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Featured researches published by John Asher Johnson.


The Astrophysical Journal | 2010

HAT-P-11b: A super-neptune planet transiting a bright K star in the kepler field

G. Á. Bakos; Guillermo Torres; A. Pál; J. D. Hartman; G. Kovács; Robert W. Noyes; D. W. Latham; Dimitar D. Sasselov; B. Sipőcz; Gilbert A. Esquerdo; Debra A. Fischer; John Asher Johnson; G. W. Marcy; R. P. Butler; Howard Isaacson; Andrew W. Howard; S. S. Vogt; Gábor Kovács; J. M. Fernandez; A. Moór; Robert P. Stefanik; J. Lázár; I. Papp; P. Sári

We report on the discovery of HAT-P-11b, the smallest radius transiting extrasolar planet (TEP) discovered from the ground, and the first hot Neptune discovered to date by transit searches. HAT-P-11b orbits the bright (V = 9.587) and metal rich ([Fe/H] = +0.31 ± 0.05) K4 dwarf star GSC 03561-02092 with P = 4.8878162 ± 0.0000071 days and produces a transit signal with depth of 4.2 mmag, the shallowest found by transit searches that is due to a confirmed planet. We present a global analysis of the available photometric and radial velocity (RV) data that result in stellar and planetary parameters, with simultaneous treatment of systematic variations. The planet, like its near-twin GJ 436b, is somewhat larger than Neptune (17 M_⊕, 3.8 R_⊕) both in mass M_p = 0.081 ± 0.009 M_J(25.8 ± 2.9 M_⊕) and radius R_p = 0.422 ± 0.014 R_J(4.73 ± 0.16 R_⊕). HAT-P-11b orbits in an eccentric orbit with e = 0.198 ± 0.046 and ω = 355o.2 ± 17o.3, causing a reflex motion of its parent star with amplitude 11.6 ± 1.2 ms^(–1), a challenging detection due to the high level of chromospheric activity of the parent star. Our ephemeris for the transit events is T_c = 2454605.89132 ± 0.00032 (BJD), with duration 0.0957 ± 0.0012 days, and secondary eclipse epoch of 2454608.96 ± 0.15 days (BJD). The basic stellar parameters of the host star are M_★ = 0.809^(+0.020)_(–0.027) M_☉, R_★ = 0.752 ± 0.021 R_☉, and T_(eff★) = 4780 ± 50 K. Importantly, HAT-P-11 will lie on one of the detectors of the forthcoming Kepler mission; this should make possible fruitful investigations of the detailed physical characteristic of both the planet and its parent star at unprecedented precision. We discuss an interesting constraint on the eccentricity of the system by the transit light curve and stellar parameters. This will be particularly useful for eccentric TEPs with low-amplitude RV variations in Keplers field. We also present a blend analysis, that for the first time treats the case of a blended transiting hot Jupiter mimicking a transiting hot Neptune, and proves that HAT-P-11b is not such a blend.


Proceedings of SPIE | 2014

Transiting Exoplanet Survey Satellite (TESS)

George R. Ricker; Joshua N. Winn; R. Vanderspek; David W. Latham; G. Á. Bakos; Jacob L. Bean; Zachory K. Berta-Thompson; Timothy M. Brown; Lars A. Buchhave; Nathaniel R. Butler; R. Paul Butler; W. J. Chaplin; David Charbonneau; Jørgen Christensen-Dalsgaard; Mark Clampin; Drake Deming; John P. Doty; Nathan De Lee; Courtney D. Dressing; Edward W. Dunham; Michael Endl; Francois Fressin; Jian Ge; Thomas Henning; Matthew J. Holman; Andrew W. Howard; Shigeru Ida; Jon M. Jenkins; Garrett Jernigan; John Asher Johnson

The Transiting Exoplanet Survey Satellite (TESS ) will search for planets transiting bright and nearby stars. TESS has been selected by NASA for launch in 2017 as an Astrophysics Explorer mission. The spacecraft will be placed into a highly elliptical 13.7-day orbit around the Earth. During its two-year mission, TESS will employ four wide-field optical CCD cameras to monitor at least 200,000 main-sequence dwarf stars with IC (approximately less than) 13 for temporary drops in brightness caused by planetary transits. Each star will be observed for an interval ranging from one month to one year, depending mainly on the stars ecliptic latitude. The longest observing intervals will be for stars near the ecliptic poles, which are the optimal locations for follow-up observations with the James Webb Space Telescope. Brightness measurements of preselected target stars will be recorded every 2 min, and full frame images will be recorded every 30 min. TESS stars will be 10-100 times brighter than those surveyed by the pioneering Kepler mission. This will make TESS planets easier to characterize with follow-up observations. TESS is expected to find more than a thousand planets smaller than Neptune, including dozens that are comparable in size to the Earth. Public data releases will occur every four months, inviting immediate community-wide efforts to study the new planets. The TESS legacy will be a catalog of the nearest and brightest stars hosting transiting planets, which will endure as highly favorable targets for detailed investigations.


