Orbit Fit and Astrometric record for 20TZ114

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: 20TZ114   
# Created Sun Oct 19 01:12:10 2025
# Orbit generated by ELGB
# -->Covariance matrix from a Bernstein fit
# Fitting     45 observations of     48
# Arc:  19.98y
# First observation: 2005/09/25
#  Last observation: 2025/09/17
# Chi-squared of fit:   620.20 DOF:     84 RMS:  0.66
# Min/Max residuals:    -2.04    1.83
# Exact a, adot, b, bdot, g, gdot:
  1.592624E-05  2.551913E-02  3.629967E-06  5.141478E-03  2.603526E-02  1.216361E-03
# Covariance matrix:
  4.8506E-13 -5.5055E-14  1.4734E-14 -6.4737E-15 -4.0374E-14 -5.6957E-14
 -5.5055E-14  1.5201E-14 -6.0656E-15  2.7928E-15  2.2722E-14  2.4439E-14
  1.4734E-14 -6.0656E-15  4.1149E-13 -2.4240E-14 -6.0971E-15 -1.0815E-14
 -6.4737E-15  2.7928E-15 -2.4240E-14  1.9560E-15  4.6281E-15  4.9415E-15
 -4.0374E-14  2.2722E-14 -6.0971E-15  4.6281E-15  1.0976E-13  3.8699E-14
 -5.6957E-14  2.4439E-14 -1.0815E-14  4.9415E-15  3.8699E-14  4.3280E-14
#      lat0       lon0       xBary       yBary       zBary        JD0
   11.765153   -7.368422   -0.167703    0.202555   -0.972083  2453638.691214
# Heliocentric elements and errors
Epoch:              2453638.5000  =  2005/09/25
Mean Anomaly:           92.74321 +/-     0.043
Argument of Peri:      307.25167 +/-     0.037
Long of Asc Node:      308.20112 +/-     0.000
Inclination:            16.09982 +/-     0.000
Eccentricity:         0.05115842 +/-    0.0000
Semi-Major Axis:     39.18091717 +/-    0.0018
Time of Perihelion: 2430560.9370 +/-      10.7
Perihelion:          37.17648324 +/-    0.0017
Aphelion:            41.18535111 +/-    0.0019
Period (y)              245.2563 +/-      0.02
# Ecliptic coordinates at JD0 (AU and AU/d)
Ecliptic X           38.29422040 +/-    0.0005
Ecliptic Y           -4.78448057 +/-    0.0001
Ecliptic Z            7.83187361 +/-    0.0001
Ecliptic XDOT         0.00036101 +/-    0.0000
Ecliptic YDOT         0.00265289 +/-    0.0000
Ecliptic ZDOT         0.00055541 +/-    0.0000
# Distances at JD0 (AU)
Heliocenter to KBO   39.37860320 +/-    0.0005
Geocenter to KBO     38.40945845 +/-    0.0005
# Hcoef:  5.44

The following table shows the complete astrometric record for 20TZ114. 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 (20TZ114) followed by the observatory code and reference code for the source of the astrometry.

