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Characterization of an ultradense reproducible Z pinch

dc.contributor.authorDusto, D.en_US
dc.contributor.authorRockett, F. P. D.en_US
dc.contributor.authorStee, D. G.en_US
dc.contributor.authorAckenhusen, John G.en_US
dc.contributor.authorBach, Bach, David Rudolphen_US
dc.contributor.authorDuderstadt, James J.en_US
dc.date.accessioned2010-05-06T21:39:30Z
dc.date.available2010-05-06T21:39:30Z
dc.date.issued1977-12-15en_US
dc.identifier.citationDusto, D.; Rockett, F P. D.; Stee, D. G.; Ackenhusen, F J. G.; Bach, D. R.; Duderstadt, J. J. (1977). "Characterization of an ultradense reproducible Z pinch." Applied Physics Letters 31(12): 801-803. <http://hdl.handle.net/2027.42/70116>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70116
dc.description.abstractThe apparent complexity of the laser‐plasma coupling in laser fusion target irradiation has stimulated the need for carefully controlled experimental studies of the laser‐plasma interaction at the critical surface. A helium Z pinch has been constructed which produces a high density plasma, independent of the laser, enabling the separation of the laser‐plasma interaction physics from the plasma formation mechanism. Its peak electron density (4×1019 cm−3), critical density scale length (70–200 μ), and temperature (∼25 eV) make it suitable for simulating and studying laser‐pellet interaction mechanisms at CO2 laser wavelengths. Detailed numerical modelling of these experiments was employed as a check against our diagnostics, as well as providing physical insight in those ranges of experimental parameters where measurements were not made.en_US
dc.format.extent3102 bytes
dc.format.extent233108 bytes
dc.format.mimetypetext/plain
dc.format.mimetypeapplication/pdf
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleCharacterization of an ultradense reproducible Z pinchen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumThe University of Michigan, Ann Arbor, Michigan 48109en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70116/2/APPLAB-31-12-801-1.pdf
dc.identifier.doi10.1063/1.89555en_US
dc.identifier.sourceApplied Physics Lettersen_US
dc.identifier.citedreferenceD. W. Forslund, Bull. Am. Phys. Soc. 21, 1066 (1976).en_US
dc.identifier.citedreferenceP. D. Rockett, D. G. Steel, J. G. Ackenhusen, and D. R. Bach, Phys. Rev. Lett. (to be published).en_US
dc.identifier.citedreferenceD. G. Steel, P. D. Rockett, D. R. Bach, and P. L. Colestock, Rev. Sci. Instrum. (to be published).en_US
dc.identifier.citedreferenceH. Zwicker and U. Schumacher, Z. Phys. 183, 435 (1955).en_US
dc.identifier.citedreferenceY. Hashino, H. Suemitsu, and K. Fukuda, Jpn. J. Appl. Phys. 11, 710 (1972).en_US
dc.identifier.citedreferenceM. A. Uman, Introduction to Plasma Physics (McGraw‐Hill, New York, 1964).en_US
dc.identifier.citedreferenceD. Duston and J. J. Duderstadt, J. Appl. Phys. (to be published).en_US
dc.owningcollnamePhysics, Department of


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