完整後設資料紀錄
DC 欄位語言
dc.contributor.author張俊彥en_US
dc.contributor.authorZhang, Zun-Yanen_US
dc.contributor.author施敏en_US
dc.contributor.authorShi, Minen_US
dc.date.accessioned2014-12-12T02:01:08Z-
dc.date.available2014-12-12T02:01:08Z-
dc.date.issued1970en_US
dc.identifier.urihttp://140.113.39.130/cdrfb3/record/nctu/#NT594428001en_US
dc.identifier.urihttp://hdl.handle.net/11536/51028-
dc.description.abstract金屬半導體介面之研究 張俊彥 ABSTRACT /////// Carrier transport in metal-semiconductor systems has been analyzed in terms of the most accurate quantum transmission coefficients. The fieldenhanced redistribution of carriers in systems formed between a metal and two-valley semiconductor (such as GaAs) has also been considered. In addition, the effects due to image-force lowering, interface states, temperature, and impurity concentration have been incorporated in the transport analysis to give a coherent and unified treatment. The satuation current density Js for a given metal-semiconductor system is found to reach a minimum value at a particular doping e. g. for ptSi n-type-si system at 300°K the value of Js is 8×10-8 A/cm2 at a doping of 1014 cm-3,reaches a minimum of 6×10-8 A/cm2 at 1016 cm-3, then rapidly increases to 10+3 A/cm2 at 1020 cm-3. This fact indicated the importance of doping effect on the rectifying for ohmic behavior of the system. the room-temperature transition doping for breakdown in metal-silicon system occurs at 1018 cm-3, for lower dopings the breakdown is due to avalanche multiplication, and for higher dopings due to tunneling of carriers from metal Fermi level to semiconductor hand edges. For the two-valley system with low doping e.g. 1014 to 1016 cm-3 one obtains negative differential resistance in the reverse direction. the metal-silicon barriers are fabricated by planar technique with guard-ring structures to eliminate edge effects. Extensive experimental studies including current-voltage, capacitance-voltage, photoelectric, and differential conductance measurements covering doping range from 1014 to 1020 cm-3 and temperature fange from 77°K to 373°K give good agreement with the theoretical predictions. differentiation measurements at 4.2°K also reveal scatterings of phonons with interface stated ans phonon-phonon interactions between different valleys along the <100> axis.zh_TW
dc.language.isozh_TWen_US
dc.subject金屬zh_TW
dc.subject半導體zh_TW
dc.subject介面zh_TW
dc.subject電子工程zh_TW
dc.subjectMETALen_US
dc.subjectSEMICONDUCTORen_US
dc.subjectINTERFACEen_US
dc.subjectTRANSPORT-ANALYSISen_US
dc.subjectSATURATION-CURRENTen_US
dc.subjectGUARD-RING-STRUCTUREen_US
dc.subjectMETAL-SILICON-SYSTEMen_US
dc.subjectELECTRONIC-ENGINEERINGen_US
dc.title金屬半導體介面之研究zh_TW
dc.typeThesisen_US
dc.contributor.department電子研究所zh_TW
顯示於類別:畢業論文