2005 09  25.190471 23 14 16.76   +07 52 55.0   21.8r 20TZ114   645  C~93U1      
2005 09  25.191301 23 14 16.76   +07 52 55.0   21.3i 20TZ114   645  C~93U1      
2005 09  25.193788 23 14 16.76   +07 52 55.0   22.6g 20TZ114   645  C~93U1      
2017 07  22.36368  00 18 41.62   +17 43 33.1         20TZ114   W84  C~93U1      
2017 07  22.36714  00 18 41.62   +17 43 33.3   21.5r 20TZ114   W84  C~93U1      
2020 10  07.332167 00 29 17.235  +19 43 38.35  21.2G 20TZ114   G96  C~93U1      
2020 10  07.337293 00 29 17.187  +19 43 36.74  21.5G 20TZ114   G96  C~93U1      
2020 10  23.183861 00 28 00.852  +19 35 00.82  20.9G 20TZ114   G96  C~93U1      
2020 10  23.195007 00 28 00.722  +19 34 59.40  20.7G 20TZ114   G96  C~93U1      
2020 10  23.200583 00 28 00.672  +19 34 58.39  21.1G 20TZ114   G96  C~93U1      
2022 01  06.074888 00 30 52.593  +19 41 21.85  21.4G 20TZ114   G96  C~93U1      
2022 01  06.080612 00 30 52.722  +19 41 20.11  21.1G 20TZ114   G96  C~93U1      
2022 09  25.323991 00 40 58.182  +21 15 07.92  20.8G 20TZ114   G96  C~93U1      
2022 09  25.329128 00 40 58.105  +21 15 07.02  21.4G 20TZ114   G96  C~93U1      
2022 09  25.334271 00 40 57.939  +21 15 06.88  20.5G 20TZ114   G96  C~93U1      
2022 09  25.339410 00 40 57.920  +21 15 06.73  20.6G 20TZ114   G96  C~93U1      
2022 10  17.233105 00 39 08.050  +21 04 54.35  21.4G 20TZ114   G96  C~93U1      
2022 10  17.238692 00 39 08.037  +21 04 54.33  21.3G 20TZ114   G96  C~93U1      
2022 10  17.244279 00 39 07.944  +21 04 53.95  21.1G 20TZ114   G96  C~93U1      
2022 10  25.202673 00 38 29.814  +21 00 28.22  21.5G 20TZ114   G96  C~93U1      
2022 10  25.207845 00 38 29.738  +21 00 27.16  21.5G 20TZ114   G96  C~93U1      
2022 10  25.213034 00 38 29.734  +21 00 27.02  21.6G 20TZ114   G96  C~93U1      
2022 11  15.234718 00 37 03.006  +20 47 56.88  21.2G 20TZ114   G96  C~93U1      
2022 11  15.239898 00 37 02.945  +20 47 56.82  21.2G 20TZ114   G96  C~93U1      
2022 11  15.250254 00 37 02.725  +20 47 55.37  21.3G 20TZ114   G96  C~93U1      
2022 11  28.166395 00 36 24.447  +20 40 23.76  21.0G 20TZ114   G96  C~93U1      
2022 11  28.177779 00 36 24.432  +20 40 23.16  21.3G 20TZ114   G96  C~93U1      
2022 11  28.183471 00 36 24.377  +20 40 23.07  20.8G 20TZ114   G96  C~93U1      
2022 12  25.092144 00 35 52.833  +20 27 27.63  21.6G 20TZ114   G96  C~93U1      
2022 12  25.103766 00 35 52.871  +20 27 23.61  21.5G 20TZ114   G96  C~93U1      
2024 01  10.071733 00 41 20.235  +21 04 15.81  21.0G 20TZ114   G96  C~93U1      
2024 01  10.077546 00 41 20.339  +21 04 15.01  21.7G 20TZ114   G96  C~93U1      
2024 01  10.083368 00 41 20.364  +21 04 13.56  20.9G 20TZ114   G96  C~93U1      
2024 09  23.393042 00 51 52.897  +22 38 40.39  21.3G 20TZ114   G96  C~93U1      
2024 09  23.398185 00 51 52.876  +22 38 40.04  21.4G 20TZ114   G96  C~93U1      
2024 09  23.403337 00 51 52.780  +22 38 39.99  20.7G 20TZ114   G96  C~93U1      
2024 10  11.330855 00 50 22.006  +22 31 15.88  21.7G 20TZ114   G96  C~93U1      
2024 10  11.336080 00 50 21.796  +22 31 14.57  21.6G 20TZ114   G96  C~93U1      
2024 10  28.181988 00 48 58.774  +22 22 13.40  21.3G 20TZ114   G96  C~93U1      
2024 10  28.187257 00 48 58.766  +22 22 12.47  21.4G 20TZ114   G96  C~93U1      
2025 08  23.437300 00 59 31.578  +23 23 36.30  22.0w 20TZ114   F52  C~9501      
2025 08  23.449340 00 59 31.539  +23 23 36.39  22.0w 20TZ114   F52  C~9501      
2025 08  23.461434 00 59 31.505  +23 23 36.45  21.7w 20TZ114   F52  C~9501      
2025 08  23.473541 00 59 31.441  +23 23 36.46  22.1w 20TZ114   F52  C~9501      
2025 09  17.423365 00 57 49.753  +23 20 48.89  21.8w 20TZ114   F52  C~98Sa      
2025 09  17.436294 00 57 49.702  +23 20 48.73  21.8w 20TZ114   F52  C~98Sa      
2025 09  17.449267 00 57 49.637  +23 20 48.15  21.8w 20TZ114   F52  C~98Sa      
2025 09  17.462311 00 57 49.566  +23 20 48.16  21.6w 20TZ114   F52  C~98Sa      

