Abstract

ABSTRACTTo date, only 18 exoplanets with radial velocity (RV) semi-amplitude <2 m s−1 have had their masses directly constrained. The biggest obstacle to RV detection of such exoplanets is variability intrinsic to stars themselves, e.g. nuisance signals arising from surface magnetic activity such as rotating spots and plages, which can drown out or even mimic planetary RV signals. We use Kepler-37 – known to host three transiting planets, one of which, Kepler-37d, should be on the cusp of RV detectability with modern spectrographs – as a case study in disentangling planetary and stellar activity signals. We show how two different statistical techniques – one seeking to identify activity signals in stellar spectra, and another to model activity signals in extracted RVs and activity indicators – can each enable a detection of the hitherto elusive Kepler-37d. Moreover, we show that these two approaches can be complementary, and in combination, facilitate a definitive detection and precise characterization of Kepler-37d. Its RV semi-amplitude of 1.22 ± 0.31 m s−1 (mass 5.4 ± 1.4 M⊕) is formally consistent with TOI-178b’s $1.05^{+0.25}_{-0.30}$ m s−1, the latter being the smallest detected RV signal of any transiting planet to date, though dynamical simulations suggest Kepler-37d’s mass may be on the lower end of our 1σ credible interval. Its consequent density is consistent with either a water-world or that of a gaseous envelope ($\sim 0.4{{\ \rm per\ cent}}$ by mass) surrounding a rocky core. Based on RV modelling and a re-analysis of Kepler-37 TTVs, we also suggest that the putative (non-transiting) planet Kepler-37e should be stripped of its ‘confirmed’ status.

Highlights

  • Since the discovery of the first exoplanet over 25 yr ago (Mayor & Queloz 1995), Doppler spectroscopy – known as the radial velocity (RV) method – has been a cornerstone of exoplanetary science

  • Following visual inspection of RVs extracted by the HARPS-N Data Reduction Software (DRS; see Section 4.1), we identified five RVs as possible outliers, viz. from spectra taken on the nights of 2014 April 20, 2014

  • In cases where we modelled stellar activity explicitly, we used the Gaussian process (GP) framework developed by Rajpaul et al (2015), hereafter R15, to model RVs simultaneously with log RHK and bisector span (BIS) observations – the latter two time series being sensitive to activity-induced variability, but not planetary signals

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Summary

INTRODUCTION

Since the discovery of the first exoplanet over 25 yr ago (Mayor & Queloz 1995), Doppler spectroscopy – known as the radial velocity (RV) method – has been a cornerstone of exoplanetary science. At the time of writing, the NASA Exoplanet Archive contained 1321 confirmed exoplanets with RV signals detected and inconsistent with zero at a 3σ level; of these, only 556 have a true mass (rather than minimum mass Mpsin ip) measurement Of the latter 556 planets, only 18 have RV semi-amplitudes

A HARPS-N mass for the elusive Kepler-37d 1849
The star
Three transiting planets
Kepler-37e?
Expected RV detectability
Details of observations
Refined stellar parameters
DRS RV extraction and activity indicators
Pairwise GP extraction
Summary statistic
Comparison of the DRS and PWGP RVs
RV MODELLING
Keplerian signals and RV offsets
Stellar activity
Summary of modelling approaches used in this work
Bayesian model and parameter inference
Likelihood function
Parameter priors
POLYCHORD
Model selection
Non-detection of Kepler-37b and Kepler-37c
Non-detection of new planets
Decisive detection of Kepler-37d
A HARPS-N mass for the elusive Kepler-37d
Non-detection of Kepler-37e
Model residual analysis
Quantitative justification for GP modelling
Computational burdens of our analysis
Parameter inference
Dynamical stability analysis
Kepler-37e: re-examining Kepler-37d’s TTVs
Final characterization of transiting planets
CONCLUSIONS
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