6,320 research outputs found

    Evaluation of pressure and thermal data from a wind tunnel test of a large-scale, powered, STOL fighter model

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    A STOL fighter model employing the vectored-engine-over wing concept was tested at low speeds in the NASA/Ames 40 by 80-foot wind tunnel. The model, approximately 0.75 scale of an operational fighter, was powered by two General Electric J-97 turbojet engines. Limited pressure and thermal instrumentation were provided to measure power effects (chordwise and spanwise blowing) and control-surface-deflection effects. An indepth study of the pressure and temperature data revealed many flow field features - the foremost being wing and canard leading-edge vortices. These vortices delineated regions of attached and separated flow, and their movements were often keys to an understanding of flow field changes caused by power and control-surface variations. Chordwise blowing increased wing lift and caused a modest aft shift in the center of pressure. The induced effects of chordwise blowing extended forward to the canard and significantly increased the canard lift when the surface was stalled. Spanwise blowing effectively enhanced the wing leading-edge vortex, thereby increasing lift and causing a forward shift in the center of pressure

    Analytic Solution for the Ground State Energy of the Extensive Many-Body Problem

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    A closed form expression for the ground state energy density of the general extensive many-body problem is given in terms of the Lanczos tri-diagonal form of the Hamiltonian. Given the general expressions of the diagonal and off-diagonal elements of the Hamiltonian Lanczos matrix, αn(N)\alpha_n(N) and βn(N)\beta_n(N), asymptotic forms α(z)\alpha(z) and β(z)\beta(z) can be defined in terms of a new parameter z≡n/Nz\equiv n/N (nn is the Lanczos iteration and NN is the size of the system). By application of theorems on the zeros of orthogonal polynomials we find the ground-state energy density in the bulk limit to be given in general by E0=inf [α(z)−2 β(z)]{\cal E}_0 = {\rm inf}\,\left[\alpha(z) - 2\,\beta(z)\right].Comment: 10 pages REVTex3.0, 3 PS figure

    Spectrally resolved single-shot wavefront sensing of broadband high-harmonic sources

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    Wavefront sensors are an important tool to characterize coherent beams of extreme ultraviolet radiation. However, conventional Hartmann-type sensors do not allow for independent wavefront characterization of different spectral components that may be present in a beam, which limits their applicability for intrinsically broadband high-harmonic generation (HHG) sources. Here we introduce a wavefront sensor that measures the wavefronts of all the harmonics in a HHG beam in a single camera exposure. By replacing the mask apertures with transmission gratings at different orientations, we simultaneously detect harmonic wavefronts and spectra, and obtain sensitivity to spatiotemporal structure such as pulse front tilt as well. We demonstrate the capabilities of the sensor through a parallel measurement of the wavefronts of 9 harmonics in a wavelength range between 25 and 49 nm, with up to lambda/32 precision.Comment: 12 pages, 6 figure

    Boundary conditions associated with the Painlev\'e III' and V evaluations of some random matrix averages

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    In a previous work a random matrix average for the Laguerre unitary ensemble, generalising the generating function for the probability that an interval (0,s) (0,s) at the hard edge contains k k eigenvalues, was evaluated in terms of a Painlev\'e V transcendent in σ \sigma -form. However the boundary conditions for the corresponding differential equation were not specified for the full parameter space. Here this task is accomplished in general, and the obtained functional form is compared against the most general small s s behaviour of the Painlev\'e V equation in σ \sigma -form known from the work of Jimbo. An analogous study is carried out for the the hard edge scaling limit of the random matrix average, which we have previously evaluated in terms of a Painlev\'e \IIId transcendent in σ \sigma -form. An application of the latter result is given to the rapid evaluation of a Hankel determinant appearing in a recent work of Conrey, Rubinstein and Snaith relating to the derivative of the Riemann zeta function

