Temperature dependence of scintillation properties for a hydrothermal-method-grown zinc oxide crystal evaluated by nickel-like silver laser pulses

Yusuke Furukawa; Momoko Tanaka; Tomoharu Nakazato; Toshihiro Tatsumi; Masaharu Nishikino; Hiroshi Yamatani; Keisuke Nagashima; Toyoaki Kimura; Hidetoshi Murakami; Shigeki Saito; Nobuhiko Sarukura; Hiroaki Nishimura; Kunioki Mima; Yuji Kagamitani; Dirk Ehrentraut; Tsuguo Fukuda

doi:10.1364/JOSAB.25.00B118

Journal of the Optical Society of America B
Vol. 25,
Issue 7,
pp. B118-B121
(2008)
•https://doi.org/10.1364/JOSAB.25.00B118

Temperature dependence of scintillation properties for a hydrothermal-method-grown zinc oxide crystal evaluated by nickel-like silver laser pulses

Yusuke Furukawa, Momoko Tanaka, Tomoharu Nakazato, Toshihiro Tatsumi, Masaharu Nishikino, Hiroshi Yamatani, Keisuke Nagashima, Toyoaki Kimura, Hidetoshi Murakami, Shigeki Saito, Nobuhiko Sarukura, Hiroaki Nishimura, Kunioki Mima, Yuji Kagamitani, Dirk Ehrentraut, and Tsuguo Fukuda

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Yusuke Furukawa, Momoko Tanaka, Tomoharu Nakazato, Toshihiro Tatsumi, Masaharu Nishikino, Hiroshi Yamatani, Keisuke Nagashima, Toyoaki Kimura, Hidetoshi Murakami, Shigeki Saito, Nobuhiko Sarukura, Hiroaki Nishimura, Kunioki Mima, Yuji Kagamitani, Dirk Ehrentraut, and Tsuguo Fukuda, "Temperature dependence of scintillation properties for a hydrothermal-method-grown zinc oxide crystal evaluated by nickel-like silver laser pulses," J. Opt. Soc. Am. B 25, B118-B121 (2008)

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Abstract

The scintillation properties of a hydrothermal-method-grown zinc oxide $(ZnO)$ crystal in the extreme ultraviolet region are evaluated using a nickel-like silver laser with an emission wavelength of $13.9 nm$ . The temperature dependence of the scintillation properties of the $ZnO$ emission at a wavelength of $\sim 380 nm$ is investigated. The emission exhibits a broad peak at $386 nm$ with a full width at half-maximum (FWHM) of $15 nm$ at room temperature $(298 K)$ . Decreasing the $ZnO$ crystal temperature to $25 K$ causes the peak position to be blueshifted by $12 nm$ while the FWHM becomes narrower by $9 nm$ as compared with the room temperature case.

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Journal of the Optical Society of America B