Orbit Fit and Astrometric record for 11HM102

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: 11HM102   
# Created Thu Feb 21 02:09:08 2019
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting  159 observations of  159
# Arc:   7.07y
# First observation: 2011/04/29
#  Last observation: 2018/05/24
# Chi-squared of fit:    40.15 DOF:  312 RMS:  0.09
# Min/Max residuals:    -0.45    0.45
# Exact a, adot, b, bdot, g, gdot:
  1.671506E-05  3.932532E-02 -9.619120E-06 -2.215370E-02  3.659373E-02  2.512311E-03
# Covariance matrix:
  3.5626E-14 -1.7315E-14 -2.4898E-15  8.8027E-15  3.0610E-14 -6.6788E-14
 -1.7315E-14  4.8933E-14  6.5291E-15 -2.8090E-14 -4.8635E-15  2.1921E-13
 -2.4898E-15  6.5291E-15  1.1956E-14 -7.1329E-15 -1.2659E-15  3.2248E-14
  8.8027E-15 -2.8090E-14 -7.1329E-15  2.2485E-14  2.6755E-15 -1.3914E-13
  3.0610E-14 -4.8635E-15 -1.2659E-15  2.6755E-15  4.2676E-14 -1.8114E-14
 -6.6788E-14  2.1921E-13  3.2248E-14 -1.3914E-13 -1.8114E-14  1.0862E-12
#      lat0       lon0       xBary       yBary       zBary        JD0
    2.645455  -81.833936    0.873206    0.023414   -0.507303  2455680.803016
# Heliocentric elements and errors
Epoch:              2455680.5000  =  2011/04/29
Mean Anomaly:           18.06099 +/-     0.011
Argument of Peri:      153.48986 +/-     0.013
Long of Asc Node:      100.99369 +/-     0.000
Inclination:            29.38415 +/-     0.000
Eccentricity:         0.08032493 +/-    0.0000
Semi-Major Axis:     30.12824479 +/-    0.0009
Time of Perihelion: 2452650.1121 +/-       1.9
Perihelion:          27.70819578 +/-    0.0012
Aphelion:            32.54829380 +/-    0.0013
Period (y)              165.3747 +/-      0.01
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X            3.08972730 +/-    0.0000
Ecliptic Y          -27.64784787 +/-    0.0002
Ecliptic Z            1.26104496 +/-    0.0000
Ecliptic XDOT         0.00294802 +/-    0.0000
Ecliptic YDOT         0.00016227 +/-    0.0000
Ecliptic ZDOT        -0.00164701 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   27.84850699 +/-    0.0002
Geocenter to KBO     27.32708878 +/-    0.0002
# Hcoef:  8.28

The following table shows the complete astrometric record for 11HM102. 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 (11HM102) followed by the observatory code and reference code for the source of the astrometry.

2011 04  29.30225  18 34 51.76   -20 32 49.6         11HM102   268  C~0jJo      
2011 04  29.30402  18 34 51.75   -20 32 49.7         11HM102   268  C~0jJo      
2011 04  29.30935  18 34 51.73   -20 32 49.7         11HM102   268  C~0jJo      
2011 04  29.31112  18 34 51.73   -20 32 49.7         11HM102   268  C~0jJo      
2011 04  29.31202  18 34 51.73   -20 32 49.7         11HM102   268  C~0jJo      
2011 04  29.31291  18 34 51.72   -20 32 49.7         11HM102   268  C~0jJo      
2011 04  29.31470  18 34 51.72   -20 32 49.8         11HM102   268  C~0jJo      
2011 04  29.31648  18 34 51.71   -20 32 49.8         11HM102   268  C~0jJo      
2011 04  29.32003  18 34 51.70   -20 32 49.8         11HM102   268  C~0jJo      
2011 04  29.32182  18 34 51.70   -20 32 49.8         11HM102   268  C~0jJo      
2011 04  30.20947  18 34 49.08   -20 32 58.6         11HM102   268  C~0jJo      
2011 04  30.33360  18 34 48.70   -20 32 59.9   22.5R 11HM102   268  C~0jJo      
2011 04  30.33534  18 34 48.69   -20 32 59.9   22.4R 11HM102   268  C~0jJo      
2011 04  30.33711  18 34 48.68   -20 32 59.9   22.5R 11HM102   268  C~0jJo      
