4,753 research outputs found
Massive envelopes and filaments in the NGC 3603 star forming region
The formation of massive stars and their arrival on the zero-age
main-sequence occurs hidden behind dense clouds of gas and dust. In the giant
Hii region NGC 3603, the radiation of a young cluster of OB stars has dispersed
dust and gas in its vicinity. At a projected distance of 2:5 pc from the
cluster, a bright mid-infrared (mid-IR) source (IRS 9A) had been identified as
a massive young stellar object (MYSO), located on the side of a molecular clump
(MM2) of gas facing the cluster. We investigated the physical conditions in
MM2, based on APEX sub-mm observations using the SABOCA and SHFI instruments,
and archival ATCA 3 mm continuum and CS spectral line data. We resolved MM2
into several compact cores, one of them closely associated with IRS 9A. These
are likely infrared dark clouds as they do not show the typical hot-core
emission lines and are mostly opaque against the mid-IR background. The compact
cores have masses of up to several hundred times the solar mass and gas
temperatures of about 50 K, without evidence of internal ionizing sources. We
speculate that IRS 9A is younger than the cluster stars, but is in an
evolutionary state after that of the compact cores
Uniform in time Lâ estimates for an attraction-repulsion chemotaxis model with double saturation
In this paper we focus on this attraction-repulsion chemotaxis model with consumed signals {ut = ?u - chi & nabla; middot (u & nabla;v) + xi & nabla; middot (u & nabla;w) in ? x (0, T-max),vt = ?v - uv in ? x (0, T-max),wt = ?w - uw in ? x (0, T-max), (?) formulated in a bounded and smooth domain ? of R-n, with n >= 2, for some positive real numbers chi, xi and with T-max is an element of (0, infinity]. Once equipped with appropriately smooth initial distributions u(x, 0) = u(0)(x) >= 0, v(x, 0) = v(0)(x) >= 0 and w(x, 0) = w(0)(x) >= 0, as well as Neumann boundary conditions, we establish sufficient assumptions on its data yielding global and bounded classical solutions; these are functions u, v and w, with zero normal derivative on & part;? x (0, T-max), satisfying pointwise the equations in problem (? ) with T-max = infinity. This is proved for any such initial data, whenever chi and xi belong to bounded and open intervals, depending respectively on Ilv(0)Il(L infinity()?) and Ilw0Il(L infinity)(?). Finally, we illustrate some aspects of the dynamics present within the chemotaxis system by means of numerical simulations
Performance of two transferred modules in the Lagunera Region: Water relations
Water policy / Performance / Privatization / Irrigation systems / Operations / Maintenance / Irrigation efficiency / Water users' associations / Water rights / Water allocation / Water supply / Water distribution
Human-robot visual interface for 3D steering of a flexible, bioinspired needle for neurosurgery
Robotic minimally invasive surgery has been a subject of intense research and development over the last three decades, due to the clinical advantages it holds for patients and doctors alike. Particularly for drug delivery mechanisms, higher precision and the ability to follow complex trajectories in three dimensions (3D), has led to interest in flexible, steerable needles such as the programmable bevel-tip needle (PBN). Steering in 3D, however, holds practical challenges for surgeons, as interfaces are traditionally designed for straight line paths. This work presents a pilot study undertaken to evaluate a novel human-machine visual interface for the steering of a robotic PBN, where both qualitative evaluation of the interface and quantitative evaluation of the performance of the subjects in following a 3D path are measured. A series of needle insertions are performed in phantom tissue (gelatin) by the experiment subjects. User could adequately use the system with little training and low workload, and reach the target point at the end of the path with millimeter range accuracy
Thermally-driven phase transitions in freestanding low-buckled silicene, germanene, and stanene
Low-buckled silicene, germanene, and stanene are group graphene
allotropes. They form a honeycomb lattice out of two interpenetrating ( and
) triangular sublattices that are vertically separated by a small distance
. The atomic numbers of silicon, germanium, and tin are larger to
carbon's (), making them the first experimentally viable two-dimensional
topological insulators. Those materials have a twice-energy-degenerate
atomistic structure characterized by the buckling direction of the
sublattice with respect to the sublattice [whereby the atom either
protrudes {\em above} () or {\em below} () the
atoms], and the consequences of that energy degeneracy on their elastic and
electronic properties have not been reported thus far. Here, we uncover {\em
ferroelastic, bistable} behavior on silicene, which turns into an {\em average}
planar structure at about 600 K. Further, the creation of electron and hole
puddles obfuscates the zero-temperature SOC induced band gaps at temperatures
as low as 200 K, which may discard silicene as a viable two-dimensional
topological insulator for room temperature applications. Germanene, on the
