6,505 research outputs found
A Collisional Family in the Classical Kuiper Belt
The dynamical evolution of Classical Kuiper Belt Objects (CKBOs) divides into
two parts, according to the secular theory of test particle orbits. The first
part is a forced oscillation driven by the planets, while the second part is a
free oscillation whose amplitude is determined by the initial orbit of the test
particle. We extract the free orbital inclinations and free orbital
eccentricities from the osculating elements of 125 known CKBOs. The free
inclinations of 32 CKBOs strongly cluster about 2 degrees at orbital semi-major
axes between 44 and 45 AU. We propose that these objects comprise a collisional
family, the first so identified in the Kuiper Belt. Members of this family are
plausibly the fragments of an ancient parent body having a minimum diameter of
\~800 km. This body was disrupted upon colliding with a comparably sized
object, and generated ejecta having similar free inclinations. Our candidate
family is dynamically akin to a sub-family of Koronis asteroids located at
semi-major axes less than 2.91 AU; both families exhibit a wider range in free
eccentricity than in free inclination, implying that the relative velocity
between parent and projectile prior to impact lay mostly in the invariable
plane of the solar system. We urge more discoveries of new CKBOs to test the
reality of our candidate family and physical studies of candidate family
members to probe the heretofore unseen interior of a massive, primitive
planetesimal.Comment: final revised version, accepted to ApJ Letters, includes minor caveat
regarding Koronis asteroid famil
Eccentricity Excitation and Apsidal Resonance Capture in the Planetary System Upsilon Andromedae
The orbits of the outer two known planets orbiting Upsilon Andromedae are
remarkably eccentric. Planet C possesses an orbital eccentricity of e1 = 0.253.
For the more distant planet D, e2 = 0.308. Previous dynamical analyses strongly
suggest that the two orbits are nearly co-planar and are trapped in an apsidal
resonance in which the difference between their longitudes of periastron
undergoes a bounded oscillation about 0 degrees. Here we elucidate the origin
of these large eccentricities and of the apsidal alignment. Resonant
interactions between a remnant circumstellar disk of gas lying exterior to the
orbits of both planets can smoothly grow e2. Secular interactions between
planets D and C can siphon off the eccentricity of the former to grow that of
the latter. Externally amplifying e2 during the phase of the apsidal
oscillation when e2/e1 is smallest drives the oscillation amplitude towards
zero. Thus, the substantial eccentricity of planet C and the locking of orbital
apsides are both consequences of externally pumping the eccentricity of planet
D over timescales exceeding apsidal precession periods of order 1e4 yr. We
explain why the recently detected stellar companion to Upsilon Andromedae is
largely dynamically decoupled from the planetary system.Comment: accepted to Ap
Spectral Energy Distributions of Passive T Tauri Disks: Inclination
We compute spectral energy distributions (SEDs) for passive T Tauri disks
viewed at arbitrary inclinations. Semi-analytic models of disks in radiative
and hydrostatic equilibrium are employed. Over viewing angles for which the
flared disk does not occult the central star, the SED varies negligibly with
inclination. For such aspects, the SED shortward of ~80 microns is particularly
insensitive to orientation, since short wavelength disk emission is dominated
by superheated surface layers which are optically thin. The SED of a nearly
edge-on disk is that of a class I source. The outer disk occults inner disk
regions, and emission shortward of ~30 microns is dramatically extinguished.
Spectral features from dust grains may appear in absorption. However,
millimeter wavelength fluxes decrease by at most a factor of 2 from face-on to
edge-on orientations.
We present illustrative applications of our SED models. The class I source
04108+2803B is considered a T Tauri star hidden from view by an inclined
circumstellar disk. Fits to its observed SED yield model-dependent values for
the disk mass of ~0.015 solar masses and a disk inclination of ~65 degrees
relative to face-on. The class II source GM Aur represents a T Tauri star
unobscured by its circumstellar disk. Fitted parameters include a disk mass of
\~0.050 solar masses and an inclination of ~60 degrees.Comment: Accepted to ApJ, 20 pages, 7 figures, aaspp4.st
On the Plutinos and Twotinos of the Kuiper Belt
We illuminate dynamical properties of Kuiper Belt Objects (KBOs) in the 3:2
(``Plutino'') and 2:1 (``Twotino'') Neptunian resonances within the model of
resonant capture and migration. We analyze a series of numerical integrations,
each involving the 4 migratory giant planets and 400 test particles distributed
throughout trans-Neptunian space, to measure efficiencies of capture as
functions of migration speed. Snapshots of the spatial distribution of resonant
KBOs reveal that Twotinos cluster +/- 75 degrees away from Neptune's longitude,
while Plutinos cluster +/- 90 degrees away. Longitudinal clustering persists
even for surveys that are not volume-limited in their ability to detect
resonant KBOs. Remarkably, between -90 degrees and -60 degrees of Neptune's
longitude, we find the sky density of Twotinos to nearly equal that of
Plutinos, despite the greater average distance of Twotinos. We couple our
findings to observations to crudely estimate that the intrinsic Twotino
population is within a factor of 3 of the Plutino population. Most strikingly,
the migration model predicts that more Twotinos may lie at longitudes behind
that of Neptune than ahead of it. The magnitude of the asymmetry amplifies
dramatically with faster rates of migration and can be as large as 300%. A
differential measurement of the sky density of 2:1 resonant objects behind of
and in front of Neptune's longitude would powerfully constrain the migration
history of that planet.Comment: AJ, in press, to appear in December 2002 issue. For version with
higher resolution figures, see
http://astron.berkeley.edu/~echiang/ppp/ppp.htm
Excitation of Orbital Eccentricities by Repeated Resonance Crossings: Requirements
Divergent migration of planets within a viscous circumstellar disk can
engender resonance crossings and dramatic excitation of orbital eccentricities.
