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: 99CF119
# Created Wed Feb 20 02:07:50 2019
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting 42 observations of 42
# Arc: 15.97y
# First observation: 1999/02/11
# Last observation: 2015/02/01
# Chi-squared of fit: 160.41 DOF: 78 RMS: 0.35
# Min/Max residuals: -0.82 0.85
# Exact a, adot, b, bdot, g, gdot:
1.822172E-05 2.989363E-02 -3.587571E-06 -1.071887E-02 2.579902E-02 -4.553851E-03
# Covariance matrix:
8.6353E-14 -2.2904E-14 -9.1643E-15 6.2224E-15 -1.5915E-14 -3.3317E-14
-2.2904E-14 1.2843E-14 6.2134E-15 -4.2028E-15 2.6348E-15 2.2555E-14
-9.1643E-15 6.2134E-15 6.2472E-14 -7.7111E-15 5.8280E-16 1.1989E-14
6.2224E-15 -4.2028E-15 -7.7111E-15 2.6457E-15 -6.2147E-16 -8.1044E-15
-1.5915E-14 2.6348E-15 5.8280E-16 -6.2147E-16 1.1610E-13 2.6021E-15
-3.3317E-14 2.2555E-14 1.1989E-14 -8.1044E-15 2.6021E-15 4.3509E-14
# lat0 lon0 xBary yBary zBary JD0
0.489564 121.604216 -0.352641 0.007717 -0.928742 2451220.779063
# Heliocentric elements and errors
Epoch: 2451220.5000 = 1999/02/11
Mean Anomaly: 355.02132 +/- 0.001
Argument of Peri: 199.66668 +/- 0.002
Long of Asc Node: 303.43657 +/- 0.000
Inclination: 19.73435 +/- 0.000
Eccentricity: 0.56156965 +/- 0.0001
Semi-Major Axis: 88.34202965 +/- 0.0131
Time of Perihelion: 2455414.8163 +/- 66.7
Perihelion: 38.73182689 +/- 0.0077
Aphelion: 137.95223240 +/- 0.0211
Period (y) 830.3463 +/- 0.19
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X -21.09136910 +/- 0.0003
Ecliptic Y 33.61716152 +/- 0.0004
Ecliptic Z 0.33104909 +/- 0.0000
Ecliptic XDOT -0.00245542 +/- 0.0000
Ecliptic YDOT -0.00205677 +/- 0.0000
Ecliptic ZDOT -0.00114160 +/- 0.0000
# Distances at JD0 (AU)
Heliocenter to KBO 39.68723858 +/- 0.0004
Geocenter to KBO 38.76131019 +/- 0.0005
# Hcoef: 7.14
The following table shows the complete astrometric record for 99CF119. 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 (99CF119) followed by the observatory code and reference code for the source of the astrometry.
1999 02 11.27832 08 15 51.18 +20 16 48.2 23.0R 99CF119 568 Ca4178 1999 02 11.32043 08 15 50.97 +20 16 48.6 23.0R 99CF119 568 Ca4178 1999 02 17.24042 08 15 22.32 +20 17 41.7 23.0R 99CF119 568 Ca4178 1999 02 17.32277 08 15 21.91 +20 17 42.5 23.0R 99CF119 568 Ca4178 1999 04 08.26531 08 13 02.23 +20 19 32.0 23.1R 99CF119 568 Ca4843 1999 04 09.25789 08 13 01.82 +20 19 26.8 23.1R 99CF119 568 Ca4843 1999 05 06.25461 08 13 30.58 +20 14 56.8 23.3R 99CF119 568 Ca4843 1999 05 06.30545 08 13 30.72 +20 14 56.3 23.3R 99CF119 568 Ca4843 1999 12 29.61447 08 26 09.36 +19 09 03.1 99CF119 568 Ca8502 1999 12 29.63415 08 26 09.26 +19 09 03.4 99CF119 568 Ca8502 1999 12 30.60682 08 26 04.71 +19 09 13.3 99CF119 568 Ca8502 1999 12 31.43598 08 26 00.70 +19 09 22.1 22.8R 99CF119 695 Ca8502 1999 12 31.44434 08 26 00.72 +19 09 22.1 22.6R 99CF119 695 Ca8502 1999 12 31.51453 08 26 00.38 +19 09 22.6 99CF119 695 Ca8502 1999 12 31.52179 08 26 00.36 +19 09 22.7 99CF119 695 Ca8502 2000 01 29.12666 08 23 32.24 +19 14 49.5 99CF119 705 Ca9922 2000 01 29.15234 08 23 32.16 +19 14 49.5 99CF119 705 Ca9922 2000 01 29.18577 08 23 31.95 +19 14 50.2 22.9R 99CF119 705 Ca9922 2000 01 30.14579 08 23 26.84 +19 15 01.1 99CF119 705 Ca9922 2000 01 30.17000 08 23 26.70 +19 15 01.5 99CF119 705 Ca9922 2000 01 30.20438 08 23 26.51 +19 15 02.2 