Papers published on a yearly basis
Papers
More filters
••
TL;DR: The performance of this OPO shows that large-aperture PP RTA crystals are well suited for pulsed nanosecond OPO operation with pump pulse energies of tens of millijoules.
Abstract: We report on optical parametric oscillators (OPO's) based on periodically poled RbTiOAsO4 (PP RTA), which are pumped by Q-switched solid-state lasers. With a diode-pumped Nd:YVO4 laser (pulse energy, 800 ?J; pulse duration, 5.5??ns; repetition rate, 1??kHz) the PP RTA OPO generated 1.58??m signal and 3.26??m idler radiation with a signal pulse energy of 45 ?J. The large aperture of 3 mm×3 mm of the PP RTA crystal also permitted OPO operation with pump pulse energies as high as 65??mJ, provided by a flash-lamp-pumped Q-switched Nd:YAG laser (pulse duration, 20??ns; repetition rate, 10??Hz). With this pump source the OPO generated signal pulse energies as high as 17??mJ, corresponding to an efficiency of 26%. The performance of this OPO shows that large-aperture PP RTA crystals are well suited for pulsed nanosecond OPO operation with pump pulse energies of tens of millijoules.
39 citations
••
TL;DR: In this article, it was shown that if the RCS is measured as a function of an angle and is low-pass filtered with a cut off period of \phi c (radians), the distance requirement could be changed to R > 4D\phi^{-1}_{c}(1 - \lambda/2\phi c}D).
Abstract: Radar cross sections (RCS) must be measured at large distance. We exclude here the special near-field methods. The distance (R) must be so large that different RCS contributions are added in the same way as at infinite distance. This leads to the rule R > 2D^{2}/\lambda if the target cross range is confined within \pm D/2 and a phase error of \pi /4 is tolerated. It is shown, however, that if the RCS is measured as a function of an angle and is low-pass filtered with a cut off period of \phi_{c} (radians), the distance requirement could be changed to R > 4D\phi^{-1}_{c}(1 - \lambda/2\phi_{c}D)) . All RCS measurements at such distances give approximately the same result after low-pass filtering. We assume that a set of isotropic point scatterers, accurately describes the target.
39 citations
••
TL;DR: A model of specification management that identifies important steps from the conceiving of the idea to delivery and customer feedback is developed and it is concluded that following the steps proposed in the model could lead to a high quality product.
39 citations
••
TL;DR: In this paper, the dynamic fracture of an adhesive layer in a structure is analyzed and three constitutive models of the adhesive layer are used to compare the results of explicit FE-analyses with the closed form solutions.
39 citations
••
24 Jul 2000TL;DR: The theory of noise modulated radar is treated, point target response, side-lobe level, and time compression due to motion effects are analysed, and degrading effects from additive noise are analysed.
Abstract: Presently, there is an increasing interest in noise modulated radar in a wide spectrum of applications, such as surveillance, tracking, altimetry, and sub-surface profiling. Wide-band signals with high range resolution, reduced ambiguities and high ECCM performance can be achieved. In this paper, the theory of noise modulated radar is treated. Point target response, side-lobe level, and time compression due to motion effects are analysed. The processing involved correlates the received signal and the delayed reference signal. An alternative method correlates only their signs, making it possible to reduce the requirements on the analog-to-digital converters to one bit. Both approaches are studied and degrading effects from additive noise are analysed.
39 citations
Authors
Showing all 760 results
Name | H-index | Papers | Citations |
---|---|---|---|
Christer Larsson | 64 | 272 | 12916 |
Björn Johansson | 62 | 637 | 16030 |
David C. Viano | 48 | 232 | 8283 |
Thomas Schiex | 47 | 138 | 11031 |
Robin Hanson | 28 | 114 | 3519 |
Per Lötstedt | 28 | 109 | 2960 |
Brigitte Mangin | 26 | 48 | 2652 |
Lars Hanson | 19 | 117 | 1138 |
Carl Gustafson | 17 | 34 | 1035 |
Magnus Carlsson | 16 | 37 | 808 |
Per-Johan Nordlund | 14 | 26 | 2738 |
David Allouche | 14 | 26 | 680 |
Mark A. Saab | 13 | 16 | 1153 |
Andreas Gällström | 13 | 34 | 402 |
Hans Hellsten | 12 | 37 | 549 |