2011 04  30.33888  18 34 48.68   -20 32 59.9   22.5R 11HM102   268  C~0jJo      
2011 04  30.34064  18 34 48.67   -20 33 00.0   22.5R 11HM102   268  C~0jJo      
2011 04  30.34152  18 34 48.67   -20 32 59.9         11HM102   268  C~0jJo      
2011 04  30.34242  18 34 48.67   -20 32 59.9   22.6R 11HM102   268  C~0jJo      
2011 04  30.34418  18 34 48.66   -20 33 00.0   22.5R 11HM102   268  C~0jJp      
2011 04  30.34593  18 34 48.66   -20 33 00.0   22.5R 11HM102   268  C~0jJp      
2011 04  30.34772  18 34 48.65   -20 33 00.0   24.9R 11HM102   268  C~0jJp      
2011 04  30.34946  18 34 48.65   -20 33 00.0   22.9R 11HM102   268  C~0jJp      
2011 05  29.42902  18 32 28.89   -20 39 01.4         11HM102   266  C~0jJp      
2011 05  29.57806  18 32 27.93   -20 39 03.7         11HM102   266  C~0jJp      
2011 05  30.46730  18 32 22.31   -20 39 16.5         11HM102   266  C~0jJp      
2011 05  31.41887  18 32 16.19   -20 39 30.9         11HM102   266  C~0jJp      
2011 06  01.58664  18 32 08.56   -20 39 48.5         11HM102   266  C~0jJp      
2011 07  01.08961  18 28 33.93   -20 48 04.8         11HM102   269  C~0jJp      
2011 07  01.09152  18 28 33.91   -20 48 04.8         11HM102   269  C~0jJp      
2011 07  01.09345  18 28 33.90   -20 48 04.7         11HM102   269  C~0jJp      
2011 07  01.09537  18 28 33.89   -20 48 04.9         11HM102   269  C~0jJp      
2011 07  01.09728  18 28 33.88   -20 48 05.0         11HM102   269  C~0jJp      
2011 07  01.09921  18 28 33.86   -20 48 05.0         11HM102   269  C~0jJp      
2011 07  01.10007  18 28 33.85   -20 48 05.1         11HM102   269  C~0jJp      
2011 07  01.10116  18 28 33.85   -20 48 05.0         11HM102   269  C~0jJp      
2011 07  01.10307  18 28 33.83   -20 48 05.1         11HM102   269  C~0jJp      
2011 07  01.10499  18 28 33.82   -20 48 05.0         11HM102   269  C~0jJp      
2011 07  01.10692  18 28 33.80   -20 48 05.1         11HM102   269  C~0jJp      
2011 07  01.17550  18 28 33.27   -20 48 06.3         11HM102   269  C~0jJp      
2011 07  01.17744  18 28 33.26   -20 48 06.4         11HM102   269  C~0jJp      
2011 07  01.17935  18 28 33.24   -20 48 06.4         11HM102   269  C~0jJp      
2011 07  01.18129  18 28 33.23   -20 48 06.5         11HM102   269  C~0jJp      
2011 07  01.18322  18 28 33.21   -20 48 06.6         11HM102   269  C~0jJp      
2011 07  01.18502  18 28 33.21   -20 48 06.6         11HM102   269  C~0jJp      
2011 07  01.18514  18 28 33.19   -20 48 06.6         11HM102   269  C~0jJp      
2011 07  01.18705  18 28 33.18   -20 48 06.6         11HM102   269  C~0jJp      
2011 07  01.18898  18 28 33.17   -20 48 06.7         11HM102   269  C~0jJp      
2011 07  01.19090  18 28 33.15   -20 48 06.6         11HM102   269  C~0jJp      
2011 07  01.19284  18 28 33.15   -20 48 06.7         11HM102   269  C~0jJp      
2011 07  01.19476  18 28 33.13   -20 48 06.9         11HM102   269  C~0jJp      
2011 07  01.26066  18 28 32.62   -20 48 07.9         11HM102   269  C~0jJp      
2011 07  01.26257  18 28 32.59   -20 48 08.0         11HM102   269  C~0jJp      
2011 07  01.26450  18 28 32.58   -20 48 08.1         11HM102   269  C~0jJp      
2011 07  01.26643  18 28 32.57   -20 48 08.0         11HM102   269  C~0jJp      
2011 07  01.26836  18 28 32.55   -20 48 08.1         11HM102   269  C~0jJp      
2011 07  01.27016  18 28 32.55   -20 48 08.2         11HM102   269  C~0jJp      
2011 07  01.27028  18 28 32.54   -20 48 08.2         11HM102   269  C~0jJp      
