Отрывок: To characterize the optical detector in terms of photoresponse, the experiments were carried out by illuminating the detector using FCLB of varying wavelength and power density. Figure 1 shows the variation of output resistance as a function of time for three different wavelengths viz. 635 nm, 785 nm and 1064 nm wavelength of the laser beam. It is noticeable from the figure that the change in photo resistance is found to be highest when the detector was illum...
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dc.contributor.authorTalib, M.-
dc.contributor.authorMishra, I.P.-
dc.date.accessioned2018-05-18 11:24:39-
dc.date.available2018-05-18 11:24:39-
dc.date.issued2018-
dc.identifierDspace\SGAU\20180518\69510ru
dc.identifier.citationTalib M. A high performance optical detector using TiS3 nanoribbons / M. Talib, I.P. Mishra // Сборник трудов IV международной конференции и молодежной школы «Информационные технологии и нанотехнологии» (ИТНТ-2018) - Самара: Новая техника, 2018. - С.483-485.ru
dc.identifier.urihttp://repo.ssau.ru/handle/Informacionnye-tehnologii-i-nanotehnologii/A-high-performance-optical-detector-using-TiS3-nanoribbons-69510-
dc.description.abstractWe report the fabrication and characterization of TiS3 nanoribbons based detector. The TiS3 nanoribbons were fabricated using CVT method and then TiS3 nanoribbons dispersion was drop cast onto the standard electrode strip. The fabricated device was characterized by illuminating it by FCLB by varying its wavelength and power. The results shows good performance at 6.9 mW/mm2 power density of 1064 nm wavelength.ru
dc.description.sponsorshipThe authors wishing to acknowledge assistance from Department of science and technology (DST) India.ru
dc.language.isoenru
dc.publisherНовая техникаru
dc.subjectTitanium trisulfide (TiS3)ru
dc.subjectChemical vapor transport (CVT)ru
dc.subjectFiber coupled laser beam (FCLB)ru
dc.titleA high performance optical detector using TiS3 nanoribbonsru
dc.typeArticleru
dc.textpartTo characterize the optical detector in terms of photoresponse, the experiments were carried out by illuminating the detector using FCLB of varying wavelength and power density. Figure 1 shows the variation of output resistance as a function of time for three different wavelengths viz. 635 nm, 785 nm and 1064 nm wavelength of the laser beam. It is noticeable from the figure that the change in photo resistance is found to be highest when the detector was illum...-
Располагается в коллекциях: Информационные технологии и нанотехнологии

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