5,303 research outputs found
Resolved Imaging of the HD191089 Debris Disc
Two thirds of the F star members of the 12 Myr old Beta Pictoris Moving Group
(BPMG) show significant excess emission in the mid-infrared, several million
years after the expected dispersal of the protoplanetary disc. Theoretical
models of planet formation suggest that this peak in the mid-infrared emission
could be due to the formation of Pluto-sized bodies in the disc, which ignite
the collisional cascade and enhance the production of small dust. Here we
present resolved mid-infrared imaging of the disc of HD191089 (F5V in the BPMG)
and consider its implications for the state of planet formation in this system.
HD191089 was observed at 18.3 microns using T-ReCS on Gemini South and the
images were compared to models of the disc to constrain the radial distribution
of the dust. The emission observed at 18.3 microns is shown to be significantly
extended beyond the PSF at a position angle of 80 degrees. This is the first
time dust emission has been resolved around HD191089. Modelling indicates that
the emission arises from a dust belt from 28-90 AU, inclined at 35 degrees from
edge on with very little emission from the inner 28AU of the disc, indicating
the presence of an inner cavity. The steep slope of the inner edge is more
consistent with truncation by a planet than with ongoing stirring. A tentative
brightness asymmetry F(W)/F(E)=0.80+/-0.12 (1.8 sigma) between the two sides of
the disc could be evidence for perturbations from a massive body on an
eccentric orbit in the system.Comment: 11 Pages Accepted to MNRA
On the observability of resonant structures in planetesimal disks due to planetary migration
We present a thorough study of the impact of a migrating planet on a
planetesimal disk, by exploring a broad range of masses and eccentricities for
the planet. We discuss the sensitivity of the structures generated in debris
disks to the basic planet parameters. We perform many N-body numerical
simulations, using the symplectic integrator SWIFT, taking into account the
gravitational influence of the star and the planet on massless test particles.
A constant migration rate is assumed for the planet. The effect of planetary
migration on the trapping of particles in mean motion resonances is found to be
very sensitive to the initial eccentricity of the planet and of the
planetesimals. A planetary eccentricity as low as 0.05 is enough to smear out
all the resonant structures, except for the most massive planets. The
planetesimals also initially have to be on orbits with a mean eccentricity of
less than than 0.1 in order to keep the resonant clumps visible. This numerical
work extends previous analytical studies and provides a collection of disk
images that may help in interpreting the observations of structures in debris
disks. Overall, it shows that stringent conditions must be fulfilled to obtain
observable resonant structures in debris disks. Theoretical models of the
origin of planetary migration will therefore have to explain how planetary
systems remain in a suitable configuration to reproduce the observed
structures.Comment: 16 pages, 13 figures. Accepted for publication in A&
Collisional evolution of eccentric planetesimal swarms
Models for the steady state collisional evolution of low eccentricity
planetesimal belts identify debris disks with hot dust at 1AU, like eta Corvi
and HD69830, as anomalous since collisional processing should have removed most
of the planetesimal mass over their >1 Gyr lifetimes. This paper looks at the
effect of large planetesimal eccentricities (e>>0.3) on their collisional
lifetime and the amount of mass that can remain at late times M_{late}. For an
axisymmetric planetesimal disk with common pericentres and eccentricities e, we
find that M_{late} \propto e^{-5/3}(1+e)^{4/3}(1-e)^{-3}. For a scattered
disk-like population (i.e., common pericentres), in the absence of dynamical
evolution, the mass evolution at late times would be as if only planetesimals
with the largest eccentricity were present. Despite the increased remaining
mass, higher eccentricities do not increase the hot emission from the
collisional cascade until e>0.99, partly because most collisions occur near
pericentre thus increasing the dust blow-out diameter. However, at high
eccentricities (e>0.97) the blow-out population extending out from pericentre
may be detectable above the collisional cascade; higher eccentricities also
increase the probability of witnessing a recent collision. All of the imaging
and spectroscopic constraints for eta Corvi can be explained with a single
planetesimal population with pericentre at 0.75AU, apocentre at 150AU, and mass
5M_\oplus; however, the origin of such a high eccentricity population remains
challenging. The mid-IR excess to HD69830 can be explained by the ongoing
destruction of a debris belt produced in a recent collision in an eccentric
planetesimal belt, but the lack of far-IR emission requires small bound grains
