Orbit Fit and Astrometric record for 99CC119

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: 99CC119   
# Created Sat Apr 20 01:09:48 2024
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     34 observations of     34
# Arc:  24.10y
# First observation: 1999/02/10
#  Last observation: 2023/03/18
# Chi-squared of fit:    55.26 DOF:     62 RMS:  0.23
# Min/Max residuals:    -0.47    0.55
# Exact a, adot, b, bdot, g, gdot:
  1.481709E-05  2.168110E-02  1.296982E-06  1.582110E-04  2.295855E-02 -1.396299E-03
# Covariance matrix:
  1.3567E-13 -1.8717E-14  1.6696E-16 -1.0841E-16  5.8318E-14 -2.7670E-14
 -1.8717E-14  7.3014E-15 -9.8526E-17  5.1201E-17 -1.4987E-15  1.2899E-14
  1.6696E-16 -9.8526E-17  8.1046E-14 -4.5414E-15 -6.2419E-17 -1.8548E-16
 -1.0841E-16  5.1201E-17 -4.5414E-15  4.9509E-16 -1.5170E-17  9.7083E-17
  5.8318E-14 -1.4987E-15 -6.2419E-17 -1.5170E-17  1.2172E-13 -4.6119E-15
 -2.7670E-14  1.2899E-14 -1.8548E-16  9.7083E-17 -4.6119E-15  2.4469E-14
#      lat0       lon0       xBary       yBary       zBary        JD0
   -0.182752  167.816780    0.439449   -0.003067   -0.890755  2451219.944403
# Heliocentric elements and errors
Epoch:              2451220.5000  =  1999/02/11
Mean Anomaly:          275.32646 +/-     0.030
Argument of Peri:       69.88471 +/-     0.036
Long of Asc Node:      190.41075 +/-     0.002
Inclination:             0.45517 +/-     0.000
Eccentricity:         0.07301516 +/-    0.0000
Semi-Major Axis:     44.50638223 +/-    0.0027
Time of Perihelion: 2476728.5382 +/-      11.7
Perihelion:          41.25674180 +/-    0.0025
Aphelion:            47.75602267 +/-    0.0029
Period (y)              296.9215 +/-      0.03
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X          -43.34535559 +/-    0.0006
Ecliptic Y            9.80908366 +/-    0.0001
Ecliptic Z           -0.13886973 +/-    0.0000
Ecliptic XDOT        -0.00038462 +/-    0.0000
Ecliptic YDOT        -0.00255340 +/-    0.0000
Ecliptic ZDOT         0.00001940 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   44.44166357 +/-    0.0006
Geocenter to KBO     43.55683712 +/-    0.0007
# Hcoef:  7.18

The following table shows the complete astrometric record for 99CC119. 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 (99CC119) followed by the observatory code and reference code for the source of the astrometry.

1999 02  10.44366  11 14 53.77   +04 38 49.8   22.9R 99CC119   568  Ca4178      
1999 02  10.48439  11 14 53.60   +04 38 51.0   22.9R 99CC119   568  Ca4178      
1999 02  17.62044  11 14 25.71   +04 41 47.7   22.9R 99CC119   568  Ca4178      
1999 02  17.63204  11 14 25.66   +04 41 47.8   22.9R 99CC119   568  Ca4178      
1999 04  13.42497  11 10 43.24   +05 05 20.5   23.2R 99CC119   568  Ca4506      
1999 04  13.49906  11 10 43.00   +05 05 22.0   23.2R 99CC119   568  Ca4506      
2000 04  07.43238  11 15 37.08   +04 34 56.8   24.0R 99CC119   568  Cb6452      
2000 04  07.47644  11 15 36.90   +04 34 58.1   24.0R 99CC119   568  Cb6452      
2000 05  30.31788  11 13 52.17   +04 46 17.4   23.2R 99CC119   568  Cb6452      
2000 05  31.32402  11 13 52.21   +04 46 17.6   23.4R 99CC119   568  Cb6452      
2000 06  01.33507  11 13 52.33   +04 46 17.2   23.5R 99CC119   568  Cb6452      
2000 12  23.498728 11 25 49.15   +03 30 31.0         99CC119   645  C~1cF1      
2000 12  23.499557 11 25 49.15   +03 30 31.0         99CC119   645  C~1cF1      
2000 12  23.502045 11 25 49.15   +03 30 31.0         99CC119   645  C~1cF1      
2001 04  16.132769 11 19 44.30   +04 09 24.2         99CC119   645  C~1cF1      
2001 04  16.133598 11 19 44.30   +04 09 24.2         99CC119   645  C~1cF1      
2001 04  16.136086 11 19 44.29   +04 09 24.3         99CC119   645  C~1cF1      
2002 02  05.56427  11 28 59.77   +03 10 40.8   23.4R 99CC119   568  Cf1463      
2002 02  05.62465  11 28 59.57   +03 10 42.4         99CC119   568  Cf1463      
2006 01  07.506279 11 48 37.87   +01 06 18.8         99CC119   645  C~1cF1      
2006 01  07.507108 11 48 37.87   +01 06 18.8         99CC119   645  C~1cF1      
2006 01  07.509596 11 48 37.87   +01 06 18.8         99CC119   645  C~1cF1      
2013 03  12.29066  12 18 31.85   -02 03 19.5   23.7R 99CC119   G37  C~0qSP      
2013 03  12.42526  12 18 31.25   -02 03 16.2         99CC119   G37  C~0qSP      
2016 04  09.150544 12 31 00.29   -03 21 42.2         99CC119   W84  C~3i8v      
2016 04  09.160596 12 31 00.25   -03 21 42.2         99CC119   W84  C~3i8v      
2016 04  09.161632 12 31 00.28   -03 21 42.1         99CC119   W84  C~3i8v      
2017 03  02.248461 12 38 32.86   -04 09 22.9         99CC119   W84  C~3i8v      
2017 03  02.251204 12 38 32.86   -04 09 22.6         99CC119   W84  C~3i8v      
2019 04  05.217070 12 46 01.485  -04 55 27.57  23.3G 99CC119   G37  C~34bV      
2019 04  05.288400 12 46 01.150  -04 55 25.89        99CC119   G37  C~34bV      
2023 03  18.392080 13 07 07.536  -07 04 20.10  23.4G 99CC119   G37  C~6V2V      
2023 03  18.431560 13 07 07.403  -07 04 18.43        99CC119   G37  C~6V2V      
2023 03  18.473700 13 07 07.173  -07 04 17.20        99CC119   G37  C~6V2V      

