The plasma waveguide with a finite thickness of cladding
The properties of the plasma waveguide of finite thickness (plasma tube) have been studied. The analysis indicates that, in the case of finite thickness, most of the properties for the plasma waveguide with infinite thickness are retained. At high frequencies, such a plasma tube is still a nondisper...
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Veröffentlicht in: | Journal of applied physics 1991-12, Vol.70 (11), p.6653-6662 |
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creator | Shen, Hao-Ming Pao, Hsueh-Yuan |
description | The properties of the plasma waveguide of finite thickness (plasma tube) have been studied. The analysis indicates that, in the case of finite thickness, most of the properties for the plasma waveguide with infinite thickness are retained. At high frequencies, such a plasma tube is still a nondispersive waveguide system. The losses due to the finite thickness of the cladding and the conductivity of the plasma are both small. The decay coefficient decreases with the thickness exponentially. With a thickness equal to the radius of the central core, the attenuation can be as low as 0.1 dB/km. |
doi_str_mv | 10.1063/1.349837 |
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The analysis indicates that, in the case of finite thickness, most of the properties for the plasma waveguide with infinite thickness are retained. At high frequencies, such a plasma tube is still a nondispersive waveguide system. The losses due to the finite thickness of the cladding and the conductivity of the plasma are both small. The decay coefficient decreases with the thickness exponentially. 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The analysis indicates that, in the case of finite thickness, most of the properties for the plasma waveguide with infinite thickness are retained. At high frequencies, such a plasma tube is still a nondispersive waveguide system. The losses due to the finite thickness of the cladding and the conductivity of the plasma are both small. The decay coefficient decreases with the thickness exponentially. With a thickness equal to the radius of the central core, the attenuation can be as low as 0.1 dB/km.</description><subject>Exact sciences and technology</subject><subject>Physics</subject><subject>Physics of gases</subject><subject>Physics of gases, plasmas and electric discharges</subject><issn>0021-8979</issn><issn>1089-7550</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1991</creationdate><recordtype>article</recordtype><recordid>eNo9j0tLxDAURoMoOI6CPyELF2463tukTbKUwRcMuBnX5TaPabTTKU118N9bqbj6Nuc7cBi7RlghlOIOV0IaLdQJWyBok6migFO2AMgx00aZc3aR0jsAohZmwfS28bxvKe2JH-nL7z6j8_wYx4YTD7GLo-djE-1H51Pih8BtS87FbnfJzgK1yV_97ZK9PT5s18_Z5vXpZX2_ySyWZsxIIgQrdNAkC0FSu7wOSiCAqGtyFnIIQkKJptZ-MkuqpTJu-pbKBUNiyW5nrx0OKQ0-VP0Q9zR8VwjVb3GF1Vw8oTcz2lOy1IaBOhvTP1_IogRU4gebz1Qx</recordid><startdate>19911201</startdate><enddate>19911201</enddate><creator>Shen, Hao-Ming</creator><creator>Pao, Hsueh-Yuan</creator><general>American Institute of Physics</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>19911201</creationdate><title>The plasma waveguide with a finite thickness of cladding</title><author>Shen, Hao-Ming ; Pao, Hsueh-Yuan</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c169t-a410fc38f8a453a48d2bf731003bbadc020f340619b8eadd4ab479d16967df9a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1991</creationdate><topic>Exact sciences and technology</topic><topic>Physics</topic><topic>Physics of gases</topic><topic>Physics of gases, plasmas and electric discharges</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Shen, Hao-Ming</creatorcontrib><creatorcontrib>Pao, Hsueh-Yuan</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>Journal of applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Shen, Hao-Ming</au><au>Pao, Hsueh-Yuan</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The plasma waveguide with a finite thickness of cladding</atitle><jtitle>Journal of applied physics</jtitle><date>1991-12-01</date><risdate>1991</risdate><volume>70</volume><issue>11</issue><spage>6653</spage><epage>6662</epage><pages>6653-6662</pages><issn>0021-8979</issn><eissn>1089-7550</eissn><coden>JAPIAU</coden><abstract>The properties of the plasma waveguide of finite thickness (plasma tube) have been studied. The analysis indicates that, in the case of finite thickness, most of the properties for the plasma waveguide with infinite thickness are retained. At high frequencies, such a plasma tube is still a nondispersive waveguide system. The losses due to the finite thickness of the cladding and the conductivity of the plasma are both small. The decay coefficient decreases with the thickness exponentially. With a thickness equal to the radius of the central core, the attenuation can be as low as 0.1 dB/km.</abstract><cop>Woodbury, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.349837</doi><tpages>10</tpages></addata></record> |
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subjects | Exact sciences and technology Physics Physics of gases Physics of gases, plasmas and electric discharges |
title | The plasma waveguide with a finite thickness of cladding |
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