The Planetary Luminosity Problem:" Missing Planets" and The

The Planetary Luminosity Problem:" Missing Planets" and The

Draft version March 27, 2020 Typeset using LATEX twocolumn style in AASTeX62 The Planetary Luminosity Problem: \Missing Planets" and the Observational Consequences of Episodic Accretion Sean D. Brittain,1, ∗ Joan R. Najita,2 Ruobing Dong,3 and Zhaohuan Zhu4 1Clemson University 118 Kinard Laboratory Clemson, SC 29634, USA 2National Optical Astronomical Observatory 950 North Cherry Avenue Tucson, AZ 85719, USA 3Department of Physics & Astronomy University of Victoria Victoria BC V8P 1A1, Canada 4Department of Physics and Astronomy University of Nevada, Las Vegas 4505 S. Maryland Pkwy. Las Vegas, NV 89154, USA (Received March 27, 2020; Revised TBD; Accepted TBD) Submitted to ApJ ABSTRACT The high occurrence rates of spiral arms and large central clearings in protoplanetary disks, if interpreted as signposts of giant planets, indicate that gas giants form commonly as companions to young stars (< few Myr) at orbital separations of 10{300 au. However, attempts to directly image this giant planet population as companions to more mature stars (> 10 Myr) have yielded few successes. This discrepancy could be explained if most giant planets form \cold start," i.e., by radiating away much of their formation energy as they assemble their mass, rendering them faint enough to elude detection at later times. In that case, giant planets should be bright at early times, during their accretion phase, and yet forming planets are detected only rarely through direct imaging techniques. Here we explore the possibility that the low detection rate of accreting planets is the result of episodic accretion through a circumplanetary disk. We also explore the possibility that the companion orbiting the Herbig Ae star HD 142527 may be a giant planet undergoing such an accretion outburst. Keywords: stars: individual (HD 142527) | planets and satellites: formation | protoplanetary disks | planet{disk interactions | planets and satellites: detection 1. INTRODUCTION on the morphologies of protoplanetary disks surround- Giant planets are common at small orbital separa- ing young LMS (i.e., T Tauri stars). Some 10-15% of T tions, as are indirect signatures of their existence at large Tauri disks have the spectral energy distribution (SED) arXiv:2003.11980v1 [astro-ph.SR] 26 Mar 2020 of a transition disk, i.e., a protoplanetary disk in which separations. At orbital separations . 10 au, 10-20% of the central portion ( 10{40 au) is optically thin in the low mass stars (< 1:5 M ; LMS), host a gas giant planet . infrared continuum (Muzerolle et al. 2010a). Transi- (& 1 MJ ; Cassan et al. 2012; Cumming et al. 2008). At tion disk morphologies and other corroborating proper- large separations (& 10 au), a high occurrence rate of gi- ant planetary companions to LMS is also inferred, based ties are interpreted as the signpost of one or more giant planets (& 3 MJ ) orbiting within the optically thin re- gion of the disk (Dodson-Robinson & Salyk 2011; Zhu Corresponding author: Sean D. Brittain et al. 2011; Espaillat et al. 2014a). [email protected] A similar story is found for giant planet companions to ∗ Visiting Scientist, NOAO intermediate mass stars (∼1.5{2 M ; IMS). At small or- 2 Brittain et al. bital separations, radial velocity studies find that ∼14% Stone et al.(2018) found that essentially all nearby FGK of IMS harbor a gas giant planet within ∼10 au of the stars could harbor one or more 7{10 MJ planets at 5{ star (Luhn et al. 2018; Johnson et al. 2010). Transi- 50 au if they formed cold start. The planets are simply tion disk SEDs are also common among young IMS (i.e., too faint to be detected with current surveys. Herbig Ae stars); approximately 40% of Herbig Ae stars While the above discrepancy could point to the va- within 200 pc are transition disk sources Brittain & Na- lidity of cold start models over hot start models, that jita(2019). In addition, a surprisingly large fraction scenario implies that accreting planets would be very of well-studied Herbig Ae disks show dramatic two-arm bright in their youth as they radiate away their accretion spirals (∼20 % Dong et al. 2018a), which point to the energy in accretion shocks and/or through a circumplan- presence of high mass giant planets (5{13 MJ ) at 30{ etary disk. That is, young giant planets (< few Myr) 300 au (Fung & Dong 2015; Dong & Fung 2017). embedded in protoplanetary disks should be readily de- In contrast to the high frequency of indirect indica- tectable during their runaway accretion phase (Eisner tors of giant planets beyond ∼10 au, direct detection of 2015; Zhu 2015). the planets themselves has proven challenging as com- So it is perhaps surprising that giant planets are de- panions to both mature stars as well as young stars sur- tected infrequently as companions to young stars sur- rounded by protoplanetary disks. Many