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Metastable Atom Probe for Measurement of Electron Beam Density Profiles

dc.contributor.authorLockhart, James M.en_US
dc.contributor.authorZorn, Jens C.en_US
dc.date.accessioned2010-05-06T21:34:35Z
dc.date.available2010-05-06T21:34:35Z
dc.date.issued1971-03en_US
dc.identifier.citationLockhart, James M.; Zorn, Jens C. (1971). "Metastable Atom Probe for Measurement of Electron Beam Density Profiles." Review of Scientific Instruments 42(3): 315-318. <http://hdl.handle.net/2027.42/70063>en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/70063
dc.description.abstractA well collimated thermal beam of argon atoms, moving in the z direction, crosses the electron beam that is to be studied. Those argon atoms that are excited by impact to a metastable state proceed, with very little change in speed or direction, to a detector (windowless electron multiplier) some distance away. The neutral atomic beam of the metastable atom probe (MAP) has a negligible interaction with the electromagnetic fields that govern the behavior of the electron beam; moreover, almost no additional space charge is created when the atomic beam is introduced. Thus, if the cross section of the atomic argon beam is small compared to the characteristic dimensions of the electrode structure that defines the electron beam, the metastable atom count rate, monitored as a function of x and y, gives a virtually nonperturbative measurement of the density profile of the electron beam. In this paper we outline the principles and applications of the method, discuss details of its implementation, and give results obtained with an MAP that has a spatial resolution of better than 0.5 mm.en_US
dc.format.extent3102 bytes
dc.format.extent340231 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.titleMetastable Atom Probe for Measurement of Electron Beam Density Profilesen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumRandall Laboratory of Physics, The University of Michigan, Ann Arbor, Michigan 48104en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/70063/2/RSINAK-42-3-315-1.pdf
dc.identifier.doi10.1063/1.1685083en_US
dc.identifier.sourceReview of Scientific Instrumentsen_US
dc.identifier.citedreferenceJ. R. Pierce, Theory and Design of Electron Beams (Van Nostrand, New York and Princeton, 1949), pp. 54 ff.en_US
dc.identifier.citedreferenceB. Paszkowski, Electron Optics (Elsevier, New York, 1968); H. Moss, Narrow Angle Electron Guns and Cathode Ray Tubes (Academic, New York, 1968).en_US
dc.identifier.citedreferenceA preliminary report of this work has been given by J. M. Lockhart, R. Pichlik and J. C. Zorn, Bull. Amer Phys. Soc. 15, 558 (1970).en_US
dc.identifier.citedreferenceJ. C. Pearl, D. P. Donnelly, and J. C. Zorn, Phys. Lett. 30A, 145 (1969).en_US
dc.identifier.citedreferenceJ. W. Locke and J. B. French, J. Vac. Sci. Technol. 7, 46 (1970).en_US
dc.identifier.citedreferenceJ. Olmsted, A. S. Newton, and K. Street, J. Chem. Phys. 42, 2321 (1965).en_US
dc.identifier.citedreferenceD. P. Donnelly, J. C. Pearl, R. A. Heppner, and J. C. Zorn, Rev. Sci. Instrum. 40, 1242 (1969).en_US
dc.identifier.citedreferenceJ. T. Dickinson, J. M. Lockhart, and J. C. Zorn, Amer. J. Phys. 39, (1971).en_US
dc.identifier.citedreferenceA display ot this kind has been used to show the density profiles of a neutral gas jet by R. L. Hickock, J. F. Marshall, and F. C. Jobes, Rev. Sci. Instrum. 40, 471 (1970).en_US
dc.owningcollnamePhysics, Department of


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