PARAMETER DEPENDENCE OF ACOUSTOELECTRIC AMPLIFICATION IN InSb
dc.contributor.author | Fleming, W. J. | en_US |
dc.contributor.author | Rowe, J. E. (Joseph Everett) | en_US |
dc.date.accessioned | 2010-05-06T22:33:00Z | |
dc.date.available | 2010-05-06T22:33:00Z | |
dc.date.issued | 1971-02-01 | en_US |
dc.identifier.citation | Fleming, W. J.; Rowe, J. E. (1971). "PARAMETER DEPENDENCE OF ACOUSTOELECTRIC AMPLIFICATION IN InSb." Applied Physics Letters 18(3): 96-99. <http://hdl.handle.net/2027.42/70684> | en_US |
dc.identifier.uri | https://hdl.handle.net/2027.42/70684 | |
dc.description.abstract | On the basis of a hydrodynamical theory of the acoustoelectric interaction (Fleming-Rowe) reported earlier which included electron inertial terms it is found that for sufficiently large electron drift velocities sharp high-gain peaks occur. Furthermore the peak values of gain achieved greatly exceed the maximum gain of the corresponding theory of Steele. Excellent agreement with recently reported experimental measurements of microwave acoustic gain in InSb is obtained. It is also noted that for large applied fields, empirical field factors are required to give agreement with experiment. | en_US |
dc.format.extent | 3102 bytes | |
dc.format.extent | 288155 bytes | |
dc.format.mimetype | text/plain | |
dc.format.mimetype | application/pdf | |
dc.publisher | The American Institute of Physics | en_US |
dc.rights | © The American Institute of Physics | en_US |
dc.title | PARAMETER DEPENDENCE OF ACOUSTOELECTRIC AMPLIFICATION IN InSb | en_US |
dc.type | Article | en_US |
dc.subject.hlbsecondlevel | Physics | en_US |
dc.subject.hlbtoplevel | Science | en_US |
dc.description.peerreviewed | Peer Reviewed | en_US |
dc.contributor.affiliationum | Electrom Physics Laboratory, Department of Electrical Engineering, University of Michigan, Ann Arbor, Michigan 48104 | en_US |
dc.description.bitstreamurl | http://deepblue.lib.umich.edu/bitstream/2027.42/70684/2/APPLAB-18-3-96-1.pdf | |
dc.identifier.doi | 10.1063/1.1653579 | en_US |
dc.identifier.source | Applied Physics Letters | en_US |
dc.identifier.citedreference | R. K. Route and G. S. Kino, IBM J. Res. Develop. 13, 507 (1969). | en_US |
dc.identifier.citedreference | K. P. Weller and T. Van Duzer, J. Appl. Phys. 40, 4278 (1969). | en_US |
dc.identifier.citedreference | W. Harth and R. Jaenicke, Appl. Phys. Letters 14, 27 (1969). | en_US |
dc.identifier.citedreference | W. J. Fleming and J. E. Rowe, J. Appl. Phys. (to be published). | en_US |
dc.identifier.citedreference | H. Hayakawa and M. Kikuchi, Appl. Phys. Letters 17, 73 (1970). | en_US |
dc.identifier.citedreference | M. C. Steele, RCA Rev. 28, 58 (1967). | en_US |
dc.identifier.citedreference | G. S. Kino and R. Route, Appl. Phys. Letters 11, 312 (1967). | en_US |
dc.identifier.citedreference | D. L. White, J. Appl. Phys. 33, 2547 (1962). | en_US |
dc.identifier.citedreference | Y. Abe and N. Mikoshiba, Appl. Phys. Letters 13, 241 (1968). | en_US |
dc.identifier.citedreference | L. Spitzer, Jr., Physics of Fully Ionized Gases (Interscience, New York, 1956). | en_US |
dc.identifier.citedreference | It can be shown that the factor ω/ωD = qD/υsω/ωD=qD/υs of the present theory (contained in the definition of ω/ω′Dω/ω′D) and the theory of Kino and Route (Ref. 7) is modified and becomes ω/ωD = qD/υs+ωυu0/υsω/ωD=qD/υs+ωυu0/υs in the theory of Abe and Mikoshiba (Ref. 9). The additional term ωυu0/υsωυu0/υs appearing in the theory of Abe and Mikoshiba is erroneous and comes directly from the specialized magnetohydrodynamic expression [Eq. (1) of Ref. 9] which they use for the equation of momentum conservation. | en_US |
dc.identifier.citedreference | The contribution of the quartic term in (4) is negligible for all but the largest values of applied current. For example, the value of the quartic term just exceeds 1% of the value of the quadratic term for u0 = υT(J0 = 480 A/cm2).u0=υT(J0=480A/cm2). | en_US |
dc.identifier.citedreference | E. V. George and G. Bekefi, Appl. Phys. Letters 15, 33 (1969). | en_US |
dc.identifier.citedreference | H. J. Lippman and F. Kuhrt, Z. Naturforsch. 13a, 462 (1958). | en_US |
dc.identifier.citedreference | Taking I0 = J0w2I0=J0w2 and V0 = E0L,V0=E0L, I–V characteristics calculated from (6) are a good approximation to the actual measured I–V characteristics. | en_US |
dc.owningcollname | Physics, Department of |
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