2011 07  01.27220  18 28 32.52   -20 48 08.2         11HM102   269  C~0jJp      
2011 07  01.27412  18 28 32.51   -20 48 08.3         11HM102   269  C~0jJp      
2011 07  01.27604  18 28 32.49   -20 48 08.2         11HM102   269  C~0jJp      
2011 07  01.27797  18 28 32.49   -20 48 08.3         11HM102   269  C~0jJp      
2011 07  01.27991  18 28 32.47   -20 48 08.3         11HM102   269  C~0jJp      
2011 07  01.34586  18 28 31.97   -20 48 09.5         11HM102   269  C~0jJp      
2011 07  01.34779  18 28 31.94   -20 48 09.5         11HM102   269  C~0jJp      
2011 07  01.34971  18 28 31.94   -20 48 09.7         11HM102   269  C~0jJp      
2011 07  01.35164  18 28 31.92   -20 48 09.7         11HM102   269  C~0jJp      
2011 07  01.35356  18 28 31.91   -20 48 09.7         11HM102   269  C~0jJp      
2011 07  01.35548  18 28 31.89   -20 48 09.7         11HM102   269  C~0jJp      
2011 07  01.35735  18 28 31.89   -20 48 09.6         11HM102   269  C~0jJp      
2011 07  01.35741  18 28 31.87   -20 48 09.7         11HM102   269  C~0jJp      
2011 07  01.35935  18 28 31.86   -20 48 09.8         11HM102   269  C~0jJp      
2011 07  01.36127  18 28 31.84   -20 48 09.8         11HM102   269  C~0jJp      
2011 07  01.36318  18 28 31.84   -20 48 09.8         11HM102   269  C~0jJp      
2011 07  01.36510  18 28 31.81   -20 48 09.9         11HM102   269  C~0jJp      
2011 07  01.36736  18 28 31.80   -20 48 09.9         11HM102   269  C~0jJp      
2011 07  01.36935  18 28 31.78   -20 48 09.9         11HM102   269  C~0jJp      
2011 07  02.03048  18 28 26.80   -20 48 22.0         11HM102   269  C~0jJp      
2011 07  02.03240  18 28 26.78   -20 48 22.0         11HM102   269  C~0jJp      
2011 07  02.03433  18 28 26.77   -20 48 22.1         11HM102   269  C~0jJp      
2011 07  02.03625  18 28 26.76   -20 48 22.1         11HM102   269  C~0jJp      
2011 07  02.03818  18 28 26.74   -20 48 22.2         11HM102   269  C~0jJp      
2011 07  02.04000  18 28 26.72   -20 48 22.2         11HM102   269  C~0jJp      
2011 07  02.04012  18 28 26.73   -20 48 22.2         11HM102   269  C~0jJp      
2011 07  02.04204  18 28 26.71   -20 48 22.2         11HM102   269  C~0jJp      
2011 07  02.04398  18 28 26.69   -20 48 22.3         11HM102   269  C~0jJp      
2011 07  02.04589  18 28 26.68   -20 48 22.3         11HM102   269  C~0jJp      
2011 07  02.04784  18 28 26.66   -20 48 22.3         11HM102   269  C~0jJp      
2011 07  02.04975  18 28 26.65   -20 48 22.4         11HM102   269  C~0jJp      
2011 07  02.13822  18 28 25.97   -20 48 24.0         11HM102   269  C~0jJp      
2011 07  02.14013  18 28 25.96   -20 48 24.1         11HM102   269  C~0jJp      
2011 07  02.14205  18 28 25.94   -20 48 24.1         11HM102   269  C~0jJp      
2011 07  02.14398  18 28 25.93   -20 48 24.1         11HM102   269  C~0jJp      
2011 07  02.14590  18 28 25.91   -20 48 24.1         11HM102   269  C~0jJp      
2011 07  02.14771  18 28 25.89   -20 48 24.2         11HM102   269  C~0jJp      
2011 07  02.14784  18 28 25.89   -20 48 24.2         11HM102   269  C~0jJp      
2011 07  02.14977  18 28 25.88   -20 48 24.2         11HM102   269  C~0jJp      
2011 07  02.15169  18 28 25.86   -20 48 24.3         11HM102   269  C~0jJp      
2011 07  02.15362  18 28 25.85   -20 48 24.3         11HM102   269  C~0jJp      
2011 07  02.15554  18 28 25.83   -20 48 24.3         11HM102   269  C~0jJp      
2011 07  02.15746  18 28 25.82   -20 48 24.4         11HM102   269  C~0jJp      
2011 07  02.24846  18 28 25.12   -20 48 26.0         11HM102   269  C~0jJp      
