Nothing says weird like a disintegrating exoplanet. There are supposed to be 3-4 of them, and here are some 2018 updates.
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http://iopscience.iop.org/article/10...72/aaba12/meta
Radial Velocity Follow-up of the Disintegrating Planet KIC 12557548b
Kento Masuda, Teruyuki Hirano, Hajime Kawahara, and Bun'ei Sato
2018 March 30
KIC 12557548b is an ultra-short-period (0.65 days) planet observed with the Kepler spacecraft, whose transit light curves exhibit depth variations and asymmetric morphology (Rappaport et al. 2012). These features are ascribed to disintegration of the rocky planet, but it may also be worth considering less extraordinary explanations. For example, a giant planet or stellar companion on an eccentric and grazing orbit, perturbed by a third body, could produce transit depth variations via varying orbital inclinations, and asymmetric "transits" via tidal distortion of the star as observed in heartbeat binaries. Such an alternative can be tested by measuring radial velocities (RVs) over the whole orbital phase.
We obtained high-resolution (R ~ 60,000) spectra of KIC 12557548 with the High Dispersion Spectrograph (HDS, Noguchi et al. 2002) installed on the Subaru 8.2 m telescope (proposal S15B-163). The observations were performed on UT 2015 August 27 and 28 to obtain five 40 minute exposures each night, with the standard Ra setup covering 5107–7787 Å. The signal to noise per pixel was 20–30 around 5800 Å.
We performed standard reduction and wavelength calibration using Th–Ar spectra obtained before and after each exposure. Only the data from red CCDs were analyzed to apply telluric corrections (see below). We normalized the spectra and removed OH night-sky emissions using the list in Osterbrock et al. (1996), as well as cosmic-ray outliers. The spectra were then interpolated and cross-correlated with the theoretical spectrum (Coelho et al. 2005) for atmospheric parameters similar to KIC 12557548 to derive RV shifts. The RV value and its error for each exposure were obtained as the mean and its standard error calculated from the shifts in nine orders without heavy telluric contaminations or bad-quality data, and the barycentric correction was applied.
These RVs were further calibrated using telluric lines following Chubak et al. (2012). We used the SKYCALC Sky Model Calculator 7 to produce a model telluric spectrum with R = 300,000, and used it to measure velocity shifts in two wavelength ranges (7594–7621 Å and 6867–6884 Å) containing oxygen A and B bands. The average of the two was used to calibrate RV zero points.
The resulting RVs (Figure 1) were constant within ~100 m s−1 and consistent with Keck/HIRES values from Croll et al. (2014), thus providing further evidence for the disintegrating planet scenario. We used emcee (Foreman-Mackey et al. 2013) to fit the combined RV time series assuming the circular Keplerian orbit. The ephemerides were fixed at the values in the KOI catalog and uniform priors were imposed on the RV semi-amplitude K and systemic RV. We found K < 86 m s−1 as the 95th percentile of the marginal posterior. Adopting the host star mass of 0.67 M ⊙, this translates into the upper limit on the planetary mass m < 89 M ⊕.
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https://arxiv.org/abs/1807.07973
Chromatic transit light curves of disintegrating rocky planets
A. R. Ridden-Harper, C. U. Keller, M. Min, R. van Lieshout, I. A. G. Snellen
(Submitted on 20 Jul 2018)
Context. Kepler observations have revealed a class of short period exoplanets, of which Kepler-1520 b is the prototype, which have comet-like dust tails thought to be the result of small, rocky planets losing mass. The shape and chromaticity of the transits constrain the properties of the dust particles originating from the planet's surface, offering a unique opportunity to probe the composition and geophysics of rocky exoplanets.
Aims. We aim to approximate the average Kepler long-cadence light curve of Kepler-1520 b and investigate how the optical thickness and transit cross-section of a general dust tail can affect the observed wavelength dependence and depth of transit light curves.
