红外与激光工程
紅外與激光工程
홍외여격광공정
INFRARED AND LASER ENGINEERING
2014年
7期
2289-2294
,共6页
郭士亮%牛力勇%胡春海%朱君%孟靓%李志全
郭士亮%牛力勇%鬍春海%硃君%孟靚%李誌全
곽사량%우력용%호춘해%주군%맹정%리지전
半导体增益介质%MSM等离子体波导%时域有限差分法%无损传播
半導體增益介質%MSM等離子體波導%時域有限差分法%無損傳播
반도체증익개질%MSM등리자체파도%시역유한차분법%무손전파
semiconductor gain medium%metal-semiconductor-metal plasmonic waveguide%finite difference time-domain method%lossless transmission
为了深入地研究在紫外波长范围内利用增益介质补偿等离子传输损耗,设计了具有半导体增益介质的金属-半导体-金属(Metal-Semiconductor-Metal,MSM)等离子体光波导结构。基于时域有限差分法(FDTD),对该波导结构的传输损耗、有效折射率随几何结构的依赖关系进行了分析。进一步研究了利用II-VI族半导体ZnO作为增益介质时的无损传播条件。结果表明,当ZnO宽度为80 nm时,MSM等离子波导可以实现紫外波长范围的无损传播;当ZnO宽度大于80 nm时,传播增益明显大于损耗,可以实现等离子极化波的传播放大,为表面等离子体基元纳米激光器技术提供理论依据。
為瞭深入地研究在紫外波長範圍內利用增益介質補償等離子傳輸損耗,設計瞭具有半導體增益介質的金屬-半導體-金屬(Metal-Semiconductor-Metal,MSM)等離子體光波導結構。基于時域有限差分法(FDTD),對該波導結構的傳輸損耗、有效摺射率隨幾何結構的依賴關繫進行瞭分析。進一步研究瞭利用II-VI族半導體ZnO作為增益介質時的無損傳播條件。結果錶明,噹ZnO寬度為80 nm時,MSM等離子波導可以實現紫外波長範圍的無損傳播;噹ZnO寬度大于80 nm時,傳播增益明顯大于損耗,可以實現等離子極化波的傳播放大,為錶麵等離子體基元納米激光器技術提供理論依據。
위료심입지연구재자외파장범위내이용증익개질보상등리자전수손모,설계료구유반도체증익개질적금속-반도체-금속(Metal-Semiconductor-Metal,MSM)등리자체광파도결구。기우시역유한차분법(FDTD),대해파도결구적전수손모、유효절사솔수궤하결구적의뢰관계진행료분석。진일보연구료이용II-VI족반도체ZnO작위증익개질시적무손전파조건。결과표명,당ZnO관도위80 nm시,MSM등리자파도가이실현자외파장범위적무손전파;당ZnO관도대우80 nm시,전파증익명현대우손모,가이실현등리자겁화파적전파방대,위표면등리자체기원납미격광기기술제공이론의거。
For further study of the gain compensation of plasmonic waveguide for the propagation loss in the range of ultraviolet wavelengths, the metal-semiconductor-metal(MSM) plasmonic waveguide structure embedded with semiconductor gain medium was proposed and designed in this article. Based on the finite difference time-domain(FDTD) method, the dependences of propagation loss and effective refractive index on the geometrical parameters of the waveguide structure were analyzed. In addition, the condition for lossless propagation in using II-VI semiconductor material ZnO as the gain medium was investigated. The simulation results show that the lossless gain-assisted surface plasmon polartions propagation in MSM can be achieved for ultraviolet wavelengths when the width of the semiconductor core is 80 nm; and the propagation loss is much less than the gain obviously as the width of ZnO is greater than 80 nm. This achievement can realize the propagation amplification of surface plasmonic polartions, which provides the theoretical support for surface plasmon polariton nano-laser technologies.