共查询到19条相似文献,搜索用时 140 毫秒
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MOCVD生长的GaN膜的光学性质研究 总被引:5,自引:2,他引:3
本文报道(0001)晶向蓝宝石衬底上金属有机化学气相淀积(MOCVD)方法生长的单晶六角GaN薄膜室温光学性质.由光吸收谱和488umAr+激光激发的光调制反射光谱(PR)确定的禁带宽度分别为3.39和3.400eV,从光吸收谱得到了GaN薄膜的折射率随光谱能量的变化关系.对PR谱的调制机理进行的分析,发现信号来自缺陷作用下的表面电场调制.应用喇曼光谱研究了GaN薄膜中的声子模,通过对LO声子-等离激元的耦合模散射峰的研究,得到了材料中的载流子浓度和等离激元阻尼常数. 相似文献
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研究了利用太赫兹时间分辨系统研究有机卤化物钙钛矿薄膜(CH_3NH_3PbI_3 and CH_3NH_3PbI_(3-x)Cl_x)的皮秒尺度的超快太赫兹调制特性.在光激发作用下出现了太赫兹透射波的瞬时下降.相比于CH_3NH_3PbI_3薄膜,在光激发作用下CH_3NH_3PbI_(3-x)Cl_x薄膜展现了更高的调制深度(10%).通过测算材料的电导率及载流子浓度,其调制机理为瞬态光激发载流子浓度上升.实验结果表明,CH_3NH_3PbI_(3-x)Cl_x薄膜可作为一种高效超快太赫兹调制器件. 相似文献
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《红外与毫米波学报》2018,(5)
研究了利用太赫兹时间分辨系统研究有机卤化物钙钛矿薄膜(CH_3NH_3PbI_3 and CH_3NH_3PbI_(3-x)Cl_x)的皮秒尺度的超快太赫兹调制特性.在光激发作用下出现了太赫兹透射波的瞬时下降.相比于CH_3NH_3PbI_3薄膜,在光激发作用下CH_3NH_3PbI_(3-x)Cl_x薄膜展现了更高的调制深度(10%).通过测算材料的电导率及载流子浓度,其调制机理为瞬态光激发载流子浓度上升.实验结果表明,CH_3NH_3PbI_(3-x)Cl_x薄膜可作为一种高效超快太赫兹调制器件. 相似文献
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负折射率半透明薄膜的热发射特性研究 总被引:1,自引:1,他引:0
根据传输矩阵法和基尔霍夫定律研究了负折射率薄膜的热发射特性.较为系统地考察了相关参数对热辐射s偏振波的影响.研究结果表明,负折射率材料的热发射率随角频率的变化呈现复杂的振荡现象.同时也发现,它的发射率峰值有时在远离法线的区域. 相似文献
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采用真空热蒸镀技术制备了NPB有机半导体薄膜和单层夹心结构器件,通过透射谱测量研究了薄膜的光学能隙、折射率和消光系数等光学性质,结果表明有机半导体薄膜具有直接带隙半导体的光学性质,并且其折射率色散性质遵循单振子模型.另外,通过分析器件的电流-电压特性研究了薄膜的电导率、载流子迁移率和载流子浓度等电学性质.这些实验结果对于有机光电子器件的结构设计具有一定的参考价值. 相似文献
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《Lightwave Technology, Journal of》2008,26(16):2909-2918
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二维非线性梯度折射率介质的热辐射特性研究 总被引:1,自引:0,他引:1
发展了二维梯度折射率介质热辐射传递的数值求解方法,研究了非线性折射率介质的表观方向发射率.研究结果表明,采用本文方法计算二维梯度折射率介质的表观方向发射率,最大相对误差小于1.6%.通过研究发现,二维非线性梯度折射率介质的热辐射能够呈现非常明显的定向辐射的特征,我们定义这种现象为类相干发射. 相似文献
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Gustavo E. Aizenberg Pieter L. Swart Beatrys M. Lacquet 《Journal of Electronic Materials》1992,21(11):1033-1040
A new method for the characterization of ion-implanted silicon is proposed. It is based on analysis of the Fourier spectrum
of bilinearly transformed infrared reflectance versus wavenumber data of ion-implanted samples. This non-destructive technique
has been applied to previously published infrared reflectance data of 〈111〉 and 〈100〉 oriented Si samples which had been implanted
with 2.7 MeV phosphorus and 380 keV silicon ions, respectively, and annealed at 500° C for various lengths of time. The refractive
index and thickness of the amorphous layer of the as-implanted samples can be measured directly by means of this technique.