2011 07  02.25039  18 28 25.10   -20 48 26.1         11HM102   269  C~0jJp      
2011 07  02.25233  18 28 25.09   -20 48 26.1         11HM102   269  C~0jJp      
2011 07  02.25425  18 28 25.08   -20 48 26.2         11HM102   269  C~0jJp      
2011 07  02.25618  18 28 25.06   -20 48 26.2         11HM102   269  C~0jJp      
2011 07  02.25701  18 28 25.05   -20 48 26.2         11HM102   269  C~0jJp      
2011 07  02.25809  18 28 25.04   -20 48 26.2         11HM102   269  C~0jJp      
2011 07  02.26001  18 28 25.03   -20 48 26.2         11HM102   269  C~0jJp      
2011 07  02.26194  18 28 25.02   -20 48 26.3         11HM102   269  C~0jJp      
2011 07  02.26386  18 28 25.00   -20 48 26.3         11HM102   269  C~0jJp      
2011 07  02.26580  18 28 24.98   -20 48 26.3         11HM102   269  C~0jJp      
2011 07  02.28855  18 28 24.84   -20 48 26.9         11HM102   266  C~0jJp      
2011 07  02.33772  18 28 24.42   -20 48 27.7         11HM102   269  C~0jJp      
2011 07  02.34927  18 28 24.34   -20 48 27.8         11HM102   269  C~0jJp      
2011 07  02.34946  18 28 24.37   -20 48 28.1         11HM102   269  C~0jJp      
2011 07  02.35039  18 28 24.36   -20 48 28.1         11HM102   266  C~0jJp      
2011 07  02.35119  18 28 24.34   -20 48 27.8         11HM102   269  C~0jJp      
2011 07  02.35313  18 28 24.32   -20 48 27.9         11HM102   269  C~0jJp      
2011 07  02.35505  18 28 24.30   -20 48 27.9         11HM102   269  C~0jJp      
2011 07  02.35697  18 28 24.28   -20 48 27.8         11HM102   269  C~0jJp      
2011 07  02.35901  18 28 24.27   -20 48 28.1         11HM102   269  C~0jJp      
2011 07  02.41278  18 28 23.88   -20 48 29.3         11HM102   266  C~0jJp      
2011 08  03.34707  18 24 41.56   -20 58 34.0         11HM102   267  C~0jJp      
2011 08  03.35026  18 24 41.54   -20 58 34.1         11HM102   267  C~0jJp      
2011 08  03.36949  18 24 41.41   -20 58 34.5         11HM102   267  C~0jJp      
2011 08  29.02299  18 22 46.74   -21 06 38.8         11HM102   269  C~0jJp      
2011 08  29.08703  18 22 46.54   -21 06 40.1         11HM102   269  C~0jJp      
2011 08  29.15097  18 22 46.36   -21 06 41.3         11HM102   269  C~0jJp      
2011 08  30.04199  18 22 43.88   -21 06 57.8         11HM102   269  C~0jJp      
2011 08  30.10496  18 22 43.69   -21 06 58.9         11HM102   269  C~0jJp      
2012 04  17.28353  18 45 10.46   -21 37 16.0   22.0R 11HM102   268  C~0jJp      
2012 04  17.28539  18 45 10.46   -21 37 16.0   21.9R 11HM102   268  C~0jJp      
2012 04  17.28715  18 45 10.46   -21 37 16.0   22.1R 11HM102   268  C~0jJp      
2012 04  17.28892  18 45 10.45   -21 37 16.1   22.3R 11HM102   268  C~0jJp      
2012 04  17.29069  18 45 10.46   -21 37 16.1   22.2R 11HM102   268  C~0jJp      
2012 04  17.29244  18 45 10.45   -21 37 16.1   22.2R 11HM102   268  C~0jJp      
2012 04  17.29421  18 45 10.45   -21 37 16.1   22.3R 11HM102   268  C~0jJp      
2012 04  17.29596  18 45 10.45   -21 37 16.1   22.1R 11HM102   268  C~0jJp      
2012 04  17.29773  18 45 10.45   -21 37 16.1   22.3R 11HM102   268  C~0jJp      
2012 04  17.29950  18 45 10.45   -21 37 16.2   22.2R 11HM102   268  C~0jJp      
2012 04  17.30127  18 45 10.44   -21 37 16.2   22.2R 11HM102   268  C~0jJp      
2012 04  17.30303  18 45 10.44   -21 37 16.2   22.2R 11HM102   268  C~0jJp      
2012 04  17.30495  18 45 10.44   -21 37 16.1         11HM102   268  C~0jJp      
2012 04  17.30574  18 45 10.44   -21 37 16.3         11HM102   268  C~0jJp      
