Second-order nonlinear optical properties of Ge-Ga-Ag-S glass irradiated by electron beam
Ge-Ga-Ag-S chalcogenide glasses with the composition Ge30Ga3Ag4S63 were obtained by the conventional melt-quenching method. According to the visible-infrared and infrared spectra, Ge30Ga3Ag4S63 chalcogenide glass possesses wide transmittance window from 510 nm in the visible region up to 11.5 μm in...
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| Published in | Transactions of Nonferrous Metals Society of China Vol. 16; no. B01; pp. 170 - 173 |
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| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
Elsevier Ltd
01.06.2006
Key Laboratory of Silicate Materials Science and Engineering, Wuhan University of Technology, Ministry of Education, Wuhan 430070, China |
| Subjects | |
| Online Access | Get full text |
| ISSN | 1003-6326 |
| DOI | 10.1016/S1003-6326(06)60168-4 |
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| Abstract | Ge-Ga-Ag-S chalcogenide glasses with the composition Ge30Ga3Ag4S63 were obtained by the conventional melt-quenching method. According to the visible-infrared and infrared spectra, Ge30Ga3Ag4S63 chalcogenide glass possesses wide transmittance window from 510 nm in the visible region up to 11.5 μm in the infrared region. And the present glass has better glass-forming ability （the difference between glass transition temperature and the peak temperature of crystallization is larger than 100 ℃）. Utilizing maker-fringe technique, a prominent second-harmonic generation was observed in Ge30Ga3Ag4S63 chalcogenide glass after irradiated by an electron beam （Accelerating voltage： 25 kV; Irradiating current： 15 nA; Irradiating time： 10 min）. And the mechanism of second-harmonic generation in the Ge-Ga-Ag-S system glasses was discussed. |
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| AbstractList | Ge-Ga-Ag-S chalcogenide glasses with the composition Ge30Ga3Ag4S63 were obtained by the conventional melt-quenching method. According to the visible-infrared and infrared spectra, Ge30Ga3Ag4S63 chalcogenide glass possesses wide transmittance window from 510 nm in the visible region up to 11.5 μm in the infrared region. And the present glass has better glass-forming ability （the difference between glass transition temperature and the peak temperature of crystallization is larger than 100 ℃）. Utilizing maker-fringe technique, a prominent second-harmonic generation was observed in Ge30Ga3Ag4S63 chalcogenide glass after irradiated by an electron beam （Accelerating voltage： 25 kV; Irradiating current： 15 nA; Irradiating time： 10 min）. And the mechanism of second-harmonic generation in the Ge-Ga-Ag-S system glasses was discussed. Ge-Ga-Ag-S chalcogenide glasses with the composition Ge 30Ga 3Ag 4S 63 were obtained by the conventional melt-quenching method. According to the visible-infrared and infrared spectra, Ge 30Ga 3Ag 4S 63 chalcogenide glass possesses wide transmittance window from 510 nm in the visible region up to 11.5 μ in the infrared region. And the present glass has better glass-forming ability (the difference between glass transition temperature and the peak temperature of crystallization is larger than 100 °C). Utilizing maker-fringe technique, a prominent second-harmonic generation was observed in Ge 30Ga 3Ag 4S 63 chalcogenide glass after irradiated by an electron beam (Accelerating voltage: 25 kV; Irradiating current: 15 nA; Irradiating time: 10 min). And the mechanism of second-harmonic generation in the Ge-Ga-Ag-S system glasses was discussed. TG1; Ge-Ga-Ag-S chalcogenide glasses with the composition Ge30Ga3Ag4S63 were obtained by the conventional melt-quenching method. According to the visible-infrared and infrared spectra,Ge30Ga3Ag4S63 chalcogenide glass possesses wide transmittance window from 510 nm in the visible region up to 11.5 ìm in the infrared region. And the present glass has better glass-forming ability (the difference between glass transition temperature and the peak temperature of crystallization is larger than 100 ℃). Utilizing maker-fringe technique,a prominent second-harmonic generation was observed in Ge30Ga3Ag4S63 chalcogenide glass after irradiated by an electron beam (Accelerating voltage: 25 kV:Irradiating current: 15 nA:Irradiating time: 10 min). And the mechanism of second-harmonic generation in the Ge-Ga-Ag-S system glasses was discussed. |
| Author | 陶海征 董国平 肖海燕 林常规 赵修建 |
| AuthorAffiliation | Key Laboratory of Silicate Materials Science and Engineering, Wuhan University of Technology, Ministry of Education, Wuhan 430070, China |
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| Cites_doi | 10.1016/S0025-5408(00)00253-1 10.1016/j.ssc.2005.12.032 10.1007/s10854-005-3738-6 10.1063/1.106845 10.1016/0921-5107(94)90243-7 10.1007/BF02841369 10.1016/j.matlet.2005.10.003 10.1016/j.ssc.2004.11.010 10.1364/OL.30.001039 10.1364/OL.11.000516 10.1007/BF02835014 10.1063/1.124358 10.2109/jcersj.113.501 10.1364/OPEX.13.000789 |
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| Keywords | chalcogenide glasses microscopic mechanism second-harmonic generation Ge 30Ga 3Ag 4S 63 Ge30Ga3Ag4S63 |
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| Snippet | Ge-Ga-Ag-S chalcogenide glasses with the composition Ge30Ga3Ag4S63 were obtained by the conventional melt-quenching method. According to the visible-infrared... Ge-Ga-Ag-S chalcogenide glasses with the composition Ge 30Ga 3Ag 4S 63 were obtained by the conventional melt-quenching method. According to the... TG1; Ge-Ga-Ag-S chalcogenide glasses with the composition Ge30Ga3Ag4S63 were obtained by the conventional melt-quenching method. According to the... |
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| SubjectTerms | chalcogenide glasses Ge 30Ga 3Ag 4S 63 Ge-Ga-Ag-S玻璃 microscopic mechanism second-harmonic generation 二阶非线性光学性质 电子束发射 硫属化物玻璃 |
| Title | Second-order nonlinear optical properties of Ge-Ga-Ag-S glass irradiated by electron beam |
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