to be absent from the parent planetesimal belt, possibly due to sublimation.Comment: MNRAS in pres
Steady-state evolution of debris disks around A stars
In this paper a simple analytical model for the steady-state evolution of
debris disks due to collisions is confronted with Spitzer observations of main
sequence A stars. All stars are assumed to have planetesimal belts with a
distribution of initial masses and radii. In the model disk mass is constant
until the largest planetesimals reach collisional equilibrium whereupon the
mass falls off oc 1/t. We find that the detection statistics and trends seen at
both 24 and 70um can be fitted well by the model. While there is no need to
invoke stochastic evolution or delayed stirring to explain the statistics, a
moderate rate of stochastic events is not ruled out. Potentially anomalous
systems are identified by a high dust luminosity compared with the maximum
permissible in the model (HD3003, HD38678, HD115892, HD172555). Their
planetesimals may have unusual properties (high strength or low eccentricity)
or this dust could be transient. While transient phenomena are also favored for
a few systems in the literature, the overall success of our model, which
assumes planetesimals in all belts have the same strength, eccentricity and
maximum size, suggests a large degree of uniformity in the outcome of planet
formation. The distribution of planetesimal belt radii, once corrected for
detection bias, follows N(r) oc r^{-0.8+-0.3} for 3-120AU. Since the inner edge
is often attributed to an unseen planet, this provides a unique constraint on
the planetary systems of A stars. It is also shown that P-R drag may sculpt the
inner edges of A star disks close to the Spitzer detection threshold (HD2262,
HD19356, HD106591, HD115892). This model can be readily applied to the
interpretation of future surveys, and predictions are made for the upcoming
SCUBA-2 survey, including that >17% of A stars should be detectable at 850um.Comment: Accepted by Ap
Transience of hot dust around sun-like stars
There is currently debate over whether the dust content of planetary systems
is stochastically regenerated or originates in planetesimal belts evolving in
steady state. In this paper a simple model for the steady state evolution of
debris disks due to collisions is developed and confronted with the properties
of the emerging population of 7 sun-like stars that have hot dust <10AU. The
model shows there is a maximum possible disk mass at a given age, since more
massive primordial disks process their mass faster. The corresponding maximum
dust luminosity is f_max=0.00016r^(7/3)/t_age. The majority (4/7) of the hot
disks exceed this limit by >1000 and so cannot be the products of massive
asteroid belts, rather the following systems must be undergoing transient
events characterized by an unusually high dust content near the star: eta
Corvi, HD69830, HD72905 and BD+20307. It is also shown that the hot dust cannot
originate in a recent collision in an asteroid belt, since there is also a
maximum rate at which collisions of sufficient magnitude to reproduce a given
dust luminosity can occur. Further it is shown that the planetesimal belt
feeding the dust in these systems must be located further from the star than
the dust, typically at >2AU. Other notable properties of the 4 hot dust systems
are: two also have a planetesimal belt at >10AU (eta Corvi and HD72905); one
has 3 Neptune mass planets at <1AU (HD69830); all exhibit strong silicate
features in the mid-IR. We consider the most likely origin for the dust in
these systems to be a dynamical instability which scattered planetesimals
inwards from a more distant planetesimal belt in an event akin to the Late
Heavy Bombardment in our own system, the dust being released from such
planetesimals in collisions and possibly also sublimation.Comment: 16 pages, accepted by ApJ, removed HD128400 as hot dust candidat
Reflections on a Mentoring Partnership Journey
This commentary offers reflection on the mentoring partnership journey between a senior Fellow of the American Academy of Health Behavior (AAHB) and three early- or mid-career AAHB members. Their partnership was supported by the AAHB Research Scholars Mentorship Program. The authors discuss the nature of their working relationship, products they generated, and other lessons learned from the experience. The authors also offer their perspectives on effective mentorship characteristics
Recommended from our members
SN 2017gmr: An Energetic Type II-P Supernova with Asymmetries
