 26.636  -01 22 28.22  21.8z 13RE109   W84  C~4yQo      
2014 11  18.09787  00 41 26.64   -01 22 28.2   21.8z 13RE109   W84  C~3cl7      
2015 10  17.15553  00 48 17.527  -00 42 40.18  22.7r 13RE109   W84  C~4yQo      
2015 10  17.15553  00 48 17.53   -00 42 40.2   22.7r 13RE109   W84  C~3cl7      
2016 08  26.318090 00 56 31.10   +00 09 45.2   22.2i 13RE109   W84  C~35bW      
2016 08  26.319456 00 56 31.10   +00 09 45.2   21.9z 13RE109   W84  C~35bW      
2016 09  01.37842  00 56 11.560  +00 07 10.27  22.3r 13RE109   W84  C~4yQo      
2016 09  01.37842  00 56 11.56   +00 07 10.3   22.3r 13RE109   W84  C~3cl7      
2016 09  01.37979  00 56 11.56   +00 07 10.4   22.9g 13RE109   W84  C~3cl7      
2016 10  23.12717  00 52 37.550  -00 16 28.12  23.8g 13RE109   W84  C~4yQo      
2016 10  23.12717  00 52 37.55   -00 16 28.1   24.0g 13RE109   W84  C~3cl7      
2016 11  05.19660  00 51 45.441  -00 21 12.63  22.3i 13RE109   W84  C~4yQo      
2016 11  05.19660  00 51 45.44   -00 21 12.6   22.4i 13RE109   W84  C~3cl7      
2016 11  06.18077  00 51 41.790  -00 21 31.41  22.7r 13RE109   W84  C~4yQo      
2016 11  06.18077  00 51 41.79   -00 21 31.4   22.8r 13RE109   W84  C~3cl7      
2016 11  07.19710  00 51 38.068  -00 21 50.35  22.3z 13RE109   W84  C~4yQo      
2016 11  07.19710  00 51 38.07   -00 21 50.4   22.1z 13RE109   W84  C~3cl7      
2016 11  08.15371  00 51 34.615  -00 22 07.81  22.4i 13RE109   W84  C~4yQo      
2016 11  08.15371  00 51 34.61   -00 22 07.8   22.4i 13RE109   W84  C~3cl7      
2016 11  18.076690 00 51 01.66   -00 24 44.1   22.6r 13RE109   W84  C~35bW      
2016 11  18.07722  00 51 01.662  -00 24 44.09  22.6r 13RE109   W84  C~4yQo      
2016 11  18.07722  00 51 01.66   -00 24 44.1   22.6r 13RE109   W84  C~3cl7      
2016 11  18.078067 00 51 01.65   -00 24 44.1   23.5g 13RE109   W84  C~35bW      
2016 11  18.07859  00 51 01.650  -00 24 44.11  23.5g 13RE109   W84  C~4yQo      
2016 11  18.07859  00 51 01.65   -00 24 44.1   23.5g 13RE109   W84  C~3cl7      
2016 11  18.15843  00 51 01.412  -00 24 45.11  22.0z 13RE109   W84  C~4yQo      
2016 11  18.15843  00 51 01.41   -00 24 45.1   21.9z 13RE109   W84  C~3cl7      
2017 08  28.351053 01 01 10.37   +00 37 36.6   22.5r 13RE109   W84  C~35bW      
2017 08  28.35159  01 01 10.371  +00 37 36.57  22.5r 13RE109   W84  C~4yQo      
2017 08  28.352431 01 01 10.36   +00 37 36.6   22.0i 13RE109   W84  C~35bW      
2017 08  28.35296  01 01 10.366  +00 37 36.57  22.0i 13RE109   W84  C~4yQo      
2017 08  28.353796 01 01 10.35   +00 37 36.5   23.7g 13RE109   W84  C~35bW      
2017 08  28.35432  01 01 10.353  +00 37 36.45  23.6g 13RE109   W84  C~4yQo      
2017 09  18.286782 00 59 54.84   +00 28 15.2   22.2r 13RE109   W84  C~35bW      
2017 09  18.28731  00 59 54.848  +00 28 15.12  22.1r 13RE109   W84  C~4yQo      
2017 09  18.288171 00 59 54.84   +00 28 15.0   21.9i 13RE109   W84  C~35bW      
2017 09  18.28870  00 59 54.846  +00 28 14.99  21.6i 13RE109   W84  C~4yQo      
2017 09  18.289549 00 59 54.84   +00 28 15.0   23.8g 13RE109   W84  C~35bW      
2017 09  18.29007  00 59 54.848  +00 28 14.95  23.7g 13RE109   W84  C~4yQo      
2017 09  25.24522  00 59 25.995  +00 24 57.77  23.6g 13RE109   W84  C~4yQo      
2017 09  25.246076 00 59 25.98   +00 24 57.7   22.1z 13RE109   W84  C~35bW      
2017 09  25.24660  00 59 25.983  +00 24 57.64  21.9z 13RE109   W84  C~4yQo      
2017 10  22.161574 00 57 29.20   +00 12 48.9   22.1z 13RE109   W84  C~35bW      
2017 10  22.16210  00 57 29.205  +00 12 48.92  22.1z 13RE109   W84  C~4yQo      
2018 10  18.20881  01 02 32.104  +00 43 11.65  21.9z 13RE109   W84  C~4yQo      