The position of boundaries between the amorphous, recrystallized and substrate zones, as well as the position of the carrier
concentration peak can be determined for the various annealing times. Depending on the annealing time, the recrystallized
layer in 〈111〉 silicon has a refractive index which is between 2% and 4% higher than the substrate refractive index, while
the difference in refractive index between the amorphous and recrystallized layers is in the order of 5%. In contrast to these
results, the presence of the substrate/recrystallized material interface could not be detected in partially recrystallized
〈100〉 silicon by this method, implying that the refractive index step at the substrate/recrystallized material interface is
less than 1%. The step in refractive index at the crystalline/amorphous interface in 〈100〉 silicon implanted with a dose of
0.5 x 1016 cm−2 silicon ions, was measured to be 12%, and it is reduced to 8% after partial regrowth has occurred. These results confirm
the data obtained by a model-based least-squares analysis. 相似文献
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施国栋 《大气与环境光学学报》2022,17(5):521-532
在打破传统蒙特卡罗方法在光线跟踪计算时各个子过程连贯性的基础上,发展了灵活的逆正向蒙特卡罗法,进而利用该方法研究了介质的矢量辐射传输问题。通过建立一维梯度折射率半透明介质模型,模拟了大气层折射率分布,得到了考虑偏振时介质自身的Stokes矢量。研究结果表明,梯度折射率介质不同表面的发射率存在一定的区别,散射性介质在考虑偏振时表面发射率的结果与标量方法存在一定的差异。逆正向蒙特卡罗方法可用以解决矢量辐射传输这类复杂问题。 相似文献
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A new method is presented for reconstructing smooth refractive index profiles of optical waveguides from measured effective indexes. It is based on the semivectorial finite difference method to solve the polarized wave equation for a given refractive index profile. An iterative simplex algorithm is used to find the best refractive index parameters that give, as a solution, effective indexes close to the measured ones. The method is applied successfully to Ag+-Na + ion-exchanged glass slab waveguides and to diffused Mg/Ti:LiNbO3 slab waveguides. Dopant concentration profiles are obtained by using secondary ion mass spectrometry. The relationship between the refractive index change and the dopant concentration is determined for both cases. The iterative simplex algorithm-finite difference method (ISA-FDM) is compared to other index profile reconstruction methods, and the advantages with respect to WKB-based methods are pointed out 相似文献
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Bhushan Sopori Wei Chen Jamal Madjdpour N. M. Ravindra 《Journal of Electronic Materials》1999,28(12):1385-1389
A computer-software, Emissivity, has been developed to calculate the emissivity (ɛ) of silicon wafers of any surface morphology, for a given temperature and dopant concentration. The software uses a combination
of ray- and wave-optics approaches to include the interference and the polarization effects necessary for multilayer surface
coatings and multi-reflections within thin wafers. The refractive index and the absorption coefficient are calculated as a
function of temperature and dopant concentration using an empirical model for an indirect bandgap semiconductor. The results
of this model are compared with conventional emissivity calculations and experimental data. 相似文献
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Mos E.C. 't Hooft G.W. Schleipen J.J.H.B. de Waardt H. 《Quantum Electronics, IEEE Journal of》2001,37(7):911-918
Chaotic self-pulsation in a single wavelength external-cavity laser diode is observed. It is shown that the self-pulsation is caused by interdependencies between the optical output power and the compound cavity losses through the refractive index of the laser diode material. Refractive index changes result in a detuning between the externally selected wavelength and the weak internal-mode structure of the anti-reflection coated laser diode. This detuning is directly related to the compound cavity losses. On the one hand, a change in optical output power results in a change of the refractive index via the carrier density. On the other hand, it results in a change of refractive index via temperature changes. Compared to the carrier induced refractive index change, the temperature induced refractive index change is opposite in sign, a factor of ~102 smaller and slower. The switch-on and switch-off time of the self-pulsation is governed by the carrier life time. The repetition rate of the self-pulsation is governed by the thermal time constant and is in the megahertz region. Cross-modulation resulting from the thermal induced refractive index change is demonstrated. In a two-wavelength double external-cavity laser diode, optical power at one wavelength effects the optical power at the other wavelength. This cross-modulation is shown to be related to previous experiments on a laser neural network. A novel technique is introduced to measure the thermal impedance of a laser diode that is based on the cross-modulation 相似文献
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A plasmonic refractive index sensor based on metal-insulator-metal(MIM) waveguide-coupled structure is proposed and demonstrated in this paper.The physical mechanism of the device is deduced,and the finite difference time domain(FDTD) method is employed to simulate and study its index sensing characteristics.Both analytic and simulated results show that the resonant wavelength of the sensor has a linear relationship with the refractive index of material under sensing.Based on the relationship,the refractive index of the material can be obtained from the detection of the resonant wavelength.The results show that the sensitivity of the sensor can exceed 1600 nm/RIU,and it can be used in chemical and biological detections. 相似文献