39,678 research outputs found
Orion Revisited - I. The massive cluster in front of the Orion Nebula Cluster
The aim of this work is to characterize the stellar population between Earth
and the Orion A molecular cloud where the well known star formation benchmark
Orion Nebula Cluster (ONC) is embedded. We use the denser regions the Orion A
cloud to block optical background light, effectively isolating the stellar
population in front of it. We then use a multi-wavelength observational
approach to characterize the cloud's foreground stellar population. We find
that there is a rich stellar population in front of the Orion A cloud, from
B-stars to M-stars, with a distinct 1) spatial distribution, 2) luminosity
function, and 3) velocity dispersion from the reddened population inside the
Orion A cloud. The spatial distribution of this population peaks strongly
around NGC 1980 (iota Ori) and is, in all likelihood, the extended stellar
content of this poorly studied cluster. We infer an age of ~4-5 Myr for NGC
1980 and estimate a cluster population of the order of 2000 stars, which makes
it one of the most massive clusters in the entire Orion complex. What is
currently taken in the literature as the ONC is then a mix of several
intrinsically different populations, namely: 1) the youngest population,
including the Trapezium cluster and ongoing star formation in the dense gas
inside the nebula, 2) the foreground population, dominated by the NGC 1980
cluster, and 3) the poorly constrained population of foreground and background
Galactic field stars. Our results support a scenario where the ONC and L1641N
are not directly associated with NGC 1980, i.e., they are not the same
population emerging from its parental cloud, but are instead distinct
overlapping populations. This result calls for a revision of most of the
observables in the benchmark ONC region (e.g., ages, age spread, cluster size,
mass function, disk frequency, etc.). (abridged)Comment: Version 2 includes comments and clarifications from John Tobin,
Nicola Da Rio, and Lynne Hillenbrand (minor clarifying changes were made to
Figures 1, 8, and 10). A&A accepted (15 pages, 10 figures). Higher resolution
figures available upon reques
Yang-Lee zeros and the helix-coil transition in a continuum model of polyalanine
We calculate the Yang-Lee zeros for characteristic temperatures of the
helix-coil transition in a continuum model of polyalanine. The distribution of
these zeros differs from predictions of the Zimm-Bragg theory and supports
recent claims that polyalanine exhibits a true phase transition. New estimates
for critical exponents are presented and the relation of our results to the
Lee-Yang theorem is discussed.Comment: 15 pages and 5 figure
Ab initio calculation of the dynamical properties of PPP and PPV
In this work, we have calculated the vibrational modes and frequencies of the
crystalline PPP (in both the Pbam and Pnnm symmetries) and PPV (in the P21/c
symmetry). Our results are in good agreement with the available experimental
data. Also, we have calculated the temperature dependence of their specific
heats at constant volume, and of their vibrational entropies. Based on our
results, at high temperatures, the PPP is more stable in the Pnnm structure
than in the Pbam one.Comment: 5 pages, 7 figures, accepted for publication in Braz. J. Phys.,
special number, Proceedings of BWSP-12, 12th Brazilian Workshop on
Semiconductor Physic
On special limits of the Mixed Painlev\'e P Model
The paper discusses P equation for special values of its parameters
for which this equation reduces to P, I, as well as, to some
special cases of I and I equations from the Ince's list of
second order differential equations possessing Painlev\'e property.
These reductions also yield symmetries governing the reduced models obtained
from the P equation. We point out that the solvable equations on
Ince's list emerge in this reduction scheme when the underlying reflections of
the Weyl symmetry group no longer include an affine reflection through the
hyperplane orthogonal to the highest root and therefore do not give rise to an
affine Weyl group. We hypothesize that on the level of the underlying algebra
and geometry this might be a fundamental feature that distinguishes the six
Painlev\'e equations from the remaining solvable equations on the Ince's
list.Comment: 10 pages, Proc. of the 32nd International Colloquium on Group
Theoretical Methods in Physics (Group32), 2018, Prague, Czech Republi
Optimized cross-slot flow geometry for microfluidic extension rheometry
A precision-machined cross-slot flow geometry with a shape that has been optimized by numerical simulation of the fluid kinematics is fabricated and used to measure the extensional viscosity of a dilute polymer solution. Full-field birefringence microscopy is used to monitor the evolution and growth of macromolecular anisotropy along the stagnation point streamline, and we observe the formation of a strong and uniform birefringent strand when the dimensionless flow strength exceeds a critical Weissenberg number Wicrit 0:5. Birefringence and bulk pressure drop measurements provide self consistent estimates of the planar extensional viscosity of the fluid over a wide range of deformation rates (26 s1 "_ 435 s1) and are also in close agreement with numerical simulations performed by using a finitely extensible nonlinear elastic dumbbell model
Structural transitions in biomolecules - a numerical comparison of two approaches for the study of phase transitions in small systems
We compare two recently proposed methods for the characterization of phase
transitions in small systems. The usefulness of these techniques is evaluated
for the case of structural transition in alanine-based peptides.Comment: Accepted for publication in Int. J. Mol. Sci., to appear in a special
issue devoted to R.S. Berr
Helix Formation and Folding in an Artificial Peptide
We study the relation between -helix formation and folding for a
simple artificial peptide, Ala-Gly-Ala. Our data rely on
multicanonical Monte Carlo simulations where the interactions among all atoms
are taken into account. The free-energy landscape of the peptide is evaluated
for various temperatures. Our data indicate that folding of this peptide is a
two-step process: in a first step two -helices are formed which
afterwards re-arrange themselves into a U-like structure.Comment: 15 pages, with 9 eps figure
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