The Astrophysical Journal | 2009

TEN NEW AND UPDATED MULTIPLANET SYSTEMS AND A SURVEY OF EXOPLANETARY SYSTEMS

Jason T. Wright; S. Upadhyay; G. W. Marcy; Debra A. Fischer; Eric B. Ford; John Asher Johnson

We present the latest velocities for ten multiplanet systems, including a re-analysis of archival Keck and Lick data, resulting in improved velocities that supersede our previously published measurements. We derive updated orbital fits for 10 Lick and Keck systems, including two systems (HD 11964, HD 183263) for which we provide confirmation of second planets only tentatively identified elsewhere, and two others (HD 187123 and HD 217107) for which we provide a major revision of the outer planets orbit. We compile orbital elements from the literature to generate a catalog of the 28 published multiple-planet systems around stars within 200 pc. From this catalog we find several intriguing patterns emerging: (1) including those systems with long-term radial velocity trends, at least 28% of known planetary systems appear to contain multiple planets; (2) planets in multiple-planet systems have somewhat smaller eccentricities than single planets; and (3) the distribution of orbital distances of planets in multiplanet systems and single planets are inconsistent: single-planet systems show a pileup at P ~ 3 days and a jump near 1 AU, while multiplanet systems show a more uniform distribution in log-period. In addition, among all planetary systems we find the following. (1) There may be an emerging, positive correlation between stellar mass and giant-planet semimajor axis. (2) Exoplanets with M sin i > 1 M_(Jup) more massive than Jupiter have eccentricities broadly distributed across 0 < e < 0.5, while lower mass exoplanets exhibit a distribution peaked near e = 0.


Journal of Astronomical Telescopes, Instruments, and Systems | 2014

Transiting Exoplanet Survey Satellite

George R. Ricker; Joshua N. Winn; R. Vanderspek; David W. Latham; G. Á. Bakos; Jacob L. Bean; Zachory K. Berta-Thompson; Timothy M. Brown; Lars A. Buchhave; Nathaniel R. Butler; R. Paul Butler; W. J. Chaplin; David Charbonneau; Jørgen Christensen-Dalsgaard; Mark Clampin; Drake Deming; John P. Doty; Nathan De Lee; Courtney D. Dressing; Edward W. Dunham; Michael Endl; Francois Fressin; Jian Ge; Thomas Henning; Matthew J. Holman; Andrew W. Howard; Shigeru Ida; Jon M. Jenkins; Garrett Jernigan; John Asher Johnson

Abstract. The Transiting Exoplanet Survey Satellite (TESS) will search for planets transiting bright and nearby stars. TESS has been selected by NASA for launch in 2017 as an Astrophysics Explorer mission. The spacecraft will be placed into a highly elliptical 13.7-day orbit around the Earth. During its 2-year mission, TESS will employ four wide-field optical charge-coupled device cameras to monitor at least 200,000 main-sequence dwarf stars with IC≈4−13 for temporary drops in brightness caused by planetary transits. Each star will be observed for an interval ranging from 1 month to 1 year, depending mainly on the star’s ecliptic latitude. The longest observing intervals will be for stars near the ecliptic poles, which are the optimal locations for follow-up observations with the James Webb Space Telescope. Brightness measurements of preselected target stars will be recorded every 2 min, and full frame images will be recorded every 30 min. TESS stars will be 10 to 100 times brighter than those surveyed by the pioneering Kepler mission. This will make TESS planets easier to characterize with follow-up observations. TESS is expected to find more than a thousand planets smaller than Neptune, including dozens that are comparable in size to the Earth. Public data releases will occur every 4 months, inviting immediate community-wide efforts to study the new planets. The TESS legacy will be a catalog of the nearest and brightest stars hosting transiting planets, which will endure as highly favorable targets for detailed investigations.


The Astrophysical Journal | 2009

HAT-P-7: A Retrograde or Polar Orbit, and a Third Body

Joshua N. Winn; John Asher Johnson; Simon Albrecht; Andrew W. Howard; Geoffrey W. Marcy; Ian J. M. Crossfield; Matthew J. Holman

We show that the exoplanet HAT-P-7b has an extremely tilted orbit, with a true angle of at least 86° with respect to its parent stars equatorial plane, and a strong possibility of retrograde motion. We also report evidence for an additional planet or companion star. The evidence for the unparalleled orbit and the third body is based on precise observations of the stars apparent radial velocity (RV). The anomalous RV due to rotation (the Rossiter-McLaughlin effect) was found to be a blueshift during the first half of the transit and a redshift during the second half, an inversion of the usual pattern, implying that the angle between the sky-projected orbital and stellar angular momentum vectors is 182°.5 ± 9°.4. The third body is implicated by excess RV variation of the host star over 2 yr. Some possible explanations for the tilted orbit of HAT-P-7b are a close encounter with another planet, the Kozai effect, and resonant capture by an inward-migrating outer planet.


