Sources of localized waves

The synthesis of two types of Localized Wave (L W) pulses is considered; these are the 'Focus Wave Model (FWM) pulse and the X Wave pulse. First, we introduce the modified bidirectional representation where one can select new basis functions resulting in different representations for a solut...

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Main Author: Chatzipetros, Argyrios Alexandros
Other Authors: Electrical Engineering
Format: Others
Language:en
Published: Virginia Tech 2014
Subjects:
Online Access:http://hdl.handle.net/10919/38460
http://scholar.lib.vt.edu/theses/available/etd-06062008-171252/
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spelling ndltd-VTETD-oai-vtechworks.lib.vt.edu-10919-384602021-04-24T05:40:12Z Sources of localized waves Chatzipetros, Argyrios Alexandros Electrical Engineering Besieris, Ioannis M. Brown, Gary S. de Wolf, David A. Stutzman, Warren L. Kohler, Werner E. LD5655.V856 1994.C438 Electromagnetic waves The synthesis of two types of Localized Wave (L W) pulses is considered; these are the 'Focus Wave Model (FWM) pulse and the X Wave pulse. First, we introduce the modified bidirectional representation where one can select new basis functions resulting in different representations for a solution to the scalar wave equation. Through this new representation, we find a new class of focused X Waves which can be extremely localized. The modified bidirectional decomposition is applied to the nonhomogeneous scalar wave equation, resulting in moving sources generating L W pulses. In this work, we also address the possibility of exciting L W pulses from dynamic apertures, or apertures the effective radius of which is varied with time. Ideal L W pulses cannot be realized because they require infinite time excitation. However, in the case of finite L W pulses, the aperture of excitation is finite and is varied from a time - T to T. We show that the resulting L W pulses are more resistant to decay than classical monochromatic Gaussian pulses occupying the same beam waist. Both types of finite L W pulses, such as the FWM and X Wave pulse, can propagate without significant decay to much greater distances than classical monochromatic pulses. This desirable behavior is attributed to the superior aperture efficiency of the L W pulses, which in turn is attributed to their unique spectral structure. Ph. D. 2014-03-14T21:14:28Z 2014-03-14T21:14:28Z 1994-09-06 2008-06-06 2008-06-06 2008-06-06 Dissertation Text etd-06062008-171252 http://hdl.handle.net/10919/38460 http://scholar.lib.vt.edu/theses/available/etd-06062008-171252/ en OCLC# 32749858 LD5655.V856_1994.C438.pdf In Copyright http://rightsstatements.org/vocab/InC/1.0/ ix, 116 leaves BTD application/pdf application/pdf Virginia Tech
collection NDLTD
language en
format Others
sources NDLTD
topic LD5655.V856 1994.C438
Electromagnetic waves
spellingShingle LD5655.V856 1994.C438
Electromagnetic waves
Chatzipetros, Argyrios Alexandros
Sources of localized waves
description The synthesis of two types of Localized Wave (L W) pulses is considered; these are the 'Focus Wave Model (FWM) pulse and the X Wave pulse. First, we introduce the modified bidirectional representation where one can select new basis functions resulting in different representations for a solution to the scalar wave equation. Through this new representation, we find a new class of focused X Waves which can be extremely localized. The modified bidirectional decomposition is applied to the nonhomogeneous scalar wave equation, resulting in moving sources generating L W pulses. In this work, we also address the possibility of exciting L W pulses from dynamic apertures, or apertures the effective radius of which is varied with time. Ideal L W pulses cannot be realized because they require infinite time excitation. However, in the case of finite L W pulses, the aperture of excitation is finite and is varied from a time - T to T. We show that the resulting L W pulses are more resistant to decay than classical monochromatic Gaussian pulses occupying the same beam waist. Both types of finite L W pulses, such as the FWM and X Wave pulse, can propagate without significant decay to much greater distances than classical monochromatic pulses. This desirable behavior is attributed to the superior aperture efficiency of the L W pulses, which in turn is attributed to their unique spectral structure. === Ph. D.
author2 Electrical Engineering
author_facet Electrical Engineering
Chatzipetros, Argyrios Alexandros
author Chatzipetros, Argyrios Alexandros
author_sort Chatzipetros, Argyrios Alexandros
title Sources of localized waves
title_short Sources of localized waves
title_full Sources of localized waves
title_fullStr Sources of localized waves
title_full_unstemmed Sources of localized waves
title_sort sources of localized waves
publisher Virginia Tech
publishDate 2014
url http://hdl.handle.net/10919/38460
http://scholar.lib.vt.edu/theses/available/etd-06062008-171252/
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