红外与激光工程
紅外與激光工程
홍외여격광공정
INFRARED AND LASER ENGINEERING
2014年
10期
3368-3372
,共5页
高静%于峰%葛廷武%王智勇
高靜%于峰%葛廷武%王智勇
고정%우봉%갈정무%왕지용
硫系玻璃%线性折射率%色散%中红外%超连续谱
硫繫玻璃%線性摺射率%色散%中紅外%超連續譜
류계파리%선성절사솔%색산%중홍외%초련속보
chalcogenide glass%linear refractive index%dispersion%mid-IR%supercontinuum
硫系材料由于具有较长波长的红外透光截止波段,且具有较高的线性折射率和高非线性系数,是产生中红外超连续谱激光的理想非线性介质材料。由于泵浦非线性介质一般多采用波长2μm以下的激光源,所以研究材料的色散很有意义。利用4种不同形式的方程拟合了3种硫系玻璃材料As2S3、As2Se3、Ge33As12Se55的折射率随波长的变化曲线,并计算了材料色散曲线,得到了较为理想的结果,3种材料的零色散波长分别为4.8μm、7.2μm、6.1μm。同时证明了对于硫系玻璃材料,不能只利用短波长下的折射率值拟合计算长波长下的折射率。
硫繫材料由于具有較長波長的紅外透光截止波段,且具有較高的線性摺射率和高非線性繫數,是產生中紅外超連續譜激光的理想非線性介質材料。由于泵浦非線性介質一般多採用波長2μm以下的激光源,所以研究材料的色散很有意義。利用4種不同形式的方程擬閤瞭3種硫繫玻璃材料As2S3、As2Se3、Ge33As12Se55的摺射率隨波長的變化麯線,併計算瞭材料色散麯線,得到瞭較為理想的結果,3種材料的零色散波長分彆為4.8μm、7.2μm、6.1μm。同時證明瞭對于硫繫玻璃材料,不能隻利用短波長下的摺射率值擬閤計算長波長下的摺射率。
류계재료유우구유교장파장적홍외투광절지파단,차구유교고적선성절사솔화고비선성계수,시산생중홍외초련속보격광적이상비선성개질재료。유우빙포비선성개질일반다채용파장2μm이하적격광원,소이연구재료적색산흔유의의。이용4충불동형식적방정의합료3충류계파리재료As2S3、As2Se3、Ge33As12Se55적절사솔수파장적변화곡선,병계산료재료색산곡선,득도료교위이상적결과,3충재료적령색산파장분별위4.8μm、7.2μm、6.1μm。동시증명료대우류계파리재료,불능지이용단파장하적절사솔치의합계산장파장하적절사솔。
Due to a high transmission in the infrared range as well as the high linear refractive index and nonlinearity, chalcogenide glass was a good candidate for mid-infrared supercontinuum generation. Since the wavelengths of pump sources for pumping nonlinear mediums are usually less than 2 μm, it is valuable to study their material dispersion. Used four different forms of equation to fit the refractive index versus wavelength curves, three different kinds of chalcogenide glass was simulated:As2S3, As2Se3 and Ge33As12Se55, also we got their material dispersion curves by the former simulation results. Their zero-dispersion wavelengths are 4.8μm, 7.2μm, 6.1μm, respectively. While proved that it is not suitable to use refractive index data at short wavelength to fit and simulate the trend at long wavelength for chalcogenide glass.