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: 00OP67
# Created Thu Nov 21 02:08:07 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting 42 observations of 42
# Arc: 22.07y
# First observation: 2000/07/31
# Last observation: 2022/08/27
# Chi-squared of fit: 207.18 DOF: 78 RMS: 0.39
# Min/Max residuals: -0.68 1.22
# Exact a, adot, b, bdot, g, gdot:
1.534922E-05 2.783576E-02 -5.746541E-07 -2.867499E-04 2.647205E-02 4.536493E-03
# Covariance matrix:
1.5840E-13 -3.6170E-14 -6.5782E-16 3.4792E-16 4.8907E-14 -5.4006E-14
-3.6170E-14 1.5733E-14 3.5020E-16 -1.6088E-16 2.8979E-15 2.4731E-14
-6.5782E-16 3.5020E-16 6.5136E-14 -4.1633E-15 2.4504E-16 5.6661E-16
3.4792E-16 -1.6088E-16 -4.1633E-15 5.9689E-16 -1.4221E-17 -2.6336E-16
4.8907E-14 2.8979E-15 2.4504E-16 -1.4221E-17 1.1897E-13 1.0597E-15
-5.4006E-14 2.4731E-14 5.6661E-16 -2.6336E-16 1.0597E-15 4.0518E-14
# lat0 lon0 xBary yBary zBary JD0
0.489602 -36.321373 0.274797 0.008182 -0.976871 2451756.786433
# Heliocentric elements and errors
Epoch: 2451756.5000 = 2000/07/31
Mean Anomaly: 44.28580 +/- 0.008
Argument of Peri: 78.48010 +/- 0.011
Long of Asc Node: 182.73880 +/- 0.002
Inclination: 0.75085 +/- 0.000
Eccentricity: 0.18813219 +/- 0.0000
Semi-Major Axis: 43.71911811 +/- 0.0027
Time of Perihelion: 2438767.7463 +/- 2.6
Perihelion: 35.49414486 +/- 0.0025
Aphelion: 51.94409137 +/- 0.0034
Period (y) 289.0782 +/- 0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X 31.06553206 +/- 0.0004
Ecliptic Y -23.16963965 +/- 0.0003
Ecliptic Z 0.32275937 +/- 0.0000
Ecliptic XDOT 0.00207629 +/- 0.0000
Ecliptic YDOT 0.00204708 +/- 0.0000
Ecliptic ZDOT -0.00002550 +/- 0.0000
# Distances at JD0 (AU)
Heliocenter to KBO 38.75559621 +/- 0.0004
Geocenter to KBO 37.77563488 +/- 0.0005
# Hcoef: 7.48
The following table shows the complete astrometric record for 00OP67. 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 (00OP67) followed by the observatory code and reference code for the source of the astrometry.
2000 07 31.28569 21 43 20.43 -13 09 54.9 22.9R 00OP67 807 Cc0956 2000 07 31.36398 21 43 20.04 -13 09 56.9 00OP67 807 Cc0956 2000 08 25.09246 21 41 18.23 -13 20 18.1 22.5R 00OP67 807 Cc0956 2000 08 25.15870 21 41 17.89 -13 20 20.0 00OP67 807 Cc0956 2001 08 19.14746 21 47 59.74 -12 47 04.8 21.8R 00OP67 807 Cg3073 2001 08 19.22785 21 47 59.35 -12 47 07.0 00OP67 807 Cg3073 2002 08 05.41434 21 55 13.41 -12 10 13.9 23.1R 00OP67 568 Cp1807 2002 08 05.47702 21 55 13.10 -12 10 15.5 00OP67 568 Cp1807 2002 08 05.53639 21 55 12.81 -12 10 17.1 23.5R 00OP67 568 Cp1807 2002 08 08.39471 21 54 59.18 -12 11 29.4 00OP67 568 Cp1807 2002 08 10.25502 21 54 50.22 -12 12 16.5 21.8R 00OP67 807 Cg3073 2002 08 10.36021 21 54 49.68 -12 12 19.5 00OP67 807 Cg3073 2002 09 04.03803 21 52 49.82 -12 22 58.6 00OP67 950 Cp1807 2002 09 04.08518 21 52 49.60 -12 22 59.7 23.2R 00OP67 950 Cp1807 2002 09 04.11621 21 52 49.44 -12 23 00.6 00OP67 950 Cp1807 2002 11 05.13583 21 49 52.66 -12 39 09.3 00OP67 675 Cp1807 2002 11 06.16208 21 49 52.49 -12 39 12.1 00OP67 675 Cp1807 2002 11 09.24944 21 49 52.49 -12 39 14.9 00OP67 568 Cp1807 2002 11 09.25730 21 49 52.49 -12 39 15.0 00OP67 568 Cp1807 2002 11 10.26801 21 49 52.73 -12 39 14.6 00OP67 568 Cp1807 2002 11 10.27599 21 49 52.72 -12 39 14.8 00OP67 568 Cp1807 2003 10 28.06623 21 55 54.83 -12 