The Astrophysical Journal | 2009

On the Metal Richness of M Dwarfs with Planets

John Asher Johnson; Kevin Apps

Knowledge of the metallicities of M dwarfs rests predominantly on the photometric calibration of Bonfils and collaborators, which predicts that M dwarfs in the solar neighborhood, including those with known planets, are systematically metal poor compared to their higher-mass counterparts. We test this prediction using a volume-limited sample of low-mass stars, together with a subset of M dwarfs with high-metallicity, F, G, and K wide binary companions. We find that the Bonfils et al. photometric calibration systematically underestimates the metallicities of our high-metallicity M dwarfs by an average of 0.32 dex. We derive a new photometric metallicity calibration and show that M dwarfs with planets appear to be systematically metal rich, a result that is consistent with the metallicity distribution of FGK dwarfs with planets.


The Astrophysical Journal | 2014

FRIENDS OF HOT JUPITERS. I. A RADIAL VELOCITY SEARCH FOR MASSIVE, LONG-PERIOD COMPANIONS TO CLOSE-IN GAS GIANT PLANETS

Heather A. Knutson; Benjamin J. Fulton; Benjamin T. Montet; Melodie Kao; Henry Ngo; Andrew W. Howard; Justin R. Crepp; Sasha Hinkley; G. Á. Bakos; Konstantin Batygin; John Asher Johnson; Timothy D. Morton; Philip S. Muirhead

In this paper we search for distant massive companions to known transiting hot Jupiters that may have influenced the dynamical evolution of these systems. We present new radial velocity observations for a sample of 51 hot Jupiters obtained using the Keck HIRES instrument, and use these observations to search for long-term radial velocity accelerations. We find new, statistically significant accelerations in seven systems, including: HAT-P-10, HAT-P-20, HAT-P-22, HAT-P-29, HAT-P-32, WASP-10, and XO-2. We combine our radial velocity fits with Keck NIRC2 AO imaging data to place constraints on the allowed masses and orbital periods of the companions. The estimated masses of the companions range between 1-500 M_(Jup), with orbital semi-major axes typically between 1-75 AU. A significant majority of the companions detected by our survey are constrained to have minimum masses comparable to or larger than those of the short-period hot Jupiters in these systems, making them candidates for influencing the orbital evolution of the inner hot Jupiters. They also appear to occur preferentially in systems with more metal-rich host stars, and with typical orbital separations that are larger than those of multi-planet systems without hot Jupiters. We estimate a total occurrence rate of 55% +11% / -10% for companions with masses between 1-13 M_(Jup) and orbital semi-major axes between 1-20 AU in our sample. We find no statistically significant difference between the frequency of companions in hot Jupiter systems with misaligned or eccentric orbits and those with well-aligned, circular orbits. We combine our expanded sample of radial velocity measurements with constraints from transit and secondary eclipse observations to provide improved measurements of the physical and orbital characteristics of all of the hot Jupiters included in our survey.


The Astrophysical Journal | 2015

THE MASS OF KEPLER-93B AND THE COMPOSITION OF TERRESTRIAL PLANETS *

Courtney D. Dressing; David Charbonneau; X. Dumusque; S. Gettel; F. Pepe; Andrew Collier Cameron; David W. Latham; Emilio Molinari; S. Udry; L. Affer; A. S. Bonomo; Lars A. Buchhave; Rosario Cosentino; P. Figueira; Aldo F. M. Fiorenzano; A. Harutyunyan; R. D. Haywood; John Asher Johnson; Mercedes Lopez-Morales; Christophe Lovis; Luca Malavolta; Michel Mayor; Giusi Micela; Fatemeh Motalebi; Valerio Nascimbeni; David F. Phillips; Giampaolo Piotto; Don Pollacco; D. Queloz; Ken Rice