We provide quantitative criteria for the viability of this mechanism. For the
orbits of two bodies to diverge, a ring of viscous material must be shepherded
between them. As the ring diffuses in radius by virtue of its intrinsic
viscosity, the two planets are wedged further apart. The ring mass must be
smaller than the planetary masses so that the crossing of an individual
resonance lasts longer than the resonant libration period. At the same time,
the crossing cannot be of such long duration that the disk's direct influence
on the bodies' eccentricities interferes with the resonant interaction between
the two planets. This last criterion is robustly satisfied because resonant
widths are typically tiny fractions of the orbital radius. We evaluate our
criteria not only for giant planets within gaseous protoplanetary disks, but
also for shepherd moons that bracket narrow planetary rings in the solar
system. A shepherded ring of gas orbiting at a distance of 1 AU from a
solar-type star and having a surface density of less than 500 g/cm^2, a
dimensionless alpha viscosity of 0.1, and a height-to-radius aspect ratio of
0.05 can drive two Jovian-mass planets through the 2:1 and higher-order
resonances so that their eccentricities amplify to values of several tenths.
Because of the requirement that the disk mass in the vicinity of the planets be
smaller than the planet masses, divergent resonance crossings may figure
significantly into the orbital evolution of planets during the later stages of
disk evolution, including the debris disk phase.Comment: ApJ, in press, to appear in February 2003 issu
Keck Pencil-Beam Survey for Faint Kuiper Belt Objects
We present the results of a pencil-beam survey of the Kuiper Belt using the
Keck 10-m telescope. A single 0.01 square degree field is imaged 29 times for a
total integration time of 4.8 hr. Combining exposures in software allows the
detection of Kuiper Belt Objects (KBOs) having visual magnitude V < 27.9. Two
new KBOs are discovered. One object having V = 25.5 lies at a probable
heliocentric distance d = 33 AU. The second object at V = 27.2 is located at d
= 44 AU. Both KBOs have diameters of about 50 km, assuming comet-like albedos
of 4%.
Data from all surveys are pooled to construct the luminosity function from
red magnitude R = 20 to 27. The cumulative number of objects per square degree,
N (< R), is fitted to a power law of the form log_(10) N = 0.52 (R - 23.5).
Differences between power laws reported in the literature are due mainly to
which survey data are incorporated, and not to the method of fitting. The
luminosity function is consistent with a power-law size distribution for
objects having diameters s = 50 to 500 km; dn ~ s^(-q) ds, where the
differential size index q = 3.6 +/- 0.1. The distribution is such that the
smallest objects possess most of the surface area, but the largest bodies
contain the bulk of the mass. Though our inferred size index nearly matches
that derived by Dohnanyi (1969), it is unknown whether catastrophic collisions
are responsible for shaping the size distribution. Implications of the absence
of detections of classical KBOs beyond 50 AU are discussed.Comment: Accepted to AJ. Final proof-edited version: references added,
discussion of G98 revised in sections 4.3 and 5.
ISO LWS Spectra of T Tauri and Herbig AeBe stars
We present an analysis of ISO-LWS spectra of eight T Tauri and Herbig AeBe young stellar objects.
Some of the objects are in the embedded phase of star-formation, whereas others have cleared their environs
but are still surrounded by a circumstellar disk. Fine-structure lines of [OI] and [CII] are most likely excited by
far-ultraviolet photons in the circumstellar environment rather than high-velocity outflows, based on comparisons
of observed line strengths with predictions of photon-dominated and shock chemistry models. A subset of our
stars and their ISO spectra are adequately explained by models constructed by Chiang & Goldreich (1997) and
Chiang et al. (2001) of isolated, passively heated, flared circumstellar disks. For these sources, the bulk of the
LWS flux at wavelengths longward of 55 µm arises from the disk interior which is heated diffusively by reprocessed
radiation from the disk surface. At 45 µm, water ice emission bands appear in spectra of two of the coolest stars,
and are thought to arise from icy grains irradiated by central starlight in optically thin disk surface layers
Hitting Time of Quantum Walks with Perturbation
The hitting time is the required minimum time for a Markov chain-based walk
(classical or quantum) to reach a target state in the state space. We
investigate the effect of the perturbation on the hitting time of a quantum
walk. We obtain an upper bound for the perturbed quantum walk hitting time by
applying Szegedy's work and the perturbation bounds with Weyl's perturbation
theorem on classical matrix. Based on the definition of quantum hitting time
given in MNRS algorithm, we further compute the delayed perturbed hitting time
(DPHT) and delayed perturbed quantum hitting time (DPQHT). We show that the
upper bound for DPQHT is actually greater than the difference between the
square root of the upper bound for a perturbed random walk and the square root
of the lower bound for a random walk.Comment: 9 page
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