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1.
通过对双面金属包覆介质波导色散方程的微扰近似,得到当波导层为亚毫米量级时有N→0超高阶导模与偏振无关的特性.并定义了灵敏度,同时得到了灵敏度与有效折射率、厚度、波长和介电常数的关系,当有效折射率趋于零时,超高阶导模具有极高的灵敏度.  相似文献   
2.
利用密度泛函B3LYP方法,采用6-311+G基组对胸腺嘧啶分子的基态结构进行优化,计算了x,y,z三个方向上不同强度外电场条件下胸腺嘧啶的结构、能量和电荷分布.结果表明,外电场对胸腺嘧啶的结构、电荷分布、能量和分子前线轨道能级等特性均有影响,电场对分子特性的影响不仅与强度有关,而且与方向也有关,表现出胸腺分子对于电场的响应具有各向异性.  相似文献   
3.
利用超高阶导模测量PMN-PT透明陶瓷二次电光系数   总被引:3,自引:1,他引:2  
以亚毫米尺度的铌镁酸铅-钛酸铅(PMN-PT)透明陶瓷片为导波层制备了对称金属包覆波导,并利用自由空间耦合技术激发了波导中的超高阶导模.根据衰减全反射(ATR)峰的移动,得到了在波导两侧所施加电压与光强反射率的关系,从而计算了PMN-PT透明陶瓷片的二次电光系数.  相似文献   
4.
The linear optical properties and Kerr nonlinear optical response in a four-level loop configuration Ga As/Al Ga As semiconductor quantum dot are analytically studied with the phonon-assisted transition(PAT). It is shown that the changes among a single electromagnetically induced transparency(EIT) window, a double EIT window and the amplification of the probe field in the absorption curves can be controlled by varying the strength of PAT κ. Meanwhile, double switching from the anomalous dispersion regime to the normal dispersion regime can likely be achieved by increasing the Rabi energy of the external optical control field. Furthermore, we demonstrate that the group velocity of the probe field can be practically regulated by varying the PAT and the intensity of the optical control field. In the nonlinear case, it is shown that the large SPM and XPM can be achieved as linear absorption vanishes simultaneously, and the PAT can suppress both third-order self-Kerr and the cross-Kerr nonlinear effect of the QD. Our study is much more practical than its atomic counterpart due to its flexible design and the controllable interference strength, and may provide some new possibilities for technological applications.  相似文献   
5.
结合改进的显色方案,利用空芯金属包覆波导结构,测量饮用水中锰的痕量浓度.由于波导超高阶导模的高灵敏度,作为波导导波层的錳溶液消光系数的微小变化可导致反射率极小值的显著改变.而錳溶液消光系数与浓度密切相关(折射率虚部).模拟计算的结果显示该方案的检测分辨率可达到Δκ=1.0×10-6 .  相似文献   
6.
利用双面金属包覆介质波导色散方程,通过微扰近似,当波导层为亚毫米量级时有N→0的特性,得到超高阶导模与偏振无关.定义了灵敏度,得到了灵敏度与有效折射率、厚度、波长和介电常数的关系,当有效折射率趋于零时,超高阶导模具有极高的灵敏度.该理论在制备生物传感器、光电子器件中具有指导意义.  相似文献   
7.
李勇  王应  李尚升  李宗宝  罗开武  冉茂武  宋谋胜 《物理学报》2019,68(9):98101-098101
FeNiMnCo-C体系中,在压力6.5 GPa、温度1280—1300℃的极端物理条件下,采用温度梯度法成功合成了硼(B)、硫(S)协同掺杂金刚石大单晶.通过傅里叶红外光谱测试对高温高压所制备金刚石中的杂质进行了表征.借助霍尔效应对典型金刚石样品的电输运性能进行了测试,测试结果表明:硼硫协同掺杂有利于提高p型金刚石的电导率,而且硼硫在合成体系中的添加比例可以决定金刚石的p, n特性.此外,第一性原理计算结果表明,合成体系中不同比例的硼硫协同掺杂对金刚石的p, n特性以及电导率有着直接的影响,计算结果与实验测试结果相吻合.  相似文献   
8.
利用亚毫米尺度双面金属对称包覆波导测量茅台酒的折射率,测量方法只需待测茅台酒对激光透明,则折射率大小不受限制,此方法简单有效,精度可达1.0 ×10-4,从而可以用来鉴定茅台酒的真伪.  相似文献   
9.
Yong Li 《中国物理 B》2022,31(4):46107-046107
Crystallization of diamond with different nitrogen concentrations was carried out with a FeNiCo-C system at pressure of 6.5 GPa. As the nitrogen concentration in diamond increased, the color of the synthesized diamond crystals changed from colorless to yellow and finally to atrovirens (a dark green). All the Raman peaks for the obtained crystals were located at about 1330 cm-1 and contained only the sp3 hybrid diamond phase. Based on Fourier transform infrared results, the nitrogen concentration of the colorless diamond was < 1 ppm and absorption peaks corresponding to nitrogen impurities were not detected. However, the C-center nitrogen concentration of the atrovirens diamond reached 1030 ppm and the value of A-center nitrogen was approximately 180 ppm with a characteristic absorption peak at 1282 cm-1. Furthermore, neither the NV0 nor the NV- optical color center existed in diamond crystal with nitrogen impurities of less than 1 ppm by photoluminescence measurement. However, Ni-related centers located at 695 nm and 793.6 nm were observed in colorless diamond. The NE8 color center at 793.6 nm has more potential for application than the common NV centers. NV0 and NV- optical color centers coexist in diamond without any additives in the synthesis system. Importantly, only the NV- color center was noticed in diamond with a higher nitrogen concentration, which maximized optimization of the NV-/NV0 ratio in the diamond structure. This study has provided a new way to prepare diamond containing only NV- optical color centers.  相似文献   
10.
利用级联型波导结构来增强古斯-汉欣位移.用两块完全相同的对称金属包覆波导制备级联型波导,研究了反射光束的古斯-汉欣位移增强效应.结果表明,当激光在级联型波导之间反射8次、波长从859.630nm变化到859.673 nm时,古斯-汉欣位移大于5 mm,消光比可以达到50 d B.  相似文献   
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