10,591 research outputs found
An 80 pc Long Massive Molecular Filament in the Galactic Mid-Plane
The ubiquity of filaments in star forming regions on a range of scales is
clear, yet their role in the star formation process remains in question. We
suggest that there are distinct classes of filaments which are responsible for
their observed diversity in star-forming regions. An example of a massive
molecular filament in the Galactic mid-plane formed at the intersection of
UV-driven bubbles which displays a coherent velocity structure (< 4 km/s) over
80 pc is presented. We classify such sources as Massive Molecular Filaments
(MMFs; M > 10^4 Msun, length > 10 pc, velocity gradient < 5 km/s) and suggest
that MMFs are just one of the many different classes of filaments discussed in
the literature today. Many MMFs are aligned with the Galactic Plane and may be
akin to the dark dust lanes seen in Grand Design Spirals.Comment: To appear in proceedings of the 'Labyrinth of Star Formation' meeting
(18-22 June 2012, Chania, Greece), published by Springe
On the Conformal Geometry of Transverse Riemann-Lorentz Manifolds
Physical reasons suggested in \cite{Ha-Ha} for the \emph{Quantum Gravity
Problem} lead us to study \emph{type-changing metrics} on a manifold. The most
interesting cases are \emph{Transverse Riemann-Lorentz Manifolds}. Here we
study the conformal geometry of such manifolds
Mechanical properties of tungsten alloys with Y2O3 and titanium additions
In this research the mechanical behaviour of pure tungsten (W) and its alloys (2 wt.% Ti–0.47 wt.% Y2O3 and 4 wt.% Ti–0.5 wt.% Y2O3) is compared. These tungsten alloys, have been obtained by powder metallurgy. The yield strength, fracture toughness and elastic modulus have been studied in the temperature interval of 25 °C to 1000 °C. The results have shown that the addition of Ti substantially improves the bending strength and toughness of W, but it also dramatically increases the DBTT. On the other hand, the addition of 0.5% Y2O3, is enough to improve noticeably the oxidation behaviour at the higher temperatures. The grain size, fractography and microstructure are studied in these materials. Titanium is a good grain growth inhibitor and effective precursor of liquid phase in HIP. The simultaneous presence of Y2O3 and Ti permits to obtain materials with low pores presenc
Typical and extreme entropies of long-lived isolated quantum systems
In this paper, we investigate and compare two well-developed definitions of
entropy relevant for describing the dynamics of isolated quantum systems:
bipartite entanglement entropy and observational entropy. In a model system of
interacting particles in a one-dimensional lattice, we numerically solve for
the full quantum behavior of the system. We characterize the fluctuations, and
find the maximal, minimal, and typical entropy of each type that the system can
eventually attain through its evolution. While both entropies are low for some
"special" configurations and high for more "generic" ones, there are several
fundamental differences in their behavior. Observational entropy behaves in
accord with classical Boltzmann entropy (e.g. equilibrium is a condition of
near-maximal entropy and uniformly distributed particles, and minimal entropy
is a very compact configuration). Entanglement entropy is rather different:
minimal entropy "empties out" one partition while maximal entropy apportions
the particles between the partitions, and neither is typical. Beyond these
qualitative results, we characterize both entropies and their fluctuations in
some detail as they depend on temperature, particle number, and box size.Comment: Additional comments are made in the caption of figure 10 (a).
Equation 7 and a brief description are added in relation to figure
A comparison of methods for DPLL loop filter design
Four design methodologies for loop filters for a class of digital phase-locked loops (DPLLs) are presented. The first design maps an optimum analog filter into the digital domain; the second approach designs a filter that minimizes in discrete time weighted combination of the variance of the phase error due to noise and the sum square of the deterministic phase error component; the third method uses Kalman filter estimation theory to design a filter composed of a least squares fading memory estimator and a predictor. The last design relies on classical theory, including rules for the design of compensators. Linear analysis is used throughout the article to compare different designs, and includes stability, steady state performance and transient behavior of the loops. Design methodology is not critical when the loop update rate can be made high relative to loop bandwidth, as the performance approaches that of continuous time. For low update rates, however, the miminization method is significantly superior to the other methods
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