    X-ray Halos and Large Grains in the Diffuse Interstellar Medium

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    Recent observations with dust detectors on board the interplanetary spacecraft Ulysses and Galileo have recorded a substantial flux of large interstellar grains with radii between 0.25 and 2.0 mu entering the solar system from the local interstellar cloud. The most commonly used interstellar grain size distribution is characterized by a a^-3.5 power law in grain radii a, and extends to a maximum grain radius of 0.25 mu. The extension of the interstellar grain size distribution to such large radii will have a major effect on the median grain size, and on the amount of mass needed to be tied up in dust for a given visual optical depth. It is therefore important to investigate whether this population of larger dust particles prevails in the general interstellar medium, or if it is merely a local phenomenon. The presence of large interstellar grains can be mainly inferred from their effect on the intensity and radial profiles of scattering halos around X-ray sources. In this paper we examine the grain size distribution that gives rise to the X-ray halo around Nova Cygni 1992. The results of our study confirm the need to extend the interstellar grain size distribution in the direction of this source to and possibly beyond 2.0 mu. The model that gives the best fit to the halo data is characterized by: (1) a grain size distribution that follows an a^-3.5 power law up to 0.50 mu, followed by an a^-4.0 extension from 0.50 mu to 2.0 mu; and (2) silicate and graphite (carbon) dust-to-gas mass ratios of 0.0044 and 0.0022, respectively, consistent with solar abundances constraints. Additional observations of X-ray halos probing other spatial directions are badly needed to test the general validity of this result.Comment: 17 pages, incl. 1 figure, accepted for publ. by ApJ Letter

    {\bf Ï„\tau-Function Evaluation of Gap Probabilities in Orthogonal and Symplectic Matrix Ensembles}

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    It has recently been emphasized that all known exact evaluations of gap probabilities for classical unitary matrix ensembles are in fact Ï„\tau-functions for certain Painlev\'e systems. We show that all exact evaluations of gap probabilities for classical orthogonal matrix ensembles, either known or derivable from the existing literature, are likewise Ï„\tau-functions for certain Painlev\'e systems. In the case of symplectic matrix ensembles all exact evaluations, either known or derivable from the existing literature, are identified as the mean of two Ï„\tau-functions, both of which correspond to Hamiltonians satisfying the same differential equation, differing only in the boundary condition. Furthermore the product of these two Ï„\tau-functions gives the gap probability in the corresponding unitary symmetry case, while one of those Ï„\tau-functions is the gap probability in the corresponding orthogonal symmetry case.Comment: AMS-Late

    Ion distribution and ablation depth measurements of a fs-ps laser-irradiated solid tin target

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    The ablation of solid tin surfaces by an 800-nanometer-wavelength laser is studied for a pulse length range from 500 fs to 4.5 ps and a fluence range spanning 0.9 to 22 J/cm^2. The ablation depth and volume are obtained employing a high-numerical-aperture optical microscope, while the ion yield and energy distributions are obtained from a set of Faraday cups set up under various angles. We found a slight increase of the ion yield for an increasing pulse length, while the ablation depth is slightly decreasing. The ablation volume remained constant as a function of pulse length. The ablation depth follows a two-region logarithmic dependence on the fluence, in agreement with the available literature and theory. In the examined fluence range, the ion yield angular distribution is sharply peaked along the target normal at low fluences but rapidly broadens with increasing fluence. The total ionization fraction increases monotonically with fluence to a 5-6% maximum, which is substantially lower than the typical ionization fractions obtained with nanosecond-pulse ablation. The angular distribution of the ions does not depend on the laser pulse length within the measurement uncertainty. These results are of particular interest for the possible utilization of fs-ps laser systems in plasma sources of extreme ultraviolet light for nanolithography.Comment: 8 pages, 7 figure

    Pensioen wijzigen jegens slapers en pensioengerechtigden

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    Naar aanleiding van de eerdere publicatie van auteurs inzake 'Wijzigingsvraagstukken in de pensioendriehoek'(TPV 2012/42), is een reactie verschenen van Breuker. In dit artikel wordt gereageer op het artikel van Breuker en verduidelijken auteurs hun standpunt over de juridische (on)houdbaarheid van (1) de uitewerkte rechtsverhouding en (2) pensioenwijzigingen jegens slapers en pensioengerechtigden. De conclusie luidt dat wijziging van opgebouwd pensioen jegens slapers en pensioengerechtigden - inclusief onvoorwaardelijke indexatie - moeilijk is maar wel mogelijk. Een dergelijke wijziging geschiedt onder de Pensioenwet binnen de marges van de wet: via waardeoverdracht of korten. Het door de wetgever gestimuleerde invaren is daar een voorbeeld van. Onder de (voormalige) Pensioen- en Spaarfondsenwet ligt dit anders volgens auteurs. Er gold geen wettelijke beperking ten aanzien van het voorwaardelijk maken van onvoorwaardelijke indexatie. Het pad om de wijzigingen rechtsgeldig door te voeren jegens slapers en pensioengerechtigden is nog steeds hobbelig en onzeker
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