Methods. We developed a new 3D model that ejects sublimating particles from the planet surface to build up a dust tail, assuming it to be optically thin, and used 3D radiative transfer computations that fully treat scattering using the distribution of hollow spheres (DHS) method, to generate transit light curves between 0.45 and 2.5 μ m.
Results. We show that the transit depth is wavelength independent for optically thick tails, potentially explaining why only some observations indicate a wavelength dependence. From the 3D nature of our simulated tails, we show that their transit cross-sections are related to the component of particle ejection velocity perpendicular to the planet's orbital plane and use this to derive a minimum ejection velocity of 1.2 kms −1. To fit the average transit depth of Kepler-1520 b of 0.87%, we require a high dust mas-loss rate of 7−80 M⊕ Gyr −1 which implies planet lifetimes that may be inconsistent with the observed sample. Therefore, these mass-loss rates should be considered to be upper limits.
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http://adsabs.harvard.edu/abs/2018AAS...23211102C
The Ongoing Evolution of the K2-22 System
Colon, Knicole D.; Zhou, George; Shporer, Avi; Collins, Karen A.; Bieryla, Allyson; Latham, David W.; Espinoza, Nestor; Murgas, Felipe; Pattarakijwanich, Petchara; Awiphan, Supachai; TECH Collaboration
06/2018
Of the thousands of exoplanets known, only three disintegrating planets have been identified. These disintegrating planets appear to have tails of dusty material that produce asymmetric transit shapes. K2-22b is one of these few disintegrating planets discovered to date, and its light curve not only displays highly variable transit depths but also uniquely displays evidence of a leading dust tail. Here, we present results from a large ground-based photometric observing campaign of the K2-22 system that took place between December 2016 and May 2017, which we use to investigate the evolution of the transit of K2-22b. Last observed in early 2015, in these new observations we recover the transit around the expected time and measure a typical depth of <1%. We find that the transit depth has decreased compared to observations from 2014 and 2015, where the maximum transit depth measured at that time was ~1.3%. These new observations support ongoing variability in the transit depth, shape, and time of K2-22b, although the overall shallowness of the transit makes a detailed analysis of the transit shape and timing difficult. In addition, we find no strong evidence of wavelength-dependent transit depths for epochs where we have simultaneous coverage at multiple wavelengths. Given the observed decrease in the transit depth between 2015 and 2017, we encourage continued high-precision photometric monitoring of this system in order to further constrain the evolution timescale and to aid comparative studies with the other few disintegrating planets known.
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https://arxiv.org/pdf/1804.01997.pdf
Transiting Disintegrating Planetary Debris around WD 1145+017
Andrew Vanderburg and Saul A. Rappaport
4/2018
More than a decade after astronomers realized that disrupted planetary material likely pollutes the surfaces of many white dwarf stars, the discovery of transiting debris orbiting the white dwarf WD 1145+017 has opened the door to new explorations of this process. We describe the observational evidence for transiting planetary material and the current theoretical understanding (and in some cases lack thereof) of the phenomenon.
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https://arxiv.org/abs/1712.07461
Light-curve analysis of KOI 2700b: the second extrasolar planet with a comet-like tail
Z. Garai
(Submitted on 20 Dec 2017)
The Kepler object KOI 2700b (KIC 8639908b) was discovered recently as the second exoplanet with a comet-like tail. It exhibits a distinctly asymmetric transit profile, likely indicative of the emission of dusty effluents and reminiscent of KIC 12557548b, the first exoplanet with a comet-like tail. The scientific goal of this work is to verify the disintegrating-planet scenario of KOI 2700b by modeling its light curve and to put constraints on various tail and planet properties, as was done in the case of KIC 12557548b. We obtained the phase-folded and binned transit light curve of KOI 2700b, which we subsequently iteratively modeled using the radiative-transfer code SHELLSPEC. We modeled the comet-like tail as part of a ring around the parent star and we also included the solid body of the planet in the model. During the modeling we applied selected species and dust particle sizes. We confirmed the disintegrating-planet scenario of KOI 2700b. Furthermore, via modeling, we derived some interesting features of KOI 2700b and its comet-like tail.