2012 04  17.30672  18 45 10.44   -21 37 16.2         11HM102   268  C~0jJp      
2014 05  06.54799  19 04 49.511  -23 46 57.06  22.5G 11HM102   F51  C~2r7L      
2014 05  06.55895  19 04 49.467  -23 46 56.89  23.0G 11HM102   F51  C~2r7L      
2014 05  06.56987  19 04 49.439  -23 46 57.09  22.4G 11HM102   F51  C~2r7L      
2014 05  06.58083  19 04 49.400  -23 46 57.32  22.7G 11HM102   F51  C~2r7L      
2015 05  22.55146  19 14 12.970  -24 51 40.80  22.6G 11HM102   F51  C~2r7L      
2015 05  25.56680  19 13 58.320  -24 52 55.69  22.9G 11HM102   F51  C~2r7L      
2015 06  10.54352  19 12 24.942  -24 59 49.37  23.4G 11HM102   F51  C~2r7L      
2016 07  05.47234  19 19 59.011  -26 09 06.49  22.3G 11HM102   F51  C~2r7L      
2016 08  03.38900  19 16 22.230  -26 20 55.86  22.9G 11HM102   F51  C~2r7L      
2017 05  26.55177  19 35 07.866  -26 43 01.62  22.8G 11HM102   F51  C~2r7L      
2017 06  23.49705  19 32 19.353  -26 57 41.31  22.8G 11HM102   F51  C~2r7L      
2017 07  26.37986  19 28 09.934  -27 13 22.74  22.3G 11HM102   F51  C~2r7L      
2017 08  13.33503  19 26 04.223  -27 19 53.23  23.1G 11HM102   F51  C~2r7L      
2018 05  24.57837  19 46 06.203  -27 31 29.76  23.1G 11HM102   F51  C~2r7L      

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     0.01
  2   0.0000      0.00    -0.01       0.00    -0.07
  3   0.0000      0.00    -0.07       0.00    -0.02
  4   0.0000      0.00     0.01       0.00     0.00
  5   0.0000      0.00     0.05       0.00     0.01
  6   0.0000      0.00    -0.06       0.00     0.02
  7   0.0000      0.00     0.02       0.00    -0.06
  8   0.0000      0.00    -0.05       0.00    -0.04
  9   0.0000      0.00    -0.04       0.00    -0.01
 10   0.0001      0.00     0.05       0.00     0.01
 11   0.0025      0.00    -0.01       0.00    -0.06
 12   0.0028      0.00     0.12       0.00    -0.08
 13   0.0028      0.00     0.05       0.00    -0.06
 14   0.0028      0.00    -0.01       0.00    -0.05
 15   0.0028      0.00     0.07       0.00    -0.03
 16   0.0028      0.00     0.00       0.00    -0.11
 17   0.0028      0.00     0.05       0.00    -0.00
 18   0.0028      0.00     0.09       0.00     0.01
 19   0.0029      0.00     0.02       0.00    -0.07
 20   0.0029      0.00     0.11       0.00    -0.06
 21   0.0029      0.00     0.04       0.00    -0.04
 22   0.0029      0.00     0.12       0.00    -0.02
 23   0.0825      0.00    -0.16       0.00    -0.11
 24   0.0829      0.00    -0.15       0.00    -0.21
 25   0.0853      0.00     0.12       0.00     0.14
 26   0.0879      0.00     0.03       0.00    -0.08
 27   0.0911      0.00     0.01       0.00    -0.08
 28   0.1719      0.00    -0.14       0.00     0.07
 29   0.1719      0.00    -0.22       0.00     0.10
 30   0.1719      0.00    -0.15       0.00     0.24
 31   0.1719      0.00    -0.07       0.00     0.07
 32   0.1719      0.00    -0.00       0.00     0.01
 33   0.1719      0.00    -0.08       0.00     0.05
 34   0.1719      0.00    -0.13       0.00    -0.04
 35   0.1719      0.00    -0.00       0.00     0.08
 36   0.1719      0.00    -0.08       0.00     0.02
 37   0.1719      0.00    -0.01       0.00     0.15
 38   0.1719      0.00    -0.09       0.00     0.09
 39   0.1721      0.00    -0.09       0.00     0.15
 40   0.1721      0.00    -0.02       0.00     0.09
 41   0.1721      0.00    -0.10       0.00     0.12
 42   0.1722      0.00    -0.02       0.00     0.06
 43   0.1722      0.00    -0.10       0.00    -0.01
 44   0.1722      0.00     0.11       0.00     0.03
