stability of planets in binary star systems · exoplanets in multiple star systems observations:...
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Stability of PlanetsStability of Planetsin Binary Star Systemsin Binary Star SystemsÁkos Bazsó
in collaboration with:E. Pilat-Lohinger, D. Bancelin, B. Funk
ADG Group
Outline
Exoplanets in multiple star systems
Secular perturbation theory
Application: tight binary systems
Summary + Outlook
About
NFN sub-project SP8“Binary Star Systems and Habitability”
Stand-alone project“Exoplanets: Architecture, Evolution and Habitability”
Basic dynamical types
S-type motion (“satellite”)around one star
P-type motion (“planetary”)around both stars
Image: R. Schwarz
Exoplanets in multiple star systems
Observations: (Schwarz 2014, Binary Catalogue)
● 55 binary star systems with 81 planets
● 43 S-type + 12 P-type systems
● 10 multiple star systems with 10 planets
Example: γ Cep (Hatzes et al. 2003)
● RV measurements since 1981
● Indication for a “planet” (Campbell et al. 1988)
● Binary period ~57 yrs, planet period ~2.5 yrs
Multiplicity of stars
~45% of solar like stars (F6 – K3) with d < 25 pc in multiple star systems (Raghavan et al. 2010)
Known exoplanet host stars:
single double triple+ source
77% 20% 3% Raghavan et al. (2006)
83% 15% 2% Mugrauer & Neuhäuser (2009)
88% 10% 2% Roell et al. (2012)
Exoplanet catalogues
The Extrasolar Planets Encyclopaediahttp://exoplanet.eu
Exoplanet Orbit Databasehttp://exoplanets.org
Open Exoplanet Cataloguehttp://www.openexoplanetcatalogue.com
The Planetary Habitability Laboratoryhttp://phl.upr.edu/home
NASA Exoplanet Archivehttp://exoplanetarchive.ipac.caltech.edu
Binary Catalogue of Exoplanetshttp://www.univie.ac.at/adg/schwarz/multiple.html
Habitable Zone Galleryhttp://www.hzgallery.org
Binary Catalogue
Binary Catalogue of Exoplanetshttp://www.univie.ac.at/adg/schwarz/multiple.html
Dynamical stability
Stability limit for S-type planetsRabl & Dvorak (1988), Holman & Wiegert (1999), Pilat-Lohinger & Dvorak (2002)
Parameters (abin
, ebin
, μ)
Outer limit at roughly max. ¼ of stellar separation (for μ = 0.5)
Implications for planet formation → truncation of protoplanetary disk
Secular perturbation theory in a nutshell
Secular perturbation theory
“secular” = long time-scales:
min. 3 interacting massive bodies (m0, m
1, m
2)
gravitational perturbations lead to ...
● mean motion resonances (MMR)
● secular resonances (SR)
resonance = integer ratio of 2 frequencies
T sec≫T rev
f 1/ f 2=p /q∈ℚ
Single star – single planet
two-body problem = indefinitely stable
Basic parameters
● Semi-major axis a● Eccentricity e
0 < e < 1● Solar system planets:
e ≤ 0.2
pericenter apocenter
Binary star system
precession of pericenter (and line of nodes) with time
Laplace-Lagrange linear theory
Developed for solar system (low mass-ratio)
Limits = low eccentricity / inclination
Objects = host star + 2 perturbers + massless test planet
Simple analytical formula (Murray & Dermott 1999)
g = free (proper) secular frequency of test planet
gj = fundamental Eigenfrequencies of system
Free/forced eccentricity
h(t)=efree sin(g t+ϕ)+∑ jA (g , g j ,e j)sin(g j t+ϕ j)
Example 1: frequencies for planets
Example 2: asteroid main-belt
Image: Tsiganis (2008)
Application
Binary star systems with separation a < 100 AU
Typical setting:
● host star (“primary”)
● companion star (“secondary”)
● giant planet (Jupiter like) around primary
● stability of additional (terrestrial) planets ?
Explanation for numerical results
Semi-analytical method
● Determine secular frequency of giant planet
● Find intersection with analytical curve of free frequency
Aim of study
Investigated systemsStar 1 Star 2 Planet
name MassM
sun
SpectralType
MassM
sun
DistanceAU
Ecc. MassM
jup
DistanceAU
Ecc.
GJ 3021 0.90 G6V 0.15 (?) 68 0.20 (?) 3.37 0.49 0.51
Gliese 86 0.83 K0V 0.49 19 0.40 4.01 0.11 0.05
94 Cet 1.34 F8V 0.20 (?) ≥ 100 (?) 0.20 (?) 1.68 1.42 0.30
HD 41004 0.70 K2V 0.15 (?) 23 0.20 (?) 2.54 1.64 0.20 (?)
τ Boo 1.30 F6IV 0.40 (?) 45 0.20 (?) 5.90 0.046 0.02
HD 177830 1.47 K0IV 0.23 97 0.20 (?) 1.49 1.22 ≈ 0.00
HD 196885 1.33 F8V 0.45 21 0.42 2.98 2.60 0.48
γ Cep 1.40 K1III 0.41 19 0.41 1.85 2.05 0.05
(?) = estimated values; minimum masses M sin(i)
Selected systemsStar 1 Star 2 Planet
name MassM
sun
SpectralType
MassM
sun
DistanceAU
Ecc. MassM
jup
DistanceAU
Ecc.
GJ 3021 0.90 G6V 0.15 68 0.20 3.37 0.49 0.51
Gliese 86 0.83 K0V 0.49 19 0.40 4.01 0.11 0.05
94 Cet 1.34 F8V 0.20 ≥ 100 0.20 1.68 1.42 0.30
HD 41004 0.70 K2V 0.15 23 0.20 2.54 1.64 0.20
τ Boo 1.30 F6IV 0.40 45 0.20 5.90 0.046 0.02
HD 177830 1.47 K0IV 0.23 97 0.20 1.49 1.22 ≈ 0.00
HD 196885 1.33 F8V 0.45 21 0.42 2.98 2.60 0.48
γ Cep 1.40 K1III 0.41 19 0.41 1.85 2.05 0.05
Numerical results for HD 41004
Image: E. Pilat-Lohinger
Why not the other systems ?
HD 1237
HD 41004
Dependence on secondary star 1
increasing a2
Dependence on secondary star 2
increasing m2
HD 196885
Outlook
Ongoing work
Determine width of perturbation – dependence on parameters (mass, distance, eccentricity, …)
Goals:
● Catalogue for observers
● Binary star systems allowing “unperturbed” habitable zone (small eccentricity)
That's all folks ...That's all folks ...
References
Campbell, Walker & Yang (1988), ApJ 331, 902
Hatzes, Cochran, Endl et al. (2003), ApJ 599, 1383
Holman & Wiegert (1999), AJ 117, 621
Mugrauer & Neuhäuser (2009), A&A 494, 373
Murray & Dermott (1999), Solar System Dynamics, Cambridge Univ. Press
Pilat-Lohinger & Dvorak (2002), CMDA 82, 143
Rabl & Dvorak (1988), A&A 191, 385
Raghavan, Henry, Mason et al. (2006), ApJ 646, 523
Raghavan, McAlister, Henry et al. (2010), ApJS 190, 1
Roell, Neuhäuser, Seifahrt & Mugrauer (2012), A&A 542, 92
Tsiganis (2008), Lecture Notes in Physics 729, 111, Springer