The recent ALMA observations of the disk surrounding HL Tau reveal a very complex dust spatial distribution. We present a radiative transfer model accounting for the observed gaps and bright rings as well as radial changes of the emissivity index. We find that the dust density is depleted by at least a factor of 10 in the main gaps compared to the surrounding rings. Ring masses range from 10-100 M ⊕ in dust, and we find that each of the deepest gaps is consistent with the removal of up to 40 M ⊕ of dust. If this material has accumulated into rocky bodies, these would be close to the point of runaway gas accretion. Our model indicates that the outermost ring is depleted in millimeter grains compared to the central rings. This suggests faster grain growth in the central regions and/or radial migration of the larger grains. The morphology of the gaps observed by ALMA -well separated and showing a high degree of contrast with the bright rings over all azimuths -indicates that the millimeter dust disk is geometrically thin (scale height ≈ 1 AU at 100 AU) and that a large amount of settling of large grains has already occurred. Assuming a standard dust settling model, we find that the observations are consistent with a turbulent viscosity coefficient of a few 10 −4 . We estimate the gas/dust ratio in this thin layer to be of the order of 5 if the initial ratio is 100. The HCO + and CO emission is consistent with gas in Keplerian motion around a 1.7 M star at radii from ≤ 10 − 120 AU.
Instrumental setup and data reduction ALMA setup. ALMA Band 7 observations of HD142527 were carried out in the night of June 2 2012. The precipitable water vapor in the atmosphere was stable between 1.4 and 1.8 mm, with clear sky conditions. The ALMA correlator was configured in the Frequency Division Mode (FDM) to provide 468.750 MHz bandwidth in four different spectral windows at 122.07 kHz resolution (0.1 km/s) per channel. Each spectral window was positioned in order to target the CO(3-2) transition at 345.7959 GHz, HCO+ as well as CS(7-6) and HCN(4-3). The measured system temperatures ranged from 207 to 285 K in the different spectral windows. The number of 12 m antennas available at the time of the observation was 19, although two antennas reported very large system temperatures (DA41 and DV12) and were flagged during data reduction. Excluding calibration overheads, a total time on source of 52 minutes was spent yielding an RMS of 15 mJy in 0.1 km s −1 channels. The primary flux calibrator was Titan, which provided a mean transferred flux of 14.2 Jy for 3c279, the bandpass calibrator, and 0.55 Jy for J1604-446, the phase calibrator. Amplitude calibration used the CASA Butler-JPL-Horizons 2010 model for Titan, which gives an estimated systematic flux uncertainty of ⇠10%. All the line data were processed with continuum subtraction in the visibility domain. Image synthesis. Image synthesis was performed using two different techniques, depending on the application. For a traditional way to present the visibility dataset we use Cotton-Schwab CLEAN in the CASA package. This technique represents the consensus in image synthesis. We use Briggs weighting with robustness parameter of zero. For deconvolved models we use a non-parametric least-squares modeling technique 31 with a regularizing entropy term (i.e. as in the family of maximum entropy methods, MEM here and elsewhere). MEM model images are restored by convolving with the clean beam and by adding the residuals calculated using the difmap package 32. For the residuals we use weights comparable to our choice in CASA, a mixture of natural and uniform weights. A detailed example of this MEM algorithm is shown in the HCO + channel maps, Fig. S4. 1 Registration of ALMA images. A ⇠0.1 arcsec astrometric uncertainty could affect the ALMA data. However, we checked the astrometry by confirming that the centroid of the Keplerian velocity field (seen in the RGB image for CO(3-2) in Fig. 1) lies indeed at the po
We present Atacama Large Millimeter/submillimeter Array (ALMA) observations from the 2014 Long Baseline Campaign in dust continuum and spectral line emission from the HL Tau region. The continuum images at wavelengths of 2.9, 1.3, and 0.87 mm have unprecedented angular resolutions of 0″. 075 (10 AU) to 0″. 025 (3.5 AU), revealing an astonishing level of detail in the circumstellar disk surrounding the young solar analog HL Tau, with a pattern of bright and dark rings observed at all wavelengths. By fitting ellipses to the most distinct rings, we measure precise values for the disk inclination (46 .72 0 .05 ± • •) and position angle (138 .02 0 .07).
Discs of gas and dust surrounding young stars are the birthplace of planets. However, the direct detection of protoplanets forming within discs has proved elusive to date. We present the detection of a large, localized deviation from Keplerian velocity in the protoplanetary disc surrounding the young star HD 163296. The observed velocity pattern is consistent with the dynamical effect of a two-Jupiter-mass planet orbiting at a radius ≈ 260 au from the star.