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    -0.07       0.00    -0.23
     2   0.0001      0.00    -0.27       0.00    -0.01
     3   0.0196      0.00     0.03       0.00     0.17
     4   0.0197      0.00    -0.01       0.00    -0.03
     5   0.1697      0.00    -0.24       0.00     0.55
     6   0.1699      0.00    -0.09       0.00     0.49
     7   1.1553      0.00     0.36       0.00    -0.33
     8   1.1555      0.00     0.11       0.00    -0.05
     9   1.3001      0.00     0.13       0.00     0.02
    10   1.3029      0.00     0.18       0.00     0.11
    11   1.3057      0.00     0.16       0.00     0.13
    12   1.8674      0.00    -0.08       0.00    -0.33
    13   1.8674      0.00    -0.08       0.00    -0.33
    14   1.8674      0.00    -0.07       0.00    -0.33
    15   2.1785      0.00     0.02       0.00    -0.13
    16   2.1785      0.00     0.07       0.00    -0.15
    17   2.1785      0.00     0.04       0.00    -0.10
    18   2.9873      0.00    -0.13       0.00     0.02
    19   2.9875      0.00    -0.01       0.00     0.31
    20   6.9078      0.00     0.01       0.00     0.02
    21   6.9078      0.00     0.03       0.00     0.02
    22   6.9078      0.00     0.07       0.00     0.00
    23  14.0831      0.00     0.37       0.00     0.32
    24  14.0835      0.00    -0.00       0.00    -0.06
    25  17.1600      0.00    -0.39       0.00     0.31
    26  17.1601      0.00    -0.33       0.00     0.03
    27  17.1601      0.00     0.18       0.00     0.10
    28  18.0556      0.00    -0.27       0.00    -0.33
    29  18.0556      0.00    -0.11       0.00    -0.09
    30  20.1472      0.00     0.28       0.00     0.04
    31  20.1474      0.00     0.02       0.00    -0.27
    32  24.0984      0.00     0.01       0.00    -0.47
    33  24.0985      0.00     0.48       0.00     0.20
    34  24.0986      0.00    -0.35       0.00     0.37

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.

99CC119    quality flag:3

Type:      CLASSICAL CLASSICAL CLASSICAL

axisobj        44.579    44.579    44.579
ecceobj         0.072     0.072     0.072
incobj          0.457     0.457     0.457
qmin           40.931    40.918    40.911
qmax           48.938    48.935    48.941
amean          44.829    44.829    44.829
amin           44.479    44.463    44.473
amax           45.205    45.203    45.207
emean           0.070     0.070     0.070
emin            0.055     0.055     0.055
emax            0.083     0.083     0.083
imean           1.999     1.999     1.999
imin            1.380     1.380     1.380
imax            2.523     2.521     2.524
excite_mean     0.078     0.078     0.078
fracstop        1.000     1.000     1.000
cjmean          3.104     3.104     3.104

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       165.4     165.4     165.7
kozaiamp        180.0     180.0     179.9