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DIRECT OBSERVATION OF SI DELTA-DOPED GAAS BY TRANSMISSION ELECTRON-MICROSCOPY

dc.citation.epage2630en_US
dc.citation.issue21en_US
dc.citation.spage2628en_US
dc.citation.volume60en_US
dc.citation.woscount14
dc.contributor.authorLIU, DGen_US
dc.contributor.authorFAN, JCen_US
dc.contributor.authorLEE, CPen_US
dc.contributor.authorTSAI, CMen_US
dc.contributor.authorCHANG, KHen_US
dc.contributor.authorLIOU, DCen_US
dc.contributor.authorLEE, TLen_US
dc.contributor.authorCHEN, LJen_US
dc.contributor.department電控工程研究所zh_TW
dc.contributor.departmentInstitute of Electrical and Control Engineeringen_US
dc.date.accessioned2014-12-08T15:04:54Z
dc.date.available2014-12-08T15:04:54Z
dc.date.issued1992-05-25en_US
dc.description.abstractDirect observation of the Si delta-doped layer in GaAs has been achieved by high resolution transmission electron microscopy. Samples with different Si doses, from half a monolayer to two monolayers, were studied. The observed spreading of the delta-doped layer showed that Si atoms are largely confined in five monolayers at most (in the highest dose case), indicating excellent confinements of dopants in GaAs. From the images, the Si atoms were uniformly distributed in the doped layer, no cluster formation was observed. For delta-doped GaAs grown at low temperature (480-degrees-C), stacking faults originated from the doped layers were observed. These faults were thought to be caused by the large unrelaxed strain in the low-temperature grown GaAs.en_US
dc.identifier.doi10.1063/1.106902en_US
dc.identifier.issn0003-6951en_US
dc.identifier.journalAPPLIED PHYSICS LETTERSen_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.106902en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/3415
dc.identifier.wosnumberWOS:A1992HV49100018
dc.language.isoen_USen_US
dc.titleDIRECT OBSERVATION OF SI DELTA-DOPED GAAS BY TRANSMISSION ELECTRON-MICROSCOPYen_US
dc.typeArticleen_US

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