 45   0.1722      0.00    -0.18       0.00     0.03
 46   0.1722      0.00    -0.11       0.00     0.06
 47   0.1722      0.00    -0.03       0.00    -0.00
 48   0.1722      0.00    -0.11       0.00     0.13
 49   0.1722      0.00     0.12       0.00     0.07
 50   0.1722      0.00     0.04       0.00    -0.10
 51   0.1724      0.00     0.02       0.00     0.09
 52   0.1724      0.00    -0.20       0.00     0.03
 53   0.1724      0.00    -0.13       0.00    -0.04
 54   0.1724      0.00    -0.06       0.00     0.10
 55   0.1724      0.00    -0.13       0.00     0.03
 56   0.1724      0.00     0.07       0.00    -0.04
 57   0.1724      0.00    -0.06       0.00    -0.03
 58   0.1724      0.00    -0.14       0.00     0.00
 59   0.1724      0.00    -0.07       0.00    -0.06
 60   0.1724      0.00    -0.15       0.00     0.07
 61   0.1724      0.00     0.08       0.00     0.00
 62   0.1724      0.00     0.00       0.00     0.04
 63   0.1726      0.00     0.11       0.00     0.01
 64   0.1726      0.00    -0.12       0.00     0.05
 65   0.1726      0.00     0.10       0.00    -0.12
 66   0.1726      0.00     0.03       0.00    -0.09
 67   0.1726      0.00     0.10       0.00    -0.05
 68   0.1726      0.00     0.02       0.00    -0.02
 69   0.1726      0.00     0.23       0.00     0.11
 70   0.1726      0.00    -0.06       0.00     0.02
 71   0.1726      0.00     0.01       0.00    -0.05
 72   0.1726      0.00    -0.07       0.00    -0.02
 73   0.1727      0.00     0.15       0.00     0.02
 74   0.1727      0.00    -0.08       0.00    -0.05
 75   0.1727      0.00     0.03       0.00    -0.01
 76   0.1727      0.00    -0.04       0.00     0.03
 77   0.1745      0.00     0.06       0.00     0.00
 78   0.1745      0.00    -0.02       0.00     0.04
 79   0.1745      0.00     0.05       0.00    -0.03
 80   0.1745      0.00     0.12       0.00     0.01
 81   0.1745      0.00     0.04       0.00    -0.05
 82   0.1745      0.00    -0.05       0.00    -0.02
 83   0.1745      0.00     0.12       0.00    -0.02
 84   0.1745      0.00     0.04       0.00     0.02
 85   0.1745      0.00    -0.04       0.00    -0.04
 86   0.1745      0.00     0.03       0.00    -0.01
 87   0.1745      0.00    -0.04       0.00     0.03
 88   0.1745      0.00     0.02       0.00    -0.04
 89   0.1748      0.00     0.04       0.00     0.01
 90   0.1748      0.00     0.11       0.00    -0.05
 91   0.1748      0.00     0.03       0.00    -0.02
 92   0.1748      0.00     0.11       0.00     0.02
 93   0.1748      0.00     0.03       0.00     0.05
 94   0.1748      0.00    -0.06       0.00    -0.01
 95   0.1748      0.00    -0.05       0.00    -0.01
 96   0.1748      0.00     0.03       0.00     0.02
 97   0.1748      0.00    -0.05       0.00    -0.04
 98   0.1748      0.00     0.02       0.00    -0.00
 99   0.1748      0.00    -0.05       0.00     0.03
100   0.1748      0.00     0.02       0.00    -0.03
101   0.1751      0.00     0.05       0.00     0.02
102   0.1751      0.00    -0.02       0.00    -0.04
103   0.1751      0.00     0.05       0.00    -0.01
104   0.1751      0.00     0.12       0.00    -0.07
105   0.1751      0.00     0.05       0.00    -0.04
106   0.1751      0.00    -0.01       0.00    -0.02
107   0.1751      0.00    -0.03       0.00    -0.00
108   0.1751      0.00     0.04       0.00     0.03
109   0.1751      0.00     0.11       0.00    -0.03
110   0.1751      0.00     0.03       0.00     0.00
111   0.1751      0.00    -0.04       0.00     0.04
