完整後設資料紀錄
DC 欄位 | 值 | 語言 |
---|---|---|
dc.contributor.author | 張俊彥 | en_US |
dc.contributor.author | Zhang, Zun-Yan | en_US |
dc.contributor.author | 施敏 | en_US |
dc.contributor.author | Shi, Min | en_US |
dc.date.accessioned | 2014-12-12T02:01:08Z | - |
dc.date.available | 2014-12-12T02:01:08Z | - |
dc.date.issued | 1970 | en_US |
dc.identifier.uri | http://140.113.39.130/cdrfb3/record/nctu/#NT594428001 | en_US |
dc.identifier.uri | http://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.iso | zh_TW | en_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.subject | METAL | en_US |
dc.subject | SEMICONDUCTOR | en_US |
dc.subject | INTERFACE | en_US |
dc.subject | TRANSPORT-ANALYSIS | en_US |
dc.subject | SATURATION-CURRENT | en_US |
dc.subject | GUARD-RING-STRUCTURE | en_US |
dc.subject | METAL-SILICON-SYSTEM | en_US |
dc.subject | ELECTRONIC-ENGINEERING | en_US |
dc.title | 金屬半導體介面之研究 | zh_TW |
dc.type | Thesis | en_US |
dc.contributor.department | 電子研究所 | zh_TW |
顯示於類別: | 畢業論文 |