08 17.3 00OP67 309 Cp1807 2003 10 28.14402 21 55 54.72 -12 08 17.8 00OP67 309 Cp1807 2003 10 29.02924 21 55 53.70 -12 08 23.3 00OP67 309 Cp1807 2003 10 29.10690 21 55 53.61 -12 08 24.2 00OP67 309 Cp1807 2004 08 12.40412 22 06 34.11 -11 11 05.0 00OP67 568 Cp1807 2004 08 12.43860 22 06 33.94 -11 11 05.8 23.8R 00OP67 568 Cp1807 2004 08 12.46886 22 06 33.80 -11 11 06.6 00OP67 568 Cp1807 2006 06 12.33973 22 21 20.94 -09 50 32.4 22.8R 00OP67 250 S~06AN 2006 06 12.34413 22 21 20.94 -09 50 32.4 00OP67 250 S~06AN 2006 06 12.40504 22 21 20.90 -09 50 32.7 00OP67 250 S~06AN 2006 06 12.40944 22 21 20.89 -09 50 32.7 00OP67 250 S~06AN 2014 09 26.21653 22 58 56.59 -06 14 44.3 22.7R 00OP67 695 C~1LJ2 2014 09 26.27874 22 58 56.33 -06 14 45.8 00OP67 695 C~1LJ2 2014 09 26.33550 22 58 56.09 -06 14 47.4 00OP67 695 C~1LJ2 2021 10 03.03994 23 33 56.69 -02 40 55.4 24.2V 00OP67 W84 C~552i 2021 10 03.08811 23 33 56.48 -02 40 56.8 24.5V 00OP67 W84 C~552i 2021 10 03.11320 23 33 56.38 -02 40 57.5 24.3V 00OP67 W84 C~552i 2021 10 03.16130 23 33 56.17 -02 40 58.8 24.4V 00OP67 W84 C~552i 2022 08 27.373410 23 41 28.330 -01 53 18.52 23.8G 00OP67 G37 C~5nDr 2022 08 27.406190 23 41 28.202 -01 53 19.25 00OP67 G37 C~5nDr 2022 08 27.440920 23 41 28.057 -01 53 20.31 00OP67 G37 C~5nDr
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 0.23 0.00 0.17
2 0.0002 0.00 0.07 0.00 0.05
3 0.0679 0.00 0.52 0.00 0.19
4 0.0681 0.00 0.37 0.00 -0.04
5 1.0510 0.00 -0.01 0.00 0.13
6 1.0512 0.00 0.21 0.00 0.00
7 2.0127 0.00 -0.44 0.00 -0.15
8 2.0128 0.00 -0.55 0.00 -0.17
9 2.0130 0.00 -0.60 0.00 -0.28
10 2.0208 0.00 -0.52 0.00 -0.17
11 2.0259 0.00 -0.20 0.00 0.18
12 2.0262 0.00 -0.55 0.00 -0.13
13 2.0938 0.00 0.05 0.00 -0.19
14 2.0939 0.00 0.14 0.00 -0.11
15 2.0940 0.00 -0.04 0.00 -0.24
16 2.2638 0.00 0.29 0.00 0.75
17 2.2666 0.00 0.66 0.00 -0.12
18 2.2751 0.00 -0.34 0.00 -0.48
19 2.2751 0.00 -0.35 0.00 -0.58
20 2.2778 0.00 -0.23 0.00 -0.47
21 2.2779 0.00 -0.41 0.00 -0.68
22 3.2410 0.00 0.34 0.00 0.46
23 3.2412 0.00 0.17 0.00 0.51
24 3.2437 0.00 0.08 0.00 1.22
25 3.2439 0.00 0.11 0.00 0.83
26 4.0332 0.00 -0.14 0.00 0.33
27 4.0333 0.00 -0.18 0.00 0.44
28 4.0334 0.00 -0.08 0.00 0.43
29 5.8646 0.00 0.74 0.00 -0.55
30 5.8646 0.00 0.79 0.00 -0.53
31 5.8648 0.00 0.87 0.00 -0.59
32 5.8648 0.00 0.77 0.00 -0.58
33 14.1545 0.00 -0.40 0.00 0.11
34 14.1547 0.00 -0.27 0.00 0.27
35 14.1548 0.00 -0.20 0.00 0.17
36 21.1739 0.00 0.12 0.00 0.08
37 21.1740 0.00 0.03 0.00 -0.01
38 21.1741 0.00 0.13 0.00 -0.03
39 21.1742 0.00 0.05 0.00 -0.03
40 22.0728 0.00 -0.10 0.00 -0.10
41 22.0729 0.00 -0.00 0.00 0.03
42 22.0730 0.00 -0.04 0.00 -0.12
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.
00OP67 quality flag:3 Type: 7:4EEE 7:4EEE 7:4EEE axisobj 43.815 43.815 43.815 ecceobj 0.189 0.189 0.189 incobj 0.751 0.751 0.751 qmin 34.573 34.574 34.572 qmax 53.434 53.431 53.437 amean 43.727 43.727 43.727 amin 43.306 43.306 43.306 amax 44.220 44.219 44.220 emean 0.194 0.194 0.194 emin 0.179 0.179 0.179 emax 0.209 0.209 0.209 imean 1.801 1.800 1.802 imin 1.494 1.500 1.488 imax 2.051 2.045 2.058 excite_mean 0.196 0.196 0.196 fracstop 1.000 1.000 1.000 cjmean 3.052 3.052 3.052 libcent 0 177.9 177.9 178.4 libamp 0 64.1 63.8 64.0 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 202.1 202.2 202.0 kozaiamp 179.9 180.0 180.0