人工晶体学报
人工晶體學報
인공정체학보
2009年
5期
1059-1062
,共4页
郭飞云%庄乃锋%赵斌%陈建中
郭飛雲%莊迺鋒%趙斌%陳建中
곽비운%장내봉%조빈%진건중
磁光晶体%提拉法%费尔德常数%磁光优值
磁光晶體%提拉法%費爾德常數%磁光優值
자광정체%제랍법%비이덕상수%자광우치
magneto-optical crystal%Czochralski method%Verdet constant%magneto-optical figure of merit
采用Czochralski法生长了Li_(0.067)Na_(0.933)Tb(MoO_4)_2晶体,并测试了Li~+在NaTb(MoO_4)_2晶体中的有效分凝系数.由粉末X射线衍射数据计算了晶体的晶胞参数.室温下,采用消光法测试了Li_(0.063)Na_(0.933)Tb(MoO_4)_2晶体在532 nm、633 nm和1064 nm处的费尔德常数,分别为-293.6 rad·m~(-1)·T~(-1)、-200.5 rad·m~(-1)·T~(-1)和-68.6 rad·m~(-1)·T~(-1),与纯NaTb(MoO_4)_2相比,其费尔德常数均有所增加.结果表明,在1064 nm处Li_(0.067)Na_(0.933)Tb(MoO_4)_2晶体有较高的磁光优值.
採用Czochralski法生長瞭Li_(0.067)Na_(0.933)Tb(MoO_4)_2晶體,併測試瞭Li~+在NaTb(MoO_4)_2晶體中的有效分凝繫數.由粉末X射線衍射數據計算瞭晶體的晶胞參數.室溫下,採用消光法測試瞭Li_(0.063)Na_(0.933)Tb(MoO_4)_2晶體在532 nm、633 nm和1064 nm處的費爾德常數,分彆為-293.6 rad·m~(-1)·T~(-1)、-200.5 rad·m~(-1)·T~(-1)和-68.6 rad·m~(-1)·T~(-1),與純NaTb(MoO_4)_2相比,其費爾德常數均有所增加.結果錶明,在1064 nm處Li_(0.067)Na_(0.933)Tb(MoO_4)_2晶體有較高的磁光優值.
채용Czochralski법생장료Li_(0.067)Na_(0.933)Tb(MoO_4)_2정체,병측시료Li~+재NaTb(MoO_4)_2정체중적유효분응계수.유분말X사선연사수거계산료정체적정포삼수.실온하,채용소광법측시료Li_(0.063)Na_(0.933)Tb(MoO_4)_2정체재532 nm、633 nm화1064 nm처적비이덕상수,분별위-293.6 rad·m~(-1)·T~(-1)、-200.5 rad·m~(-1)·T~(-1)화-68.6 rad·m~(-1)·T~(-1),여순NaTb(MoO_4)_2상비,기비이덕상수균유소증가.결과표명,재1064 nm처Li_(0.067)Na_(0.933)Tb(MoO_4)_2정체유교고적자광우치.
Li_(0.067)Na_(0.933)Tb(MoO_4)_2 magneto-optical crystal was grown by the Czochralski method. The effective segregation coefficient of Li~+ in NaTb(MoO_4)_2 was measured. The lattice parameters of the crystal were determined by XRD data. Verdet constants of Li 0.067Na0.933Tb(MoO4)2 crystal at the wavelength 532 nm, 633 nm and 1064 nm were investigated by the extinction method at room temperature. They are -293.6 rad·m~(-1)·T~(-1),-200.5 rad·m~(-1)·T~(-1) and -68.6 rad·m~(-1)·T~(-1), respectively, and are larger than that of pure NaTb(MoO_4)_2 at corresponding wavelengths. The results showed that Li_(0.067)Na_(0.933)Tb(MoO_4)_2 has a larger magneto-optical figure of merit at 1064 nm wavelength.