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dc.contributor.authorKu, S. A.en_US
dc.contributor.authorTu, C. M.en_US
dc.contributor.authorChu, W. -C.en_US
dc.contributor.authorLuo, C. W.en_US
dc.contributor.authorWu, K. H.en_US
dc.contributor.authorYabushita, A.en_US
dc.contributor.authorChi, C. C.en_US
dc.contributor.authorKobayashi, T.en_US
dc.date.accessioned2014-12-08T15:31:22Z-
dc.date.available2014-12-08T15:31:22Z-
dc.date.issued2013-06-17en_US
dc.identifier.issn1094-4087en_US
dc.identifier.urihttp://dx.doi.org/10.1364/OE.21.013930en_US
dc.identifier.urihttp://hdl.handle.net/11536/22292-
dc.description.abstractThis study systematically investigates the influence of free carriers on the generation of THz in ZnTe crystals, over a wide range of pumping fluences. As the pumping fluence is increased (< 6.36 mJ/cm(2)), the concentration of free carriers gradually increases and the THz output power is saturated, as clearly demonstrated by the time delay in the THz temporal waveforms, the changes in the THz spectral weight and the red-shift in the PL spectra. For high pumping fluences (> 6.36 mJ/cm(2)), spectacularly, there is a significant quadratic increase in the THz output power when the pumping fluence is increased, as well as at low pumping fluences of < 0.58 mJ/cm(2), because of the saturation of free carriers. (C) 2013 Optical Society of Americaen_US
dc.language.isoen_USen_US
dc.titleSaturation of the free carrier absorption in ZnTe crystalsen_US
dc.typeArticleen_US
dc.identifier.doi10.1364/OE.21.013930en_US
dc.identifier.journalOPTICS EXPRESSen_US
dc.citation.volume21en_US
dc.citation.issue12en_US
dc.citation.spage13930en_US
dc.citation.epage13937en_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000320510300005-
dc.citation.woscount5-
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