Atmospheric Lensing and Oblateness Effects during an Extrasolar Planetary Transit

Future high-precision photometric measurements of transiting extrasolar planets promise to tell us much about the characteristics of these systems. We examine how atmospheric lensing and (projected) planet oblateness/ellipticity modify transit light curves. The large density gradients expected in planet atmospheres can offset the unfavorably large observer lens-to-source lens distance ratio and allow the existence of caustics. Under such conditions of strong lensing, which we quantify with an analytic expression, starlight from all points in the planet's shadow is refracted into view, producing a characteristic slowing down of the dimming at ingress (vice versa for egress). A search over several parameters, such as the limb-darkening profile, the planet radius, the transit speed, and the transit geometry, cannot produce a nonlensed transit light curve that can mimic a lensed light curve. The fractional change in the diminution of starlight is approximately the ratio of atmospheric scale height to planet radius, expected to be 1% or less. The lensing signal varies strongly with wavelength—caustics are hidden at wave bands where absorption and scattering are strong. Planet oblateness induces an asymmetry to the transit light curve about the point of minimum flux, which varies with the planet orientation with respect to the direction of motion. The fractional asymmetry is at the level of 0.5% for a projected oblateness of 10%, independent of whether or not lensing is important. For favorable ratios of planet radius to stellar radius (i.e., gas giant planets), the above effects are potentially observable with future space-based missions. Such measurements could constrain the planet shape and its atmospheric scale height, density, and refractive coefficient, providing information on its rotation, temperature, and composition. We have examined a large range of planetary system parameter space including the planetary scale height and orbital distance. For HD 209458b, the only currently known transiting extrasolar planet, caustics are absent because of the very small lens-source separation (and a large scale height caused by a high temperature from the small separation). Its oblateness is also expected to be small because of the tidal locking of its rotation to orbital motion. Finally, we provide estimates of other variations to transit light curves that could be of comparable importance—including rings, satellites, stellar oscillations, star spots, and weather.

[1]  John David Jackson,et al.  Classical Electrodynamics , 2020, Nature.

[2]  E. Wolf,et al.  Principles of Optics , 2019 .

[3]  Paolo Farinella,et al.  Physics of the earth and the solar system , 2011 .

[4]  J. Webb,et al.  Could We Detect O2 in the Atmosphere of a Transiting Extra-solar Earth-like Planet? , 2001, Publications of the Astronomical Society of Australia.

[5]  A. Burrows,et al.  Hubble Space Telescope Time-Series Photometry of the Transiting Planet of HD 209458 , 2001, astro-ph/0101336.

[6]  T. Brown Transmission Spectra as Diagnostics of Extrasolar Giant Planet Atmospheres , 2001, astro-ph/0101307.

[7]  A. Burrows,et al.  Theory of Extrasolar Giant Planet Transits , 2001, astro-ph/0101024.

[8]  S. Jha,et al.  Multicolor Observations of a Planetary Transit of HD 209458 , 2000, astro-ph/0007245.

[9]  Marley,et al.  On the Radii of Close-in Giant Planets , 2000, The Astrophysical journal.

[10]  R. P. Butler,et al.  A Transiting “51 Peg-like” Planet , 2000, The Astrophysical journal.

[11]  J. B. Laird,et al.  The Spectroscopic Orbit of the Planetary Companion Transiting HD 209458 , 2000, The Astrophysical journal.

[12]  Princeton,et al.  Theoretical Transmission Spectra during Extrasolar Giant Planet Transits , 1999, astro-ph/9912241.

[13]  T. Brown,et al.  Detection of Planetary Transits Across a Sun-like Star , 1999, The Astrophysical journal.

[14]  M. Born,et al.  Principles of optics : electromagnetic theory of propagation, interference and diffraction of light , 1999 .

[15]  P. Sartoretti,et al.  On the detection of satellites of extrasolar planets with the method of transits , 1999 .

[16]  B. Draine Lensing of Stars by Spherical Gas Clouds , 1998, astro-ph/9805083.

[17]  S. Tremaine,et al.  Migrating planets , 1998, Science.

[18]  W. Hubbard Lensing by Triton's Atmosphere , 1997, Science.

[19]  James L. Elliot,et al.  PROBING PLANETARY ATMOSPHERES WITH STELLAR OCCULTATIONS , 1996 .

[20]  J. Schneider,et al.  On the search for O 2 in extrasolar planets , 1994 .

[21]  Philip D. Nicholson,et al.  Saturn's Central Flash from the 3 July 1989 Occultation of 28 Sgr at McDonald and Palomar Observatories , 1993 .

[22]  B. Shustov Protostars and Planets II , 1987 .

[23]  P. Gierasch,et al.  Diffraction calculation of occultation light curves in the presence of an isothermal atmosphere. , 1976 .

[24]  C. Sagan,et al.  Occultation of beta Scorpii by Jupiter. V - The emersion of beta Scorpii C , 1975 .

[25]  T. Teichmann,et al.  Fundamentals of celestial mechanics , 1963 .

[26]  John Scott Drilling,et al.  in Allen''''s Astrophysical Quantities , 2000 .

[27]  C. Alcock Gravitational lenses , 1982, Nature.

[28]  Jean Connelly,et al.  Discovering the Solar System. , 1975 .