J/AJ/162/55      65 Transit-timing variation planets properties     (Yee+, 2021)
How close are compact multiplanet systems to the stability limit?
    Yee S.W., Tamayo D., Hadden S., Winn J.N.
   <Astron. J., 162, 55-55 (2021)>
   =2021AJ....162...55Y 2021AJ....162...55Y    (SIMBAD/NED BibCode)
ADC_Keywords: Exoplanets; Stars, variable; Stars, masses
Keywords: Exoplanet dynamics; Exoplanet formation; Exoplanet astronomy
          Celestial mechanics
Abstract:
    Transit surveys have revealed a significant population of compact
    multiplanet systems, containing several sub-Neptune-mass planets on
    close-in, tightly-packed orbits. These systems are thought to have
    formed through a final phase of giant impacts, which would tend to
    leave systems close to the edge of stability. Here, we assess this
    hypothesis, comparing observed eccentricities in systems exhibiting
    transit-timing variations versus the maximum eccentricities compatible
    with long-term stability. We use the machine-learning classifier SPOCK
    (Tamayo et al.) to rapidly classify the stability of numerous initial
    configurations and hence determine these stability limits. While
    previous studies have argued that multiplanet systems are often
    maximally packed, in the sense that they could not host any additional
    planets, we find that the existing planets in these systems have
    measured eccentricities below the limits allowed by stability by a
    factor of 2-10. We compare these results against predictions from the
    giant-impact theory of planet formation, derived from both N-body
    integrations and theoretical expectations that, in the absence of
    dissipation, the orbits of such planets should be distributed
    uniformly throughout the phase space volume allowed by stability. We
    find that the observed systems have systematically lower
    eccentricities than this scenario predicts, with a median eccentricity
    about four times lower than predicted. This suggests that, if these
    systems formed through giant impacts, then some dissipation must occur
    to damp their eccentricities. This may occur through interactions with
    the natal gas disk or a leftover population of planetesimals, or over
    longer timescales through the coupling of tidal and secular processes.
Description:
    In this paper, we focus our investigation on Transit-timing variation
    (TTV) systems containing three or more planets with good mass and
    eccentricity constraints. We draw the systems for our study from the
    analysis of Hadden & Lithwick, 2017,J/AJ/154/5, who derived masses and
    eccentricities for 55 planetary systems based on the Kepler TTV
    catalog of Rowe+, 2015, J/ApJS/217/16.
File Summary:
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 FileName    Lrecl    Records   Explanations
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ReadMe          80          .   This file
table1.dat     103         65  *Transit-timing variation (TTV) planet properties
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Note on table1.dat : The values and uncertainties reflect the mode of
    the posterior probabilities and 68.3% highest posterior density
    intervals around the mode, or 68.3% upper limits if this interval is
    consistent with zero.
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See also:
 J/ApJS/217/16 : Kepler planetary candidates. V. 3yr Q1-Q12 (Rowe+, 2015)
 J/MNRAS/448/1044 : Simul. data for 50 planetary model systems (Hansen+, 2015)
 J/ApJ/821/47  : KOI transit proba. of multi-planet syst. (Brakensiek+, 2016)
 J/A+A/605/A72 : Planetary systems AMD-stability (Laskar+, 2017)
 J/AJ/154/5    : Transit timing variations of 145 Kepler planets (Hadden+, 2017)
 J/AJ/156/18   : APOGEE DR14:Binary comp. of evolved stars (Price-Whelan+, 2018)
 J/AJ/159/281  : Characteristics of 335 KOI stars (Gilbert+, 2020)
Byte-by-byte Description of file: table1.dat
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   Bytes Format Units  Label  Explanations
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   1- 12 A12    ---    ID     Planet identifier
  14- 20 F7.3   d      Per    [3.6/131] Orbital period
  22- 24 F3.1   Msun   Mass*  [0.5/1.2] Stellar mass
  26- 29 F4.2   Msun E_Mass*  [0.03/0.1] Upper uncertainty in M*
  31- 34 F4.2   Msun e_Mass*  [0.03/0.1] Lower uncertainty in M*
      36 I1     ---  f_Massp  [0/1]Limit flag on Mp (1)
  38- 42 F5.2   Mgeo   Massp  [0.01/35.2] Planetary mass
  44- 47 F4.2   Mgeo E_Massp  [0.01/6.7]? Upper uncertainty in Mp
  49- 52 F4.2   Mgeo e_Massp  [0.01/3.8]? Lower uncertainty in Mp
  54- 58 F5.3   ---    Z      [0.001/0.16]? Free eccentricity (2)
  60- 64 F5.3   ---  E_Z      [0/0.1]? Upper uncertainty in Z
  66- 70 F5.3   ---  e_Z      [0/0.1]? Lower uncertainty in Z
  72- 76 F5.3   ---    Zcom   [0.002/0.13]? Center-of-mass eccentricity (3)
  78- 82 F5.3   ---  E_Zcom   [0.004/0.08]? Upper uncertainty in Zcom
  84- 88 F5.3   ---  e_Zcom   [0.002/0.05]? Lower uncertainty in Zcom
  90- 93 F4.2   ---    Z/Zuns [0.09/09]? Fractional distance to instability of
                               system
  95- 98 F4.2   ---  E_Z/Zuns [0.06/0.3]? Upper uncertainty in Z/Zuns
 100-103 F4.2   ---  e_Z/Zuns [0/0.2]? Lower uncertainty in Z/Zuns
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Note (1): Flags as follows:
    0 = not a limit;
    1 = lower limit.
Note (2): Derived by Hadden & Lithwick+, 2017, J/AJ/154/5. Because
          the free eccentricity Z is a property of adjacent pairs of planets,
          we have recorded Z in the row of the inner planet of the pair.
Note (3): Computed according to Eq. 3, and recorded in the row of
          the innermost planet.
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History:
    From electronic version of the journal
(End)                          Prepared by [AAS], Coralie Fix [CDS], 16-Nov-2021