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    -0.04       0.00    -0.13
     2   0.0000      0.00     0.02       0.00    -0.11
     3   0.0000      0.00     0.20       0.00    -0.03
     4  11.8225      0.00    -0.17       0.00    -0.08
     5  11.8225      0.00    -0.09       0.00     0.07
     6  15.0339      0.00     0.33       0.00     1.39
     7  15.0339      0.00     0.00       0.00    -0.06
     8  15.0773      0.00     0.94       0.00     1.67
     9  15.0774      0.00    -0.23       0.00     0.64
    10  15.0774      0.00    -0.60       0.00    -0.18
    11  16.2817      0.00    -0.44       0.00    -0.10
    12  16.2817      0.00     1.37       0.00    -1.76
    13  16.9997      0.00     0.82       0.00     0.82
    14  16.9997      0.00     0.06       0.00     0.04
    15  16.9997      0.00    -2.04       0.00     0.01
    16  16.9997      0.00    -1.93       0.00    -0.02
    17  17.0597      0.00     0.07       0.00    -0.48
    18  17.0597      0.00     0.29       0.00    -0.32
    19  17.0597      0.00    -0.68       0.00    -0.52
    20  17.0815      0.00     0.06       0.00     0.22
    21  17.0815      0.00    -0.71       0.00    -0.66
    22  17.0815      0.00    -0.40       0.00    -0.62
    23  17.1391      0.00     0.76       0.00     0.02
    24  17.1391      0.00     0.12       0.00     0.15
    25  17.1391      0.00 (  -2.63)      0.00 (  -0.93)
    26  17.1745      0.00     0.14       0.00     0.33
    27  17.1745      0.00     0.34       0.00     0.12
    28  17.1745      0.00    -0.27       0.00     0.22
    29  17.2482      0.00 (  -2.34)      0.00 (   1.65)
    30  17.2482      0.00 (  -1.79)      0.00 (  -2.10)
    31  18.2913      0.00    -0.91       0.00     0.51
    32  18.2913      0.00     0.51       0.00    -0.20
    33  18.2913      0.00     0.75       0.00    -1.57
    34  18.9958      0.00     1.12       0.00    -0.09
    35  18.9958      0.00     1.19       0.00    -0.33
    36  18.9958      0.00     0.14       0.00    -0.28
    37  19.0449      0.00     1.83       0.00     0.79
    38  19.0449      0.00    -0.91       0.00    -0.36
    39  19.0910      0.00    -0.55       0.00     0.19
    40  19.0910      0.00    -0.30       0.00    -0.56
    41  19.9103      0.00    -0.15       0.00     0.11
    42  19.9104      0.00    -0.13       0.00     0.18
    43  19.9104      0.00    -0.03       0.00     0.21
    44  19.9104      0.00    -0.38       0.00     0.19
    45  19.9787      0.00    -0.16       0.00     0.22
    46  19.9788      0.00     0.00       0.00     0.25
    47  19.9788      0.00    -0.03       0.00    -0.13
    48  19.9788      0.00    -0.16       0.00     0.07

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.

20TZ114    quality flag:3

Type:           3:2E      3:2E      3:2E

axisobj        39.538    39.538    39.538
ecceobj         0.048     0.048     0.048
incobj         16.086    16.086    16.086
qmin           35.823    35.850    35.866
qmax           43.360    43.393    43.385
amean          39.463    39.463    39.463
amin           39.084    39.086    39.091
amax           39.843    39.863    39.843
emean           0.062     0.062     0.063
emin            0.038     0.037     0.038
emax            0.091     0.091     0.091
imean          17.466    17.464    17.463
imin           16.781    16.744    16.732
imax           18.119    18.119    18.119
excite_mean     0.307     0.307     0.307
fracstop        1.000     1.000     1.000
cjmean          2.942     2.942     2.942

libcent 0       180.8     180.9     180.7
libamp  0        91.7      91.7      91.6
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       180.2     179.0     179.6
kozaiamp        180.0     180.0     180.0