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     0.18       0.00    -0.13
     2   0.0000      0.00     0.25       0.00    -0.18
     3   0.0270      0.00     0.06       0.00    -0.03
     4   0.0707      0.00    -0.18       0.00    -0.02
     5   0.0707      0.00    -0.08       0.00    -0.01
     6   0.0843      0.00    -0.02       0.00    -0.15
     7   0.0843      0.00    -0.09       0.00    -0.27
     8   0.1118      0.00    -0.08       0.00    -0.00
     9   0.1118      0.00     0.02       0.00     0.04
    10   0.1118      0.00    -0.04       0.00     0.01
    11   0.1120      0.00    -0.02       0.00     0.05
    12   0.1120      0.00    -0.02       0.00     0.01
    13   0.2240      0.00     0.18       0.00     0.05
    14   1.1524      0.00    -0.17       0.00     0.15
    15   1.1524      0.00    -0.20       0.00     0.15
    16   1.1524      0.00     0.07       0.00    -0.07
    17   1.1524      0.00     0.10       0.00    -0.11
    18   1.1960      0.00     0.02       0.00     0.04
    19   1.1960      0.00     0.04       0.00     0.05
    20   1.1988      0.00    -0.03       0.00     0.16
    21   1.1988      0.00    -0.03       0.00     0.21
    22   1.2016      0.00     0.05       0.00     0.05
    23   1.2016      0.00     0.04       0.00     0.05
    24   1.2096      0.00     0.05       0.00     0.11
    25   1.2096      0.00    -0.01       0.00     0.09
    26   2.1215      0.00    -0.00       0.00    -0.03
    27   2.1215      0.00    -0.05       0.00    -0.01
    28   2.9816      0.00    -0.08       0.00     0.09
    29   2.9816      0.00    -0.02       0.00     0.12
    30   2.9982      0.00     0.02       0.00     0.11
    31   2.9982      0.00     0.02       0.00     0.08
    32   2.9982      0.00     0.09       0.00     0.24
    33   3.1399      0.00     0.06       0.00    -0.10
    34   3.1399      0.00     0.06       0.00    -0.12
    35   3.1757      0.00     0.02       0.00     0.01
    36   3.1757      0.00     0.03       0.00    -0.02
    37   3.1784      0.00    -0.00       0.00    -0.01
    38   3.1784      0.00    -0.00       0.00    -0.02
    39   3.1811      0.00     0.03       0.00    -0.04
    40   3.1811      0.00     0.00       0.00     0.01
    41   3.1838      0.00    -0.06       0.00    -0.00
    42   3.1838      0.00     0.01       0.00    -0.01
    43   3.2109      0.00     0.01       0.00    -0.07
    44   3.2109      0.00     0.04       0.00    -0.06
    45   3.2109      0.00     0.07       0.00    -0.05
    46   3.2109      0.00    -0.07       0.00    -0.05
    47   3.2109      0.00    -0.05       0.00    -0.04
    48   3.2109      0.00    -0.05       0.00    -0.05
    49   3.2111      0.00     0.07       0.00     0.03
    50   3.2111      0.00     0.10       0.00     0.02
    51   3.9865      0.00     0.06       0.00    -0.05
    52   3.9865      0.00     0.10       0.00    -0.06
    53   3.9865      0.00    -0.02       0.00    -0.01
    54   3.9865      0.00     0.09       0.00    -0.03
    55   3.9865      0.00    -0.11       0.00    -0.08
    56   3.9865      0.00    -0.04       0.00    -0.12
    57   4.0438      0.00    -0.19       0.00     0.15
    58   4.0438      0.00    -0.04       0.00     0.08
    59   4.0438      0.00    -0.11       0.00    -0.01
    60   4.0438      0.00     0.02       0.00    -0.01
    61   4.0438      0.00    -0.02       0.00     0.02
    62   4.0438      0.00     0.13       0.00    -0.01
    63   4.0629      0.00     0.13       0.00     0.09
    64   4.0629      0.00    -0.04       0.00     0.04
    65   4.0629      0.00     0.04       0.00    -0.01
    66   4.1365      0.00    -0.05       0.00    -0.09
    67   4.1365      0.00     0.06       0.00    -0.06
    68   5.1250      0.00     0.09       0.00     0.01

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.

13RE109    quality flag:3

Type:         7:4EEE    7:4EEE    7:4EEE

axisobj        43.930    43.930    43.930
ecceobj         0.152     0.152     0.152
incobj          5.418     5.418     5.418
qmin           36.523    36.520    36.551
qmax           51.466    51.571    51.494
amean          43.726    43.726    43.726
amin           43.240    43.240    43.241
amax           44.240    44.253    44.240
emean           0.151     0.152     0.151
emin            0.137     0.139     0.139
emax            0.163     0.165     0.164
imean           3.944     3.928     3.937
imin            2.985     2.928     2.968
imax            5.034     5.077     5.077
excite_mean     0.166     0.167     0.167
fracstop        1.000     1.000     1.000
cjmean          3.065     3.065     3.065

libcent 0       182.5     179.9     182.2
libamp  0       136.2     141.4     142.3
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       198.5     184.1     190.0
kozaiamp        180.0     180.0     179.9