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Multipactor discharge on metals and dielectrics: Historical review and recent theories

dc.contributor.authorKishek, R. A.en_US
dc.contributor.authorLau, Y. Y.en_US
dc.contributor.authorAng, L. K.en_US
dc.contributor.authorValfells, Agusten_US
dc.contributor.authorGilgenbach, Ronald M.en_US
dc.date.accessioned2010-05-06T23:04:41Z
dc.date.available2010-05-06T23:04:41Z
dc.date.issued1998-05en_US
dc.identifier.citationKishek, R. A.; Lau, Y. Y.; Ang, L. K.; Valfells, A.; Gilgenbach, R. M. (1998). "Multipactor discharge on metals and dielectrics: Historical review and recent theories." Physics of Plasmas 5(5): 2120-2126. <http://hdl.handle.net/2027.42/71019>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/71019
dc.description.abstractThis paper reviews the history of multipactor discharge theory, focusing on recent models of multipactor accessibility and saturation. Two cases are treated in detail: That of a first-order, two-surface multipactor, and that of a single-surface multipactor on a dielectric. In both cases, susceptibility curves are constructed to indicate the regions of external parameter space where multipactor is likely to occur, taking into account the dependence on surface materials, and the effects of space charge and cavity loading. In the case of a dielectric, multipactor is found to deliver about 1% of the rf power to the surface. The two cases are contrasted in light of experimental observations. © 1998 American Institute of Physics.en_US
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dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleMultipactor discharge on metals and dielectrics: Historical review and recent theoriesen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Nuclear Engineering and Radiological Sciences, University of Michigan, Ann Arbor, Michigan 48109-2104en_US
dc.contributor.affiliationotherInstitute for Plasma Research, ERB#223, University of Maryland, College Park, Maryland 20742en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/71019/2/PHPAEN-5-5-2120-1.pdf
dc.identifier.doi10.1063/1.872883en_US
dc.identifier.sourcePhysics of Plasmasen_US
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dc.identifier.citedreferenceWe remark that Eq. (1a) is not exact for nonzero initial velocity, because in such a case the maximum stable phase θmθm is no longer given by the simple expression arctan (2/Nπ)arctan(2/Nπ) derived for zero emission velocity, but is nevertheless sufficiently accurate.en_US
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dc.owningcollnamePhysics, Department of


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