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dc.contributor.authorChen, Kejianen_US
dc.contributor.authorLi, Yu-taien_US
dc.contributor.authorYang, Mong-huanen_US
dc.contributor.authorCheung, Wing Yiuen_US
dc.contributor.authorPan, Ci-Lingen_US
dc.contributor.authorChan, Kam Taien_US
dc.date.accessioned2014-12-08T15:09:42Z-
dc.date.available2014-12-08T15:09:42Z-
dc.date.issued2009-04-01en_US
dc.identifier.issn0146-9592en_US
dc.identifier.urihttp://dx.doi.org/10.1364/OL.34.000935en_US
dc.identifier.urihttp://hdl.handle.net/11536/7418-
dc.description.abstractTerabertz wave (THz) photoconductive (PC) antennas were fabricated on oxygen-implanted GaAs (GaAs:O) and low-temperature-grown GaAs (LT-GaAs). The measured cw THz power at 0.358 THz from the GaAs:O antenna is about twice that from the LT-GaAs antenna under the same testing conditions, with the former showing no saturation up to a bias of 40 kV/cm, while the latter is already beginning to saturate at 20 kV/cm. A modified theoretical model incorporating bias-field-dependent electron saturation velocity is employed to explain the results. It shows that GaAs:O exhibits a higher electron saturation velocity, which may be further exploited to generate even larger THz powers by reducing the ion dosage and optimizing the annealing process in GaAs:O. (C) 2009 Optical Society of Americaen_US
dc.language.isoen_USen_US
dc.titleComparison of continuous-wave terahertz wave generation and bias-field-dependent saturation in GaAs:O and LT-GaAs antennasen_US
dc.typeArticleen_US
dc.identifier.doi10.1364/OL.34.000935en_US
dc.identifier.journalOPTICS LETTERSen_US
dc.citation.volume34en_US
dc.citation.issue7en_US
dc.citation.spage935en_US
dc.citation.epage937en_US
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Photonicsen_US
dc.identifier.wosnumberWOS:000265429100025-
dc.citation.woscount6-
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