112   0.1752      0.00     0.06       0.00     0.09
113   0.1753      0.00    -0.15       0.00    -0.08
114   0.1754      0.00    -0.02       0.00     0.03
115   0.1754      0.00     0.45       0.00    -0.27
116   0.1754      0.00     0.00       0.00     0.04
117   0.1754      0.00     0.20       0.00     0.06
118   0.1754      0.00     0.12       0.00    -0.00
119   0.1754      0.00     0.04       0.00     0.03
120   0.1754      0.00    -0.04       0.00     0.16
121   0.1754      0.00     0.05       0.00    -0.10
122   0.1755      0.00     0.03       0.00    -0.00
123   0.2630      0.00     0.11       0.00    -0.02
124   0.2630      0.00     0.10       0.00    -0.06
125   0.2630      0.00    -0.11       0.00    -0.09
126   0.3333      0.00     0.15       0.00     0.07
127   0.3334      0.00     0.02       0.00    -0.06
128   0.3336      0.00     0.15       0.00    -0.11
129   0.3360      0.00    -0.01       0.00    -0.22
130   0.3362      0.00    -0.18       0.00    -0.18
131   0.9691      0.00    -0.04       0.00     0.05
132   0.9692      0.00    -0.01       0.00     0.07
133   0.9692      0.00     0.02       0.00     0.09
134   0.9692      0.00    -0.11       0.00     0.01
135   0.9692      0.00     0.07       0.00     0.03
136   0.9692      0.00    -0.05       0.00     0.05
137   0.9692      0.00    -0.03       0.00     0.07
138   0.9692      0.00    -0.00       0.00     0.09
139   0.9692      0.00     0.03       0.00     0.11
140   0.9692      0.00     0.05       0.00     0.02
141   0.9692      0.00    -0.07       0.00     0.04
142   0.9692      0.00    -0.04       0.00     0.06
143   0.9692      0.00    -0.01       0.00     0.18
144   0.9692      0.00    -0.00       0.00    -0.01
145   0.9692      0.00     0.01       0.00     0.10
146   3.0205      0.00     0.14       0.00    -0.45
147   3.0206      0.00    -0.01       0.00    -0.07
148   3.0206      0.00     0.07       0.00    -0.05
149   3.0206      0.00    -0.00       0.00    -0.07
150   4.0637      0.00     0.01       0.00    -0.22
151   4.0719      0.00    -0.08       0.00     0.03
152   4.1157      0.00    -0.05       0.00     0.06
153   5.1860      0.00    -0.07       0.00     0.20
154   5.2651      0.00     0.06       0.00     0.07
155   6.0760      0.00     0.12       0.00    -0.19
156   6.1525      0.00    -0.13       0.00     0.17
157   6.2425      0.00     0.02       0.00     0.00
158   6.2917      0.00     0.04       0.00     0.04
159   7.0699      0.00    -0.00       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.

11HM102    quality flag:3

Type:            1:1       1:1       1:1

axisobj        29.989    29.989    29.989
ecceobj         0.077     0.077     0.077
incobj         29.407    29.407    29.407
qmin           26.535    26.535    26.535
qmax           33.774    33.774    33.774
amean          30.109    30.109    30.109
amin           29.855    29.855    29.855
amax           30.397    30.397    30.397
emean           0.088     0.088     0.088
emin            0.061     0.061     0.061
emax            0.115     0.115     0.115
imean          27.848    27.848    27.848
imin           27.595    27.595    27.596
imax           28.071    28.071    28.071
excite_mean     0.475     0.475     0.475
fracstop        1.000     1.000     1.000
cjmean          2.763     2.763     2.763

libcent 0       300.4     300.4     300.4
libamp  0        12.6      12.6      12.6
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       183.7     183.7     183.7
kozaiamp        180.0     180.0     180.0