2014AJ....147...32G


Query : 2014AJ....147...32G

2014AJ....147...32G - Astron. J., 147, 32 (2014/February-0)

Overstable librations can account for the paucity of mean motion resonances among exoplanet pairs.

GOLDREICH P. and SCHLICHTING H.E.

Abstract (from CDS):

We assess the multi-planet systems discovered by the Kepler satellite in terms of current ideas about orbital migration and eccentricity damping due to planet-disk interactions. Our primary focus is on first order mean motion resonances, which we investigate analytically to lowest order in eccentricity. Only a few percent of planet pairs are in close proximity to a resonance. However, predicted migration rates (parameterized by τn = n/|{dot}n|) imply that during convergent migration most planets would have been captured into first order resonances. Eccentricity damping (parameterized by τe = e/|{dot}e|) offers a plausible resolution. Estimates suggest τe/τn∼ (h/a)2 ∼ 10–2, where h/a is the ratio of disk thickness to radius. Together, eccentricity damping and orbital migration give rise to an equilibrium eccentricity, eeq∼ (τe/τn)1/2. Capture is permanent provided eeq ≲ µ1/3, where µ denotes the planet to star mass ratio. But for eeq ≳ µ1/3, capture is only temporary because librations around equilibrium are overstable and lead to passage through resonance on timescale τe. Most Kepler planet pairs have eeq> µ1/3. Since τn{Gt} τe is the timescale for migration between neighboring resonances, only a modest percentage of pairs end up trapped in resonances after the disk disappears. Thus the paucity of resonances among Kepler pairs should not be taken as evidence for in situ planet formation or the disruptive effects of disk turbulence. Planet pairs close to a mean motion resonance typically exhibit period ratios 1%-2% larger than those for exact resonance. The direction of this shift undoubtedly reflects the same asymmetry that requires convergent migration for resonance capture. Permanent resonance capture at these separations from exact resonance would demand µ(τn/τe)1/2 ≳ 0.01, a value that estimates of µ from transit data and (τe/τn)1/2 from theory are insufficient to match. Plausible alternatives involve eccentricity damping during or after disk dispersal. The overstability referred to above has applications beyond those considered in this investigation. It was discovered numerically by Meyer & Wisdom in their study of the tidal evolution of Saturn's satellites.

Abstract Copyright: ∼

Journal keyword(s): celestial mechanics - methods: analytical - methods: numerical - planet-disk interactions - planets and satellites: dynamical evolution and stability - planets and satellites: formation

Simbad objects: 1

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Number of rows : 1
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 BD-15 6290 BY* 22 53 16.7325836486 -14 15 49.304052185 12.928 11.749 10.192 9.013 7.462 M3.5V 1106 1

Query : 2014AJ....147...32G

Basic data :
BD-15 6290 -- BY Dra Variable
Other object types:
otypes_help
* (2015ApJS,BD,...), PM* (2013MNRAS,Ci,...), BY* (2017ARep), Ro* (2012A&A), V* (V*), NIR (2MASS), MIR (WISEA)
ICRS coord. (ep=J2000) :
22 53 16.7325836486 -14 15 49.304052185 (Optical) [ 0.0338 0.0258 90 ] A 2020yCat.1350....0G
FK4 coord. (ep=B1950 eq=1950) :
22 50 34.6499284991 -14 31 14.052098435 [ 0.0338 0.0258 90 ]
Gal coord. (ep=J2000) :
052.0040597500243 -59.6300891766021 [ 0.0338 0.0258 90 ]
Proper motions mas/yr :
957.715 -673.601 [0.041 0.031 90] A 2020yCat.1350....0G
Radial velocity / Redshift / cz :
V(km/s) -1.47 [0.0003] / z(spectroscopic) -0.000005 [0.000000] / cz -1.47 [0.00]
   (Opt) A 2018MNRAS.475.1960F
Parallaxes (mas):
214.0380 [0.0356] A 2020yCat.1350....0G
Spectral type:
M3.5V C 1983SAAOC...7..106W
Fluxes (12) :
U 12.928 [0.0034] B 2009AJ....137.4186L
B 11.749 [0.0017] B 2009AJ....137.4186L
V 10.192 [0.0017] B 2009AJ....137.4186L
R 9.013 [0.0017] B 2009AJ....137.4186L
G 8.875059 [0.002861] C 2020yCat.1350....0G
I 7.462 [0.0017] B 2009AJ....137.4186L
J 5.934 [0.019] C 2003yCat.2246....0C
H 5.349 [0.049] C 2003yCat.2246....0C
K 5.010 [0.021] C 2003yCat.2246....0C
g 10.919 [~] D 2012yCat.1322....0Z
r 9.872 [0.08] D 2012yCat.1322....0Z
i 8.296 [0.05] D 2012yCat.1322....0Z
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Hierarchy : number of linked objects
whatever the membership probability is (see description here ) :

: 1
: 4
: 235 Display criteria :

Identifiers (43) :
An access of full data is available using the icon Vizier near the identifier of the catalogue

BD-15 6290 GSC 05819-00957 NAME NC 59 UBV M 5470
Ci 20 1387 HIC 113020 NLTT 55130 UCAC2 26801725
CNS5 5644 HIP 113020 8pc 212.69A UCAC4 379-165686
EPIC 206019387 JP11 295 PLX 5546 V* IL Aqr
EPIC 206019392 Karmn J22532-142 PLX 5546.00 WEB 20121
GCRV 14365 LFT 1745 PM J22532-1415 WISEA J225317.42-141556.1
GEN# -0.01506290 LHS 530 Ross 780 Zkh 338
G 156-57A LPM 841 TIC 188580272 [RHG95] 3604
G 156-57 LTT 9244 TYC 5819-1255-1 Gaia DR3 2603090003484152064
GJ 876 2MASS J22531672-1415489 UBV 19209 Gaia DR2 2603090003484152064
GJ 876 A MCC 337 UBV 19610

References (1106 between 1850 and 2026) (Total 1106)
Simbad bibliographic survey began in 1850 for stars (at least bright stars) and in 1983 for all other objects (outside the solar system).
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Collections of Measurements Description of Measurements

Velocities : 11    Distance : 3    Var : 4    Rot : 5    Fe/H : 44    Plx : 6    PM : 10    SpT : 20   

   

Observing logs
Herschel : 3    ISO : 4   

   


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Link by name to the catalogue in VizieR :

BD-15 6290 G 156-57A G 156-57 GJ 876 GJ 876 A
GSC 05819-00957 HIC 113020 HIP 113020 LHS 530 2MASS J22531672-1415489
NLTT 55130 PLX 5546 TYC 5819-1255-1 UCAC2 26801725 UCAC4 379-165686
V* IL Aqr WISEA J225317.42-141556.1 Gaia DR3 2603090003484152064 Gaia DR2 2603090003484152064

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