We present high-cadence UV, optical, and near-infrared data on the luminous Type II-P supernova SN 2017gmr from hours after discovery through the first 180 days. SN 2017gmr does not show signs of narrow, high-ionization emission lines in the early optical spectra, yet the optical light-curve evolution suggests that an extra energy source from circumstellar medium (CSM) interaction must be present for at least 2 days after explosion. Modeling of the early light curve indicates a ~500 R ⊙ progenitor radius, consistent with a rather compact red supergiant, and late-time luminosities indicate that up to 0.130 ± 0.026 M ⊙ of 56Ni are present, if the light curve is solely powered by radioactive decay, although the 56Ni mass may be lower if CSM interaction contributes to the post-plateau luminosity. Prominent multipeaked emission lines of Hα and [O i] emerge after day 154, as a result of either an asymmetric explosion or asymmetries in the CSM. The lack of narrow lines within the first 2 days of explosion in the likely presence of CSM interaction may be an example of close, dense, asymmetric CSM that is quickly enveloped by the spherical supernova ejecta.NSFNational Science Foundation (NSF) [AST-1813825, AST-1515559, AST-1821987, 1821967, AST-1813176, AST-1313484, 1829740]; Department of Science and Technology (DST), Govt. of IndiaDepartment of Science & Technology (India); Indo-US Science and Technology Forum (IUSSTF); LSSTC Data Science Fellowship Program - LSSTC; Brinson Foundation; Moore FoundationGordon and Betty Moore Foundation; project "Transient Astrophysical Objects" of the National Research, Development and Innovation Office (NKFIH), Hungary - European Union [GINOP-2-3-2-15-2016-00033]; Chinese Academy of Sciences (CAS)Chinese Academy of Sciences; Swedish Research Council (Vetenskapsradet)Swedish Research Council; Swedish National Space Board; research environment grant "Gravitational Radiation and Electromagnetic Astrophysical Transients (GREAT)"; Packard FoundationThe David & Lucile Packard Foundation; "Millennium Institute of Astrophysics (MAS)" of the Iniciativa Cientifica Milenio del Ministerio Economia, Fomento y Turismo de Chile [IC120009]; CONICYT PAI/INDUSTRIA [79090016]; Science and Engineering Research Board (SERB) under the Department of Science AMP; Technology, Govt. of India [PDF/2016/001563]; Ministry of Economy, Development, and Tourism's Millennium Science Inititative [IC120009]; H2020 through an ERC Starting Grant [758638]; FONDECYTComision Nacional de Investigacion Cientifica y Tecnologica (CONICYT)CONICYT FONDECYT [11170953]; Polish NCN MAESTRO grant [2014/14/A/ST9/00121]; PRIN INAF 2017 "Towards the SKA and CTA era: discovery, localisation and physics of transient sources (PI M. Giroletti)"; Independent Research Fund Denmark [8021-00170B]; VILLUM FONDEN [13261, 16599]; Spanish MICINN grant [ESP2017-82674-R]; FEDER fundsEuropean Union (EU); National Science FoundationNational Science Foundation (NSF) [AST-1613472]; National Natural Science Foundation of China (NSFC)National Natural Science Foundation of China [11325313, 11633002, 11761141001]; National Program on Key Research and Development Project [2016YFA0400803]; Open Project Program of the Key Laboratory of Optical Astronomy, National Astronomical Observatories, Chinese Academy of Sciences; IDA (Instrumentation center for Danish Astrophysics); Gemini Observatory [GN-2017B-Q-52]; European Southern Observatory [099.D-0543(A)]; W. M. Keck FoundationW.M. Keck Foundation [NNH14CK55B]; National Aeronautics and Space AdministrationNational Aeronautics & Space Administration (NASA); National Science FoundationNational Science Foundation (NSF); NASAs Astrophysics Data Analysis Program [NNX13AF35G]This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at [email protected]
Attitudes Toward Breast Cancer Genetic Testing in Five Special Population Groups
Purpose: This study examined interest in and attitudes toward genetic testing in 5 different population groups.
Methods: The survey included African American, Asian American, Latina, Native American, and Appalachian women with varying familial histories of breast cancer. A total of 49 women were interviewed in person. Descriptive and nonparametric statistical techniques were used to assess ethnic group differences.
Results: Overall, interest in testing was high. All groups endorsed more benefits than risks. There were group differences regarding endorsement of specific benefits and risks: testing to “follow doctor recommendations” (p=0.017), “concern for effects on family” (p=0.044), “distrust of modern medicine” (p=0.036), “cost” (p=0.025), and “concerns about communication of results to others” (p=0.032). There was a significant inverse relationship between interest and genetic testing cost (p
Conclusion: Cost may be an important barrier to obtaining genetic testing services, and participants would benefit by genetic counseling that incorporates the unique cultural values and beliefs of each group to create an individualized, culturally competent program. Further research about attitudes toward genetic testing is needed among Asian Americans, Native Americans, and Appalachians for whom data are severely lacking. Future study of the different Latina perceptions toward genetic testing are encouraged
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