other hand, never undergoes a low-buckled to planar 2D transformation, becoming
amorphous at around 675 K instead, and preserving its SOC-induced bandgap
despite of band broadening. Stanene undergoes a transition onto a crystalline
3D structure at about 300 K, preserving its SOC-induced electronic band gap up
to that temperature. Unlike what is observed in silicene and germanene, stanene
readily develops a higher-coordinated structure with a high degree of
structural order. The structural phenomena is shown to have deep-reaching
consequences for the electronic and vibrational properties of those two
dimensional topological insulators.Comment: 16 pages, 21 figures. Originally submitted on December 5, 202
Statistics of Core Lifetimes in Numerical Simulations of Turbulent, Magnetically Supercritical Molecular Clouds
We present measurements of the mean dense core lifetimes in numerical
simulations of magnetically supercritical, turbulent, isothermal molecular
clouds, in order to compare with observational determinations. "Prestellar"
lifetimes (given as a function of the mean density within the cores, which in
turn is determined by the density threshold n_thr used to define them) are
consistent with observationally reported values, ranging from a few to several
free-fall times. We also present estimates of the fraction of cores in the
"prestellar", "stellar'', and "failed" (those cores that redisperse back into
the environment) stages as a function of n_thr. The number ratios are measured
indirectly in the simulations due to their resolution limitations. Our approach
contains one free parameter, the lifetime of a protostellar object t_yso (Class
0 + Class I stages), which is outside the realm of the simulations. Assuming a
value t_yso = 0.46 Myr, we obtain number ratios of starless to stellar cores
ranging from 4-5 at n_thr = 1.5 x 10^4 cm^-3 to 1 at n_thr = 1.2 x 10^5 cm^-3,
again in good agreement with observational determinations. We also find that
the mass in the failed cores is comparable to that in stellar cores at n_thr =
1.5 x 10^4 cm^-3, but becomes negligible at n_thr = 1.2 x 10^5 cm^-3, in
agreement with recent observational suggestions that at the latter densities
the cores are in general gravitationally dominated. We conclude by noting that
the timescale for core contraction and collapse is virtually the same in the
subcritical, ambipolar diffusion-mediated model of star formation, in the model
of star formation in turbulent supercritical clouds, and in a model
intermediate between the previous two, for currently accepted values of the
clouds' magnetic criticality.Comment: 25 pages, 8 figures, ApJ accepted. Fig.1 animation is at
http://www.astrosmo.unam.mx/~e.vazquez/turbulence/movies/Galvan_etal07/Galvan_etal07.htm
The Q-Sort Method: Assessing Reliability And Construct Validity Of Questionnaire Items At A Pre-Testing Stage
This paper describes the Q-sort, which is a method of assessing reliability and construct validity of questionnaire items at a pre-testing stage. The method uses Cohen\u27s Kappa and Moore and Benbasat\u27s Hit Ratio in assessing the questionnaire
A composite hydrogel for brain tissue phantoms
Synthetic phantoms are valuable tools for training, research and development in traditional and computer aided surgery, but complex organs, such as the brain, are difficult to replicate. Here, we present the development of a new composite hydrogel capable of mimicking the mechanical response of brain tissue under loading. Our results demonstrate how the combination of two different hydrogels, whose synergistic interaction results in a highly tunable blend, produces a hybrid material that closely matches the strongly dynamic and non-linear response of brain tissue. The new synthetic material is inexpensive, simple to prepare, and its constitutive components are both widely available and biocompatible. Our investigation of the properties of this engineered tissue, using both small scale testing and life-sized brain phantoms, shows that it is suitable for reproducing the brain shift phenomenon and brain tissue response to indentation and palpation
The Magnetic Electron Ion Spectrometer (MagEIS) Instruments Aboard the Radiation Belt Storm Probes (RBSP) Spacecraft
This paper describes the Magnetic Electron Ion Spectrometer (MagEIS) instruments aboard the RBSP spacecraft from an instrumentation and engineering point of view. There are four magnetic spectrometers aboard each of the two spacecraft, one low-energy unit (20â240 keV), two medium-energy units (80â1200 keV), and a high-energy unit (800â4800 keV). The high unit also contains a proton telescope (55 keVâ20 MeV). The magnetic spectrometers focus electrons within a selected energy pass band upon a focal plane of several silicon detectors where pulse-height analysis is used to determine if the energy of the incident electron is appropriate for the electron momentum selected by the magnet. Thus each event is a two-parameter analysis, an approach leading to a greatly reduced background. The physics of these instruments are described in detail followed by the engineering implementation. The data outputs are described, and examples of the calibration results and early flight data presented
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