Probe diagnostics of anisotropic plasma in a hollow cathode arc
Measuring the second derivatives of electron retarded current characteristics of a plane probe at different angle positions, the coefficients f*i(ε) of the velocity distribution function developed as a Legendre polynomial are determined for the anisotropic plasma of a hollow cathode arc discharge. T...
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Veröffentlicht in: | Journal of applied physics 1991-07, Vol.70 (1), p.99-105 |
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description | Measuring the second derivatives of electron retarded current characteristics of a plane probe at different angle positions, the coefficients f*i(ε) of the velocity distribution function developed as a Legendre polynomial are determined for the anisotropic plasma of a hollow cathode arc discharge. The integral values deduced from this for the electron concentration ne and the mean electron energy ε̄, as well as the drift velocity vd, show only a limited dependence on the number of angle positions used for measurement. Even for measurements at a single angle position (Druyvesteyn method), the values obtained for ne, ε̄, and vd differ by less than 10% from the corresponding values measured with the multiposition method, so long as vdrift ≤ vthermal. On the contrary, the shape of f*i(ε), like the angle dependence f*(θ)ε=const, is clearly affected by the number of angle positions used. A Maxwell distribution superimposed by a group of directed fast electrons proves to be a sufficient model for the plasma investigated here. |
doi_str_mv | 10.1063/1.350223 |
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The integral values deduced from this for the electron concentration ne and the mean electron energy ε̄, as well as the drift velocity vd, show only a limited dependence on the number of angle positions used for measurement. Even for measurements at a single angle position (Druyvesteyn method), the values obtained for ne, ε̄, and vd differ by less than 10% from the corresponding values measured with the multiposition method, so long as vdrift ≤ vthermal. On the contrary, the shape of f*i(ε), like the angle dependence f*(θ)ε=const, is clearly affected by the number of angle positions used. A Maxwell distribution superimposed by a group of directed fast electrons proves to be a sufficient model for the plasma investigated here.</description><identifier>ISSN: 0021-8979</identifier><identifier>EISSN: 1089-7550</identifier><identifier>DOI: 10.1063/1.350223</identifier><identifier>CODEN: JAPIAU</identifier><language>eng</language><publisher>Woodbury, NY: American Institute of Physics</publisher><subject>Exact sciences and technology ; Physics ; Physics of gases, plasmas and electric discharges ; Physics of plasmas and electric discharges ; Plasma diagnostic techniques and instrumentation</subject><ispartof>Journal of applied physics, 1991-07, Vol.70 (1), p.99-105</ispartof><rights>1991 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c255t-1637ff8e9d63e1267d82ffe2826a407825b115902d86b5ea61236f09387b67d43</citedby><cites>FETCH-LOGICAL-c255t-1637ff8e9d63e1267d82ffe2826a407825b115902d86b5ea61236f09387b67d43</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=19845962$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>KLAGGE, S</creatorcontrib><creatorcontrib>LUNK, A</creatorcontrib><title>Probe diagnostics of anisotropic plasma in a hollow cathode arc</title><title>Journal of applied physics</title><description>Measuring the second derivatives of electron retarded current characteristics of a plane probe at different angle positions, the coefficients f*i(ε) of the velocity distribution function developed as a Legendre polynomial are determined for the anisotropic plasma of a hollow cathode arc discharge. The integral values deduced from this for the electron concentration ne and the mean electron energy ε̄, as well as the drift velocity vd, show only a limited dependence on the number of angle positions used for measurement. Even for measurements at a single angle position (Druyvesteyn method), the values obtained for ne, ε̄, and vd differ by less than 10% from the corresponding values measured with the multiposition method, so long as vdrift ≤ vthermal. On the contrary, the shape of f*i(ε), like the angle dependence f*(θ)ε=const, is clearly affected by the number of angle positions used. 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The integral values deduced from this for the electron concentration ne and the mean electron energy ε̄, as well as the drift velocity vd, show only a limited dependence on the number of angle positions used for measurement. Even for measurements at a single angle position (Druyvesteyn method), the values obtained for ne, ε̄, and vd differ by less than 10% from the corresponding values measured with the multiposition method, so long as vdrift ≤ vthermal. On the contrary, the shape of f*i(ε), like the angle dependence f*(θ)ε=const, is clearly affected by the number of angle positions used. A Maxwell distribution superimposed by a group of directed fast electrons proves to be a sufficient model for the plasma investigated here.</abstract><cop>Woodbury, NY</cop><pub>American Institute of Physics</pub><doi>10.1063/1.350223</doi><tpages>7</tpages></addata></record> |
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subjects | Exact sciences and technology Physics Physics of gases, plasmas and electric discharges Physics of plasmas and electric discharges Plasma diagnostic techniques and instrumentation |
title | Probe diagnostics of anisotropic plasma in a hollow cathode arc |
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