2005MNRAS.359..567A


Query : 2005MNRAS.359..567A

2005MNRAS.359..567A - Mon. Not. R. Astron. Soc., 359, 567-579 (2005/May-2)

On detecting terrestrial planets with timing of giant planet transits.

AGOL E., STEFFEN J., SARI R. and CLARKSON W.

Abstract (from CDS):

The transits of a distant star by a planet on a Keplerian orbit occur at time intervals exactly equal to the orbital period. If a second planet orbits the same star, the orbits are not Keplerian and the transits are no longer exactly periodic. We compute the magnitude of the variation in the timing of the transits, δt. We investigate analytically several limiting cases: (i) interior perturbing planets with much smaller periods; (ii) exterior perturbing planets on eccentric orbits with much larger periods; (iii) both planets on circular orbits with arbitrary period ratio but not in resonance; (iv) planets on initially circular orbits locked in resonance. Using subscripts `out' and `in' for the exterior and interior planets, µ for planet-to-star mass ratio and the standard notation for orbital elements, our findings in these cases are as follows. (i) Planet-planet perturbations are negligible. The main effect is the wobble of the star due to the inner planet, and therefore δt∼µin(ain/aout)Pout. (ii) The exterior planet changes the period of the interior planet by µout(ain/rout)3Pin. As the distance of the exterior planet changes due to its eccentricity, the inner planet's period changes. Deviations in its transit timing accumulate over the period of the outer planet, and therefore δt∼µouteout(ain/aout)3Pout. (iii) Halfway between resonances the perturbations are small, of the order of µouta2in/(ain-aout)2Pinfor the inner planet (switch `out' and `in' for the outer planet). This increases as one gets closer to a resonance. (iv) This is perhaps the most interesting case because some systems are known to be in resonances and the perturbations are the largest. As long as the perturber is more massive than the transiting planet, the timing variations would be of the order of the period regardless of the perturber mass. For lighter perturbers, we show that the timing variations are smaller than the period by the perturber-to-transiting-planet mass ratio. An earth-mass planet in 2:1 resonance with a three-dimensional period transiting planet (e.g. HD 209458b) would cause timing variations of the order of 3 min, which would be accumulated over a year. This signal of a terrestrial planet is easily detectable with current ground-based measurements.

For the case in which both planets are on eccentric orbits, we compute numerically the transit timing variations for several known multiplanet systems, assuming they are edge-on. Transit timing measurements may be used to constrain the masses, radii and orbital elements of planetary systems, and, when combined with radial velocity measurements, provide a new means of measuring the mass and radius of the host star.


Abstract Copyright: 2005 RAS

Journal keyword(s): eclipses - planetary systems

Simbad objects: 22

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Number of rows : 22
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 * ups And b Pl 01 36 47.8415443907 +41 24 19.651368029           ~ 272 1
2 * ups And PM* 01 36 47.8415443907 +41 24 19.651368029 4.70 4.64 4.10 3.64 3.35 F9V 963 1
3 * ups And c Pl 01 36 47.8415443907 +41 24 19.651368029           ~ 156 1
4 HD 37124 PM* 05 37 02.4866159419 +20 43 50.832948117   8.35   7.2   G4IV-V 302 2
5 HD 37124c Pl 05 37 02.4866159419 +20 43 50.832948117           ~ 61 1
6 HD 37124b Pl 05 37 02.4866159419 +20 43 50.832948117           ~ 71 1
7 HD 74156 PM* 08 42 25.1219511432 +04 34 41.145751740       7.2   G1V 227 2
8 * rho01 Cnc b Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 259 1
9 * rho01 Cnc EB* 08 52 35.8111044043 +28 19 50.954994470 7.45 6.82   5.4   K0IV-V 1121 1
10 * rho01 Cnc c Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 143 1
11 * rho01 Cnc e Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 576 1
12 * rho01 Cnc d Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 155 1
13 HD 82943 PM* 09 34 50.7353072232 -12 07 46.369202196   7.17 6.53     F9VFe+0.5 470 2
14 PSR B1257+12 Psr 13 00 03.1075 +12 40 55.155           ~ 517 1
15 NAME PSR B1257+12d Pl 13 00 03.1075 +12 40 55.155           ~ 36 2
16 NAME PSR B1257+12c Pl 13 00 03.1075 +12 40 55.155           ~ 37 2
17 HD 168443 PM* 18 20 03.9332862096 -09 35 44.614653900   7.62 6.92     G6V 310 1
18 HD 209458b Pl 22 03 10.7727465312 +18 53 03.549393384           ~ 1859 1
19 HD 209458 V* 22 03 10.7727465312 +18 53 03.549393384   8.21 7.63     F9V 1115 1
20 BD-15 6290c Pl 22 53 16.7325836486 -14 15 49.304052185           ~ 195 1
21 BD-15 6290b Pl 22 53 16.7325836486 -14 15 49.304052185           ~ 253 1
22 BD-15 6290 BY* 22 53 16.7325836486 -14 15 49.304052185 12.928 11.749 10.192 9.013 7.462 M3.5V 1013 1

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