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Photocenter Correction

Optical comet astrometry can measure a center of light that is not the comet center of mass.1 In DiffOrb, the propagated state still represents the center of mass. A photocenter correction changes only the modeled optical direction before right ascension and declination are formed.

DiffOrb uses a scalar global form of the S0 offset model used in comet orbit fitting:21

offset_distance = S0 / r_h**2

S0 is in km. r_h is the heliocentric distance in au. A positive S0 moves the modeled optical point away from the Sun along the Sun-comet direction. JPL SBDB also exposes S0 as an orbit model parameter field for small-body solutions.3

The correction applies to optical right ascension and declination. It does not change the propagated orbit, force model, radar delay, or radar Doppler prediction. S0 is therefore an optical observation-model parameter, not a dynamical acceleration parameter.

References


  1. Farnocchia, D., Bellerose, J., Bhaskaran, S., Micheli, M., & Weryk, R. (2021). High-fidelity comet 67P ephemeris and predictions based on Rosetta data. Icarus, 358, 114276. https://doi.org/10.1016/j.icarus.2020.114276 

  2. Yeomans, D. K. (1994). A review of comets and nongravitational forces. In A. Milani, M. di Martino, & A. Cellino (eds.), Asteroids, Comets, Meteors 1993, IAU Symposium, Vol. 160, 241-254. https://doi.org/10.1017/S007418090004657X 

  3. NASA/JPL Solar System Dynamics. SBDB API documents orbit model_pars; SBDB Query API lists S0 and S0_sigma as query fields. https://ssd-api.jpl.nasa.gov/doc/sbdb.html and https://ssd-api.jpl.nasa.gov/doc/sbdb_query.html