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dc.contributor.authorLewkowicz, M.en_US
dc.contributor.authorKao, H. C.en_US
dc.contributor.authorRosenstein, B.en_US
dc.date.accessioned2019-04-03T06:36:05Z-
dc.date.available2019-04-03T06:36:05Z-
dc.date.issued2011-07-20en_US
dc.identifier.issn1098-0121en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.84.035414en_US
dc.identifier.urihttp://hdl.handle.net/11536/21515-
dc.description.abstractElectron-hole pairs are copiously created by an applied electric field near the Dirac point in graphene or similar two-dimensional electronic systems. It was shown recently that for sufficiently large electric fields E and ballistic times the I-V characteristics become strongly nonlinear due to Schwinger's pair creation rate, proportional to E(3/2). Since there is no energy gap the radiation from the pairs' annihilation is enhanced. The spectrum of radiation is calculated and exhibits a maximum at omega = root eEv(g)/h. The angular and polarization dependence of the emitted photons with respect to the graphene sheet is quite distinctive. For very large currents the recombination rate becomes so large that it leads to the second Ohmic regime due to radiation friction.en_US
dc.language.isoen_USen_US
dc.titleSignature of the Schwinger pair creation rate via radiation generated in graphene by a strong electric currenten_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.84.035414en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume84en_US
dc.citation.issue3en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000292924800017en_US
dc.citation.woscount12en_US
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