Abstract:We report on the determination of the mass of TOI-519 b, a transiting substellar object around a mid-M dwarf. We carried out radial velocity measurements using Subaru/InfraRed Doppler (IRD), revealing that TOI-519 b is a planet with a mass of $0.463^{+0.082}_{-0.088}\, M_{\rm Jup}$. We also found that the host star is metal rich ([Fe/H] = 0.27 ± 0.09 dex) and has the lowest effective temperature (Teff = 3322 ± 49 K) among all stars hosting known close-in giant planets based on the IRD spectra and mid-resolutio… Show more
“…A strong correlation between host star metallicity and short-period giant planet occurrence has previously been established for FGK host stars (Fischer & Valenti 2005). The emerging set of giant-planet-hosting M dwarfs appears to show this trend as well (e.g., Hirano et al 2018;Gan et al 2022;Kagetani et al 2023). The newly discovered systems bolster this conclusion.…”
Section: Discussionmentioning
confidence: 64%
“…Parviainen et al (2021) announced the discovery of TOI 519 b, and Kagetani et al (2023) published a mass measurement for the planet based on Subaru/IRD RV measurements. Transits of this system were first detected in the Sector 7 observations from TESS.…”
Section: Toi 519mentioning
confidence: 99%
“…The data are included in Table 5 and plotted in Figure 1. Kagetani et al (2023) published 18 RVs of TOI 519 derived from mid-IR spectra obtained with Subaru/IRD (Tamura et al 2012;Kotani et al 2018). We incorporated these RV measurements into our joint analysis of this system.…”
We present the discovery from the TESS mission of two giant planets transiting M-dwarf stars: TOI 4201 b and TOI 5344 b. We also provide precise radial velocity measurements and updated system parameters for three other M dwarfs with transiting giant planets: TOI 519, TOI 3629, and TOI 3714. We measure planetary masses of 0.525 ± 0.064 M
J, 0.243 ± 0.020 M
J, 0.689 ± 0.030 M
J, 2.57 ± 0.15 M
J, and 0.412±0.040 M
J for TOI 519 b, TOI 3629 b, TOI 3714 b, TOI 4201 b, and TOI 5344 b, respectively. The corresponding stellar masses are 0.372 ± 0.018 M
☉, 0.635 ± 0.032 M
☉, 0.522 ± 0.028 M
☉, 0.626 ± 0.033 M
☉, and 0.612 ± 0.034 M
☉. All five hosts have supersolar metallicities, providing further support for recent findings that, like for solar-type stars, close-in giant planets are preferentially found around metal-rich M-dwarf host stars. Finally, we describe a procedure for accounting for systematic errors in stellar evolution models when those models are included directly in fitting a transiting planet system.
“…A strong correlation between host star metallicity and short-period giant planet occurrence has previously been established for FGK host stars (Fischer & Valenti 2005). The emerging set of giant-planet-hosting M dwarfs appears to show this trend as well (e.g., Hirano et al 2018;Gan et al 2022;Kagetani et al 2023). The newly discovered systems bolster this conclusion.…”
Section: Discussionmentioning
confidence: 64%
“…Parviainen et al (2021) announced the discovery of TOI 519 b, and Kagetani et al (2023) published a mass measurement for the planet based on Subaru/IRD RV measurements. Transits of this system were first detected in the Sector 7 observations from TESS.…”
Section: Toi 519mentioning
confidence: 99%
“…The data are included in Table 5 and plotted in Figure 1. Kagetani et al (2023) published 18 RVs of TOI 519 derived from mid-IR spectra obtained with Subaru/IRD (Tamura et al 2012;Kotani et al 2018). We incorporated these RV measurements into our joint analysis of this system.…”
We present the discovery from the TESS mission of two giant planets transiting M-dwarf stars: TOI 4201 b and TOI 5344 b. We also provide precise radial velocity measurements and updated system parameters for three other M dwarfs with transiting giant planets: TOI 519, TOI 3629, and TOI 3714. We measure planetary masses of 0.525 ± 0.064 M
J, 0.243 ± 0.020 M
J, 0.689 ± 0.030 M
J, 2.57 ± 0.15 M
J, and 0.412±0.040 M
J for TOI 519 b, TOI 3629 b, TOI 3714 b, TOI 4201 b, and TOI 5344 b, respectively. The corresponding stellar masses are 0.372 ± 0.018 M
☉, 0.635 ± 0.032 M
☉, 0.522 ± 0.028 M
☉, 0.626 ± 0.033 M
☉, and 0.612 ± 0.034 M
☉. All five hosts have supersolar metallicities, providing further support for recent findings that, like for solar-type stars, close-in giant planets are preferentially found around metal-rich M-dwarf host stars. Finally, we describe a procedure for accounting for systematic errors in stellar evolution models when those models are included directly in fitting a transiting planet system.
