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Point source

About: Point source is a research topic. Over the lifetime, 5077 publications have been published within this topic receiving 94091 citations.


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Journal ArticleDOI
TL;DR: In this article, a general perturbation theory for small surface waveheights and for acoustic wavelengths of the order of the ocean surface correlation length is presented and formal solutions for the perturbed field are given and specialized, to the second order of approximation, for the case of a random ocean surface.
Abstract: A general perturbation theory is presented which is valid for small surface waveheights and for acoustic wavelengths of the order of the ocean‐surface correlation length. Formal solutions for the perturbed field are given and are specialized, to the second order of approximation, for the case of a random ocean surface. The scattering reduces the intensity of the carrier (source) signal and creates signal sidebands that are not in general symmetric in amplitude about the carrier. A pair of system functions for the signal sidebands is defined.Subject Classification: 30.40, 30.30, 30.25; 20.15.

24 citations

Journal ArticleDOI
TL;DR: In this article, the Rossi X-ray Timing Explorer (RXTE) has been used to detect a 38.5 ms Xray pulsar in observations of the soft γ-ray source IGR J18490-0000 with the Rossi x-ray timing Explorer.
Abstract: We report the discovery of a 38.5 ms X-ray pulsar in observations of the soft γ-ray source IGR J18490–0000 with the Rossi X-ray Timing Explorer (RXTE). PSR J1849–0001 is spinning down rapidly with period derivative 1.42 × 10–14 s s–1, yielding a spin-down luminosity 9.8 × 1036 erg s–1, characteristic age 42.9 kyr, and surface dipole magnetic field strength Bs = 7.5 × 1011 G. Within the INTEGRAL/IBIS error circle lies a point-like XMM-Newton and Chandra X-ray source that shows evidence of faint extended emission consistent with a pulsar wind nebula (PWN). The XMM-Newton spectrum of the point source is well fitted by an absorbed power-law model with photon index ΓPSR = 1.1 ± 0.2, N H = (4.3 ± 0.6) × 1022 cm–2, and F PSR(2-10 keV) = (3.8 ± 0.3) × 10–12 erg cm–2 s–1, while the spectral parameters of the extended emission are roughly ΓPWN ≈ 2.1 and F PWN(2-10 keV) ≈ 9 × 10–13 erg cm–2 s–1. IGR J18490–0000 is also coincident with the compact TeV source HESS J1849–000. For an assumed distance of 7 kpc in the Scutum arm tangent region, the 0.35-10 TeV luminosity of HESS J1849–000 is 0.13% of the pulsar's spin-down energy, while the ratio F(0.35-10 TeV)/F PWN(2-10 keV) ≈ 2. These properties are consistent with leptonic models of TeV emission from PWNe, with PSR J1849–0001 in a stage of transition from a synchrotron X-ray source to an inverse Compton γ-ray source.

24 citations

Journal ArticleDOI
TL;DR: In this paper, the authors developed a new inversion method, Image Deconvolution Back-Projection (IDBP), to retrieve high frequency energy radiation of seismic sources by linear inversion of observed images from a back-projection approach.

24 citations

Journal ArticleDOI
TL;DR: In this paper, it was shown that the rms temperature fluctuations of the thermal SZ effect could be underestimated by as much as 30% at an observing frequency of 30 GHz at l>1000.
Abstract: Radio point sources are strongly correlated with clusters of galaxies, so a significant fraction of the thermal Sunyaev-Zel'dovich (SZ) effect signal could be affected by point source contamination. Based on empirical estimates of the radio galaxy population, it is shown that the rms temperature fluctuations of the thermal SZ effect could be underestimated by as much as 30% at an observing frequency of 30 GHz at l>1000. The effect is larger at higher multipoles. If the recent report of excess power at small angular scales is to be explained by the thermal SZ effect, then radio point sources at an observing frequency of 30 GHz must be a surprisingly weak contaminant of the SZ effect for low-mass clusters.

24 citations

Journal ArticleDOI
TL;DR: In this paper, a theoretical simulation of automatic welding as a moving point source of heat with conduction as the dominant mode of transfer is refined to incorporate change of state across the melt boundary.

24 citations


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Performance
Metrics
No. of papers in the topic in previous years
YearPapers
202350
2022133
2021103
2020135
2019123
2018133