13,324 research outputs found

    The pulsed air gust generator Final report

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    Wind tunnel simulation of jet pulsing apparatus for controlled gust

    Bargmann representations for deformed harmonic oscillators

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    Generalizing the case of the usual harmonic oscillator, we look for Bargmann representations corresponding to deformed harmonic oscillators. Deformed harmonic oscillator algebras are generated by four operators a,a,Na, a^\dagger, N and the unity 1 such as [a,N]=a,[a,N]=a[a,N] = a, [a^\dagger,N] = -a^\dagger, aa=ψ(N)a^\dagger a = \psi(N) and aa=ψ(N+1)aa^\dagger =\psi(N+1). We discuss the conditions of existence of a scalar product expressed with a true integral on the space spanned by the eigenstates of aa (or aa^\dagger). We give various examples, in particular we consider functions ψ\psi that are linear combinations of qNq^N, qNq^{-N} and unity and that correspond to q-oscillators with Fock-representations or with non-Fock-representations.Comment: 23 pages, Late

    Point sets that minimize (k)(\le k)-edges, 3-decomposable drawings, and the rectilinear crossing number of K30K_{30}

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    There are two properties shared by all known crossing-minimizing geometric drawings of KnK_n, for nn a multiple of 3. First, the underlying nn-point set of these drawings has exactly 3(k+22)3\binom{k+2}{2} (k)(\le k)-edges, for all 0k<n/30\le k < n/3. Second, all such drawings have the nn points divided into three groups of equal size; this last property is captured under the concept of 3-decomposability. In this paper we show that these properties are tightly related: every nn-point set with exactly 3(k+22)3\binom{k+2}{2} (k)(\le k)-edges for all 0k<n/30\le k < n/3, is 3-decomposable. As an application, we prove that the rectilinear crossing number of K30K_{30} is 9726.Comment: 14 page

    M31's Heavy Element Distribution and Outer Disk

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    Hubble Space Telescope imaging of 11 fields in M31 were reduced to color-magnitude diagrams. The fields were chosen to sample all galactocentric radii to 50 kpc. Assuming that the bulk of the sampled stellar populations are older than a few Gyr, the colors of the red giants map to an abundance distribution with errors of order 0.1 dex in abundance. The radially sampled abundance distributions are all about the same width, but show a mild abundance gradient that flattens outside ~20 kpc. The various distributions were weighted and summed with the aid of new surface brightness profile fits to obtain an abundance distribution representative of the entirety of M31. M31 is a system near chemical maturity. This ``observed closed box'' is compared to analytical closed box models. M31 suffers from a lack of metal-poor stars and metal-rich stars relative to the simplest closed-box model in the same way as the solar neighborhood.Comparing to several simple chemical evolution models, neither complete mixing of gas at all times nor zero mixing, inhomogeneous models give the most convincing match to the data. As noted elsewhere, the outer disk of M31 is a factor of ten more metal-rich than the Milky Way halo, ten times more metal-rich than the dwarf spheroidals cospatial with it, and more metal-rich than most of the globular clusters at the same galactocentric radius. Difficulties of interpretation are greatly eased if we posit that the M31 disk dominates over the halo at all radii out to 50 kpc. In fact, scaling from current density models of the Milky Way, one should not expect to see halo stars dominating over disk stars until beyond our 50 kpc limit. A corollary conclusion is that most published studies of the M31 "halo" are actually studies of its disk.Comment: 28 pages, 11 black-and-white figures, in press, Astrophysical Journa

    Upper Limits on the Extragalactic Background Light from the Gamma-Ray Spectra of Blazars

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    The direct measurement of the extragalactic background light (EBL) is difficult at optical to infrared wavelengths because of the strong foreground radiation originating in the Solar System. Very high energy (VHE, E>>100 GeV) gamma rays interact with EBL photons of these wavelengths through pair production. In this work, the available VHE spectra from six blazars are used to place upper limits on the EBL. These blazars have been detected over a range of redshifts and a steepening of the spectral index is observed with increasing source distance. This can be interpreted as absorption by the EBL. In general, knowledge of the intrinsic source spectrum is necessary to determine the density of the intervening EBL. Motivated by the observed spectral steepening with redshift, upper limits on the EBL are derived by assuming that the intrinsic spectra of the six blazars are E1.8\propto E^{-1.8}. Upper limits are then placed on the EBL flux at discrete energies without assuming a specific spectral shape for the EBL. This is an advantage over other methods since the EBL spectrum is uncertain.Comment: 33 pages, 14 figures, accepted by Ap

    Evidence for a Young Stellar Population in NGC 5018

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    Two absorption line indices, Ca II and Hdelta/FeI4045, measured from high resolution spectra are used with evolutionary synthesis models to verify the presence of a young stellar population in NGC 5018. The derived age of this population is about ~2.8 Gyr with a metallicity roughly solar and it completely dominates the integrated light of the galaxy near 4000 A.Comment: 13 pages, 7 figures (figs 3-7 are color figures), to be published in the May 2000 issue of the Astrophysical Journa

    V1647 Ori (IRAS 05436-0007) in Outburst: the First Three Months

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    We report on photometric (BVRIJHK) and low dispersion spectroscopic observations of V1647 Ori, the star that drives McNeil's Nebula, between 10 February and 7 May 2004. The star is photometrically variable atop a general decline in brightness of about 0.3-0.4 magnitudes during these 87 days. The spectra are featureless, aside from H-alpha and the Ca II infrared triplet in emission, and a Na I D absorption feature. The Ca II triplet line ratios are typical of young stellar objects. The H-alpha equivalent width may be modulated on a period of about 60 days. The post-outburst extinction appears to be less than 7 mag. The data are suggestive of an FU Orionis-like event, but further monitoring will be needed to definitively characterize the outburst.Comment: Accepted for publication in the Astronomical Journa
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