99CF119 705 Ca9922 2001 01 26.30391 08 30 13.81 +18 13 19.6 22.5R 99CF119 695 Cc6423 2001 01 26.37647 08 30 13.41 +18 13 20.4 99CF119 695 Cc6423 2002 04 10.30291 08 32 13.83 +17 21 11.6 99CF119 568 Ch3072 2002 04 10.34891 08 32 13.80 +17 21 11.5 99CF119 568 Ch3072 2002 04 11.25257 08 32 13.22 +17 21 09.7 99CF119 568 Ch3072 2002 04 11.26285 08 32 13.21 +17 21 09.9 99CF119 568 Ch3072 2005 03 10.226910 08 52 33.32 +14 07 38.5 99CF119 645 C~1cF1 2005 03 10.227743 08 52 33.31 +14 07 38.5 99CF119 645 C~1cF1 2005 03 10.230231 08 52 33.30 +14 07 38.5 99CF119 645 C~1cF1 2005 12 06.439912 09 05 43.85 +12 44 03.1 22.3V 99CF119 645 C~1cF2 2005 12 06.440741 09 05 43.85 +12 44 03.0 22.4V 99CF119 645 C~1cF2 2005 12 06.443229 09 05 43.84 +12 44 03.0 23.4V 99CF119 645 C~1cF2 2006 01 31.343332 09 01 55.60 +12 51 35.9 99CF119 645 C~1cF2 2006 01 31.344161 09 01 55.60 +12 51 35.9 99CF119 645 C~1cF2 2006 01 31.346649 09 01 55.58 +12 51 36.0 99CF119 645 C~1cF2 2013 03 12.13729 09 42 07.43 +05 03 05.6 22.0R 99CF119 695 C~0uco 2013 03 12.19997 09 42 07.16 +05 03 07.0 99CF119 695 C~0uco 2013 03 13.13373 09 42 03.17 +05 03 27.7 99CF119 695 C~0uco 2015 02 01.24277 09 57 25.15 +02 29 45.6 99CF119 W84 C~2KVJ 2015 02 01.31738 09 57 24.78 +02 29 46.6 23.2r 99CF119 W84 C~2KVJ 2015 02 01.32060 09 57 24.76 +02 29 46.6 99CF119 W84 C~2KVJ
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 -0.12 0.00 -0.60 2 0.0001 0.00 -0.08 0.00 -0.61 3 0.0163 0.00 0.28 0.00 -0.71 4 0.0165 0.00 0.03 0.00 -0.62 5 0.1533 0.00 0.20 0.00 -0.13 6 0.1560 0.00 0.04 0.00 0.08 7 0.2299 0.00 -0.41 0.00 0.00 8 0.2301 0.00 -0.14 0.00 0.25 9 0.8798 0.00 0.85 0.00 -0.57 10 0.8798 0.00 0.74 0.00 -0.46 11 0.8825 0.00 0.68 0.00 -0.13 12 0.8848 0.00 -0.82 0.00 0.43 13 0.8848 0.00 0.09 0.00 0.34 14 0.8850 0.00 0.06 0.00 0.15 15 0.8850 0.00 0.28 0.00 0.18 16 0.9633 0.00 -0.67 0.00 0.39 17 0.9634 0.00 0.20 0.00 0.08 18 0.9635 0.00 -0.25 0.00 0.38 19 0.9661 0.00 -0.32 0.00 -0.03 20 0.9662 0.00 -0.47 0.00 0.08 21 0.9663 0.00 -0.54 0.00 0.37 22 1.9576 0.00 0.25 0.00 0.74 23 1.9578 0.00 0.14 0.00 0.63 24 3.1595 0.00 0.16 0.00 0.48 25 3.1597 0.00 0.24 0.00 0.46 26 3.1621 0.00 0.14 0.00 0.16 27 3.1622 0.00 0.09 0.00 0.38 28 6.0752 0.00 0.10 0.00 -0.02 29 6.0752 0.00 0.00 0.00 -0.03 30 6.0752 0.00 -0.00 0.00 -0.06 31 6.8177 0.00 -0.29 0.00 -0.28 32 6.8177 0.00 -0.26 0.00 -0.38 33 6.8177 0.00 -0.33 0.00 -0.37 34 6.9707 0.00 -0.07 0.00 -0.34 35 6.9707 0.00 -0.01 0.00 -0.35 36 6.9708 0.00 -0.11 0.00 -0.29 37 14.0804 0.00 0.12 0.00 0.11 38 14.0806 0.00 0.17 0.00 0.11 39 14.0831 0.00 -0.01 0.00 0.04 40 15.9725 0.00 0.11 0.00 0.14 41 15.9727 0.00 -0.04 0.00 0.03 42 15.9727 0.00 -0.11 0.00 -0.02
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.
99CF119 quality flag:3 Type: SCATNEAR SCATNEAR SCATNEAR axisobj 88.990 88.990 88.991 ecceobj 0.565 0.565 0.565 incobj 19.710 19.710 19.710 qmin 37.065 37.089 37.113 qmax 143.844 144.200 143.825 amean 88.874 88.871 88.879 amin 87.465 87.466 87.489 amax 90.908 91.096 90.898 emean 0.568 0.568 0.568 emin 0.554 0.555 0.554 emax 0.583 0.583 0.582 imean 20.719 20.719 20.721 imin 19.972 19.979 19.987 imax 21.638 21.612 21.634 excite_mean 0.669 0.669 0.669 fracstop 1.000 1.000 1.000 cjmean 2.983 2.983 2.983 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 198.2 197.9 198.1 kozaiamp 180.0 180.0 180.0