Abstract:Many stars are surrounded by disks of dusty debris formed in the collisions of asteroids, comets and dwarf planets. But is gas also released in such events? Observations at submm wavelengths of the archetypal debris disk around β Pictoris show that 0.3% of a Moon mass of carbon monoxide orbits in its debris belt. The gas distribution is highly asymmetric, with 30% found in a single clump 85AU from the star, in a plane closely aligned with the orbit of the inner planet, β Pic b. This gas clump delineates a region of enhanced collisions, either from a mean motion resonance with an unseen giant planet, or from the remnants of a collision of Mars--mass planets. Main Text:Debris disks are the end product of collisional cascades of km--sized bodies orbiting stars (including the Sun), and are normally thought to contain negligible gas. At a distance of 19.44 parsec (1) and age of 20 million years (2), β Pictoris is one of the closest, brightest and youngest examples. Its edge--on disk was the first to be imaged in scattered light, showing the distribution of micron--sized dust grains (3). Various subsequent observations have provided evidence of infalling comets within a few Astronomical Units (AU) of the star (4), a massive planet at ~10 AU (5), as well as atomic gas extending out to ~300AU (6); it is still unclear how these features are linked. By observing such debris disks at mm wavelengths, it is possible to trace the mm--sized dust and, by inference, the parent bodies of the collisional cascade, known as planetesimals (7).We observed β Pic using the Atacama Large Millimeter/submillimeter Array (ALMA) at a wavelength of 870µm in both the continuum and the J=3--2 12 CO line with a resolution of 12AU (8). The continuum image (Fig.1A) shows maxima in the surface brightness ~60AU either side of the star. At separations from 30--80AU the continuum is, on average, 15% brighter to the southwest. These results indicate that the mm grains lie in a broad slightly asymmetric belt nearly co--located with the disk of sub--micron reflecting dust (9). The total flux of 60±6mJy corresponds to a dust mass of 4.7±0.5x10 23 kg (6.4M Moon ), if we assume a standard dust mass opacity (0.15m 2 kg --1 at 850µm) and temperature of 85K (10).The planet β Pic b was close to maximum SW elongation at the time of the observations, with a projected separation of 8.7AU (11). Its location is coincident with a dip in the continuum surface brightness at a significance level of 4σ, suggesting that it may influence the innermost dust distribution.ALMA also detected the disk in the 12 CO J=3--2 transition (Fig.1B), with a clear velocity gradient along the major axis, illustrated in the position--velocity (PV) diagram (Fig.2). This shows the characteristic distribution of a broad belt of orbiting gas, with inner and outer radii of 50 and 160AU, and a peak around 85AU. No gas 3 emission is seen inside 50AU. The CO distribution is, on average, a factor of 2 brighter to the southwest, and a similar asymmetry was seen in the mid--infrared emission...
We describe results from a survey for J=3-2 12CO emission from visible stars with an infrared excess. The line is clearly detected in 21 objects, with molecular gas (>10^-3 Jupiter masses) common in targets with infrared excesses >0.01 (>56% of objects). Such high excesses indicate the presence of a disc of opening angle >12 degrees; within this, the optically thick disc prevents CO photodissociation. Two or three stars with associated CO have an excess <0.01, implying a disc opening angle <1 degree. Most line profiles are double-peaked or relatively broad. Model fits, assuming a Keplerian disc, indicate outer radii, R_out, of ~20-300 au. As many as 5 discs have outer radii smaller than the Solar System (50 au), and a further 4 have gas at radii <20 au. R_out is independent of the stellar spectral type (from K through to B9), but is correlated with total dust mass. R_out appears to decrease with time: discs around stars of age 3-7 Myr have a mean radius of ~210 au, whereas discs of age 7-20 Myr are a factor of 3 smaller. The only bona fide debris disc with detected CO is HD9672; this has a double peaked line profile and is the most compact gas disc observed, with a modelled radius 17 au). A fit to HD141569 suggests the gas lies in two rings of radii 90 and 250 au, similar to the scattered light structure. In both AB Aur and HD163296 the sizes of the molecular and dust scattering discs are also similar, suggesting that the gas and small dust grains are co-located.Comment: 16 pages, 5 figures MNRAS - accepte
Dust emission around the nearby star ǫ Eridani has been imaged using a new submillimetre camera (SCUBA at the JCMT). At 850 µm wavelength a ring of dust is seen, peaking at 60 AU from the star and with much lower emission inside 30 AU. The mass of the ring is at least ∼ 0.01 M ⊕ in dust, while an upper limit of 0.4 M ⊕ in molecular gas is imposed by CO observations. The total mass is comparable to the estimated amount of material, 0.04-0.3 M ⊕ , in comets orbiting the Solar System.The most probable origin of the the ring structure is that it is a young analogue to the Kuiper Belt in our Solar System, and that the central region has been partially cleared by the formation of grains into planetesimals. Dust clearing around ǫ Eri is seen within the radius of Neptune's orbit, and the peak emission at 35-75 AU lies within the estimated Kuiper Belt zone of 30-100 AU radius. ǫ Eri is a main-sequence star of type K2V (0.8 M ⊙ ) with an estimated age of 0.5-1.0 Gyr, so this interpretation is consistent with the early history of the Solar System where heavy bombardment occurred up to ≈ 0.6 Gyr. An unexpected discovery is substructure within the ring, and these asymmetries could be due to perturbations by planets.
Accurate measurements of the physical structure of protoplanetary discs are critical inputs for planet formation models. These constraints are traditionally established via complex modelling of continuum and line observations. Instead, we present an empirical framework to locate the CO isotopologue emitting surfaces from high spectral and spatial resolution ALMA observations. We apply this framework to the disc surrounding IM Lupi, where we report the first direct, i.e. model independent, measurements of the radial and vertical gradients of temperature and velocity in a protoplanetary disc. The measured disc structure is consistent with an irradiated self-similar disc structure, where the temperature increases and the velocity decreases towards the disc surface. We also directly map the vertical CO snow line, which is located at about one gas scale height at radii between 150 and 300 au, with a CO freeze-out temperature of 21 ± 2 K. In the outer disc (> 300 au), where the gas surface density transitions from a power law to an exponential taper, the velocity rotation field becomes significantly sub-Keplerian, in agreement with the expected steeper pressure gradient. The sub-Keplerian velocities should result in a very efficient inward migration of large dust grains, explaining the lack of millimetre continuum emission outside of 300 au. The sub-Keplerian motions may also be the signature of the base of an externally irradiated photo-evaporative wind. In the same outer region, the measured CO temperature above the snow line decreases to ≈ 15 K because of the reduced gas density, which can result in a lower CO freeze-out temperature, photo-desorption, or deviations from local thermodynamic equilibrium.
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