“…Recent discoveries of GEMS have extended beyond early M-dwarfs to mid and late M-dwarfs (Figure 8; Morales et al 2019;Feng et al 2020;Hobson et al 2023;Kagetani et al 2023;Kanodia et al 2023), making it harder to reconcile the observations with the predictions from the core-accretion mechanism (e.g., Burn et al 2021). Utilizing planet candidates from the TESS mission, Gan et al (2023) estimated the occurrence rate of transiting hot Jupiters to be 0.27% for stars with masses from 0.45 to 0.65 M e .…”
Section: M-dwarf Gas Giant Demographicsmentioning
confidence: 99%
“…In comparison to the constrained Kepler fields of view, the Transiting Exoplanet Survey Satellite (TESS) mission targets stars distributed across the entire sky, and hence can detect the transiting exoplanets orbiting relatively bright nearby M-dwarfs (Muirhead et al 2018). This has been helpful to detect and confirm a number of GEMS (Johnson et al 2012;Canas et al 2020Canas et al , 2022Canas et al , 2023Jordan et al 2022;Kanodia et al 2022Kanodia et al , 2023Hobson et al 2023;Kagetani et al 2023;Lin et al 2023). These detections from Doppler and the transiting survey are a challenge to explain for core-accretion (Morales et al 2019;Schlecker et al 2022;Kanodia et al 2023).…”
Recent discoveries of gas giant exoplanets around M-dwarfs from transiting and radial velocity surveys are difficult to explain with core-accretion models. We present here a homogeneous suite of 162 models of gravitationally unstable gaseous disks. These models represent an existence proof for gas giants more massive than 0.1 Jupiter masses to form by the gas disk gravitational instability (GDGI) mechanism around M-dwarfs for comparison with observed exoplanet demographics and protoplanetary disk mass estimates for M-dwarf stars. We use the Enzo 2.6 adaptive mesh refinement (AMR) 3D hydrodynamics code to follow the formation and initial orbital evolution of gas giant protoplanets in gravitationally unstable gaseous disks in orbit around M-dwarfs with stellar masses ranging from 0.1 M
⊙ to 0.5 M
⊙. The gas disk masses are varied over a range from disks that are too low in mass to form gas giants rapidly to those where numerous gas giants are formed, therefore revealing the critical disk mass necessary for gas giants to form by the GDGI mechanism around M-dwarfs. The disk masses vary from 0.01 M
⊙ to 0.05 M
⊙ while the disk to star mass ratios explored the range from 0.04 to 0.3. The models have varied initial outer disk temperatures (10–60 K) and varied levels of AMR grid spatial resolution, producing a sample of expected gas giant protoplanets for each star mass. Broadly speaking, disk masses of at least 0.02 M
⊙ are needed for the GDGI mechanism to form gas giant protoplanets around M-dwarfs.
We report the discovery and characterisation of a giant transiting planet orbiting a nearby M3.5V dwarf (d = 80.4\,pc, $G$ = 15.1\,mag, $K$=11.2\,mag, $R_ $M_ Using the photometric time series from TESS sectors 10, 36, 46, and 63 and near-infrared spectrophotometry from ExTrA, we measured a planetary radius of $0.77 and an orbital period of 1.52 days. With high-resolution spectroscopy taken by the CFHT/SPIRou and ESO/ESPRESSO spectrographs, we refined the host star parameters ($ Fe/H and measured the mass of the planet ($0.273 Based on these measurements, TOI-4860\,b joins the small set of massive planets ($>80$ found around mid to late M dwarfs ($<0.4$ providing both an interesting challenge to planet formation theory and a favourable target for further atmospheric studies with transmission spectroscopy. We identified an additional signal in the radial velocity data that we attribute to an eccentric planet candidate ($e=0.66 with an orbital period of $427 days and a minimum mass of $1.66 but additional data would be needed to confirm this.
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