Kepler-93b is a 1.478 ± 0.019 R⊕ planet with a 4.7 day period around a bright (V = 10.2), astroseismically characterized host star with a mass of 0.911 ± 0.033 Mand a radius of 0.919 ± 0.011 R� . Based on 86 radial velocity observations obtained with the HARPS-N spectrograph on the Telescopio Nazionale Galileo and 32 archival Keck/HIRES observations, we present a precise mass estimate of 4.02 ± 0.68 M⊕. The corresponding high density of 6.88 ± 1.18 g cm −3 is consistent with a rocky composition of primarily iron and magnesium silicate. We compare Kepler-93b to other dense planets with well-constrained parameters and find that between 1 and 6 M⊕, all dense planets including the Earth and Venus are well-described by the same fixed ratio of iron to magnesium silicate. There are as of yet no examples of such planets with masses > 6 M⊕. All known planets in this mass regime have lower densities requiring significant fractions of volatiles or H/He gas. We also constrain the mass and period of the outer companion in the Kepler-93 system from the long-term radial velocity trend and archival adaptive optics images. As the sample of dense planets with well-constrained masses and radii continues to grow, we will be able to test whether the fixed compositional model found for the seven dense planets considered in this paper extends to the full population of 1-6 M⊕ planets.


The Astrophysical Journal | 2009

HAT-P-13b,c: A transiting hot jupiter with a massive outer companion on an eccentric orbit

G. Á. Bakos; Andrew W. Howard; Robert W. Noyes; J. D. Hartman; Guillermo Torres; G. Kovács; Debra A. Fischer; D. W. Latham; John Asher Johnson; G. W. Marcy; Dimitar D. Sasselov; Robert P. Stefanik; B. Sipőcz; Gábor Kovács; Gilbert A. Esquerdo; A. Pál; J. Lázár; I. Papp; P. Sári

We report on the discovery of a planetary system with a close-in transiting hot Jupiter on a near circular orbit and a massive outer planet on a highly eccentric orbit. The inner planet, HAT-P-13b, transits the bright V = 10.622 G4 dwarf star GSC 3416 – 00543 every P = 2.916260 ± 0.000010 days, with transit epoch T_c = 2454779.92979 ± 0.00038 (BJD) and duration 0.1345 ± 0.0017 days. The outer planet HAT-P-13c orbits the star every P_2 = 428.5 ± 3.0 days with a nominal transit center (assuming zero impact parameter) of T_(2c) = 2454870.4 ± 1.8 (BJD) or time of periastron passage T_(2,peri) = 2454890.05 ± 0.48 (BJD). Transits of the outer planet have not been observed, and may not be present. The host star has a mass of 1.22^(+0.05)_(–0.10) M_☉, radius of 1.56 ± 0.08 R_☉, effective temperature of 5653 ± 90 K, and is rather metal-rich with [Fe/H] = +0.41 ± 0.08. The inner planetary companion has a mass of 0.853^(+0.029)_(–0.046) M_J, and radius of 1.281 ± 0.079 R_J, yielding a mean density of 0.498^(+0.103)_(–0.069) g cm^(–3). The outer companion has m_2 sin i_2 = 15.2 ± 1.0 M_J, and orbits on a highly eccentric orbit of e_2 = 0.691 ± 0.018. While we have not detected significant transit timing variations of HAT-P-13b, due to gravitational and light-travel time effects, future observations will constrain the orbital inclination of HAT-P-13c, along with its mutual inclination to HAT-P-13b. The HAT-P-13 (b, c) double-planet system may prove extremely valuable for theoretical studies of the formation and dynamics of planetary systems.


The Astrophysical Journal | 2009

THE NASA-UC ETA-EARTH PROGRAM. I. A SUPER-EARTH ORBITING HD 7924*

Andrew W. Howard; John Asher Johnson; Geoffrey W. Marcy; Debra A. Fischer; Jason T. Wright; Gregory W. Henry; Matthew J. Giguere; Howard Isaacson; Jeff A. Valenti; Jay Anderson; Nikolai Piskunov

We report the discovery of the first low-mass planet to emerge from the NASA-UC Eta-Earth Program, a super-Earth orbiting the K0 dwarf HD 7924. Keplerian modeling of precise Doppler radial velocities reveals a planet with minimum mass M_P sin i = 9.26 M_⊕ in a P = 5.398 d orbit. Based on Keck-HIRES measurements from 2001 to 2008, the planet is robustly detected with an estimated false alarm probability of less than 0.001. Photometric observations using the Automated Photometric Telescopes at Fairborn Observatory show that HD 7924 is photometrically constant over the radial velocity period to 0.19 mmag, supporting the existence of the planetary companion. No transits were detected down to a photometric limit of ~0.5 mmag, eliminating transiting planets with a variety of compositions. HD 7924b is one of only eight planets detected by the radial velocity technique with M_P sin i < 10 M_⊕ and as such is a member of an emerging family of low-mass planets that together constrain theories of planet formation.

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Andrew W. Howard

California Institute of Technology

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Howard Isaacson

San Francisco State University

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Andrew Vanderburg

University of Texas at Austin

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Joshua N. Winn

Massachusetts Institute of Technology

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