完整後設資料紀錄
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dc.contributor.authorCheng, Feien_US
dc.contributor.authorLee, Chien-Juen_US
dc.contributor.authorChoi, Junhoen_US
dc.contributor.authorWang, Chun-Yuanen_US
dc.contributor.authorZhan, Qiangen_US
dc.contributor.authorZhang, Huien_US
dc.contributor.authorGwo, Shangjren_US
dc.contributor.authorChang, Wen-Haoen_US
dc.contributor.authorLi, Xiaoqinen_US
dc.contributor.authorShih, Chih-Kangen_US
dc.date.accessioned2019-04-02T06:00:17Z-
dc.date.available2019-04-02T06:00:17Z-
dc.date.issued2019-01-23en_US
dc.identifier.issn1944-8244en_US
dc.identifier.urihttp://dx.doi.org/10.1021/acsami.8b16667en_US
dc.identifier.urihttp://hdl.handle.net/11536/148783-
dc.description.abstractSingle crystalline Ag films on dielectric substrates have received tremendous attention recently due to their technological potentials as low loss plasmonic materials. Two different growth approaches have been used to produce single crystalline Ag films previously. One approach is based on repetitive cycles of a two-step process (low temperature deposition followed by RT annealing) using molecular beam epitaxy (MBE), which is extremely time-consuming due to the need for repeat growth cycles. Another approach is based on rapid e-beam deposition which is capable of growing thick single crystalline Ag films (>300 nm) but lacks the precision in thickness control of thin epitaxial films. Here, we report a universal approach to grow atomically smooth epitaxial Ag films by eliminating the repetitive cycles used in the previous two-step MBE method while maintaining the precise thickness control from a few monolayers to the optically thick regime, thus overcoming the limitations of the two aforementioned methods. In addition, we develop an in situ growth of aluminum oxide as the capping layer to protect the epitaxial Ag films. The quality of the epitaxial Ag films was evaluated using a variety of techniques, and the superior optical performance of the films is demonstrated by measuring the propagation length of surface plasmon polaritons (similar to 80 mu m at 632 nm) as well as their capability to support a plasmonic nanolaser in infrared incorporating an InGaAsP quantum well as the gain media.en_US
dc.language.isoen_USen_US
dc.subjectepitaxial growthen_US
dc.subjectsingle crystalline silver filmen_US
dc.subjectsurface plasmon polaritonsen_US
dc.subjectpropagation lengthen_US
dc.subjectplasmonic lasingen_US
dc.titleEpitaxial Growth of Optically Thick, Single Crystalline Silver Films for Plasmonicsen_US
dc.typeArticleen_US
dc.identifier.doi10.1021/acsami.8b16667en_US
dc.identifier.journalACS APPLIED MATERIALS & INTERFACESen_US
dc.citation.volume11en_US
dc.citation.spage3189en_US
dc.citation.epage3195en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000457067300072en_US
dc.citation.woscount0en_US
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