high contrast rounded by protoplanetary disks. While transition disks imaging surveys have searched for giant planet com- have been targeted in many high contrast imaging stud- panions to stars older than 10 Myr at orbital separa- ies (e.g., Subaru SEEDS), planetary companion candi- tions >10 au. As summarized by Bowler(2016, see also dates have been detected in only a few sources. The Nielsen et al. 2019), such studies find that high mass best candidates to date are the companions to two planets (5{13 MJ ) are detected at 30{300 au orbital sep- LMS transition disks|PDS 70 (Keppler et al. 2018) aration in only a small fraction of mature IMS (2.8% and LkCa 15 (Kraus & Ireland 2012; Sallum et al. Bowler 2016), assuming they are as bright as predicted 2015)|and the companions to the IMS transition disk by \hot start" planetary evolutionary models. The low HD 100546 (P´erezet al. 2019; Brittain et al. 2019). As incidence rate is much less than the ∼20% two-arm spi- in the case of the spatially resolved (stellar) compan- ral arm fraction of young IMS that points to planets in ion to the IMS transition disk HD 142527 (Biller et al. the same range of mass and orbital separation (Dong 2012; Close et al. 2014), Hα emission from the PDS 70 et al. 2018a). For mature LMS stars, ∼ 1% have a 1{ and LkCa 15 companions suggests that they are actively 13 MJ giant planet at 10{100 au (Nielsen et al. 2019, accreting. Figure 18), a much lower occurrence rate than the 10{ Here we explore the reason for the infrequent detec- 15% occurrence rate of transition disks among the T tion of accreting giant planets in protoplanetary disks Tauri star population. despite the likelihood that such planets occur commonly The discrepancy between the detection rates of in- and radiate away their accretion energy as they accrete. direct signposts of planet formation and of the plan- We propose that the low \luminosity problem" of form- ets themselves could indicate that the indirect signposts ing planets is solved in a similar fashion to the lumi- are caused by something other than planets. For exam- nosity problem of foming stars (Kenyon et al. 1990; ple, two-armed spirals can also arise from gravitationally Kenyon & Hartmann 1995). Namely, forming plan- unstable disks (Dong et al. 2015a; Kratter & Lodato ets accrete episodically, much like how forming stars 2016). However, the lifetime of the gravitationally un- undergo FU Ori-like outbursts. Previous studies have stable phase is too short to account for the large number argued that circumplanetary disks, like circumstellar of two-armed spirals observed around young stars (Dong disks, are likely to harbor significant dead zones and et al. 2018a; Hall et al. 2018). would accrete episodically (Lubow & Martin 2012), or Alternatively, the discrepantly low detection rate of that vortices form in circumplanetary disks and generate high mass giant planets as companions to mature stars short-timescale outbursts (Zhu et al. 2016). could be entirely due to the use of the hot start mod- To explore this scenario in the context of the devel- els, which assume that planets retain their heat of for- oping detection statistics and properties of young plan- mation (i.e., gravitational potential energy) when they etary companions, we summarize in section 2 the prop- form. The alternative \cold start" models (Marley et al. erties of resolved planetary companions to young proto- 2007; Fortney et al. 2008) assume that planets radiate planetary disk sources. In section 3, we describe a simple away much of their accretion energy in the formation toy model for episodic accretion based on the theoretical phase. As a result, they predict considerably fainter literature and illustrate how episodic accretion can po- planets at ages >10 Myr compared to hot start models. tentially account for the low detection rate of accreting Missing Planets 3 planets. In section 4, we explore the possibility that the is about three orders of magnitude below the accretion companion to HD 142527 is actually a planetary com- luminosity inferred for LkCa 15b (Sallum et al. 2015). panion undergoing an accretion outburst rather than a Table 1 lists the 40 sources from the SEEDS study and low mass stellar companion and discuss ways to discrim- the studies of individual disks that have been observed inate between the two possibilities. We conclude with with angular differential imaging or aperture masking. a discussion of our results and opportunities for future Of these 24 are LMS and 16 are IMS (Column 2). Of progress. the 40 sources, 20 have been classified as transition disks (Column 4). The 4 sources with two-arm spirals|the 2. SEARCHES FOR YOUNG PLANETS other signature of high-mass giant planets|are all tran- sition disk sources. Column 5 provides the cavity size The largest published near infrared imaging survey for of the transition disks.

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