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dc.contributor.authorChang, Chieh-Fengen_US
dc.contributor.authorChen, Hsing-Chaoen_US
dc.contributor.authorChen, Miin-Jangen_US
dc.contributor.authorLiu, Wei-Reinen_US
dc.contributor.authorHsieh, Wen-Fengen_US
dc.contributor.authorHsu, Chia-Hungen_US
dc.contributor.authorChen, Chao-Yuen_US
dc.contributor.authorChang, Fu-Hsiungen_US
dc.contributor.authorYu, Che-Hangen_US
dc.contributor.authorSun, Chi-Kuangen_US
dc.date.accessioned2014-12-08T15:07:09Z-
dc.date.available2014-12-08T15:07:09Z-
dc.date.issued2010-03-29en_US
dc.identifier.issn1094-4087en_US
dc.identifier.urihttp://hdl.handle.net/11536/5623-
dc.description.abstractDirect-backward third harmonic generation (DBTHG) has been regarded as negligible or even inexistent due to the large value of wave-vector mismatch. In the past, BTHG signals were often interpreted as back-reflected or back-scattered forward-THG (FTHG). In this paper, we theoretically and experimentally demonstrate that backward third harmonic waves can be directly generated, and that their magnitude can be comparable with FTHG in nanostructures. Experimental data of DBTHG from ZnO thin films, CdSe quantum dots and Fe(3)O(4) nanoparticles agree well with simulation results based on the Green's function. An integral equation was also derived for fast computation of DBTHG in nano films. Our investigation suggests that DBTHG can be a potentially powerful tool in nano-science research, especially when combined with FTHG measurements. (C) 2010 Optical Society of Americaen_US
dc.language.isoen_USen_US
dc.titleDirect backward third-harmonic generation in nanostructuresen_US
dc.typeArticleen_US
dc.identifier.journalOPTICS EXPRESSen_US
dc.citation.volume18en_US
dc.citation.issue7en_US
dc.citation.spage7397en_US
dc.citation.epage7406en_US
dc.contributor.department光電工程學系zh_TW
dc.contributor.departmentDepartment of Photonicsen_US
dc.identifier.wosnumberWOS:000276602000097-
dc.citation.woscount6-
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