Experimental demonstration of underwater optical wireless power transfer using a laser diode

We experimentally demonstrate an underwater optical wireless power transfer(OWPT) using a laser diode(LD)as a power transmitter. We investigate the characteristics of a solar cell and a photodiode(PD) as a power receiver. We optimize the LD, the PD, and the solar cell to achieve the maximum transfer efficiency. The maximum transfer efficiency of the back-to-back OWPT is measured as 4.3% with the PD receiver. Subsequently, we demonstrate the OWPT in tap and sea water. Our result shows an attenuation of 3 dB/m in sea water.     

Geometrical optics-based ray field tracing method for complex source beam applications

Due to the fact that traditional ray field tracking approaches require a large number of geometrical optical(GO) ray tubes,they are very inefficient in many practical applications.An improved ray model scheme for a complex source beam(CSB) tracking technique is proposed in this paper.The source field can be expressed by a superposition of CSBs,then every CSB basis function has a Gaussian-type amplitude distribution and is suitable for replacing a GO ray tube in the ray tracing approach.The complex phase matching technique is adopted to find the reflected beam in the reflection point where local approximation is used to represent the curved surface in its neighborhood.A new solution to multiple reflections using the conventional right-handed reflected system is used to track the field easily.Numerical results show the accuracy of the proposed method.     

Two-dimensional electron gas characteristics of InP-based high electron mobility transistor terahertz detector

The samples of In_xGa_(1-x)As/In_(0.52)Al_(0.48)As two-dimensional electron gas(2DEG)are grown by molecular beam epitaxy(MBE).In the sample preparation process,the In content and spacer layer thickness are changed and two kinds of methods,i.e.,contrast body doping andδ-doping are used.The samples are analyzed by the Hall measurements at 300 Kand 77 K.The In_xGa_(1-x)As/In_(0.52)Al_(0.48)As 2DEG channel structures with mobilities as high as 10289 cm~2/V·s(300 K)and42040 cm~2/V·s(77 K)are obtained,and the values of carrier concentration(Nc)are 3.465×10~(12)/cm~2and 2.502×10~(12)/cm~2,respectively.The THz response rates of In P-based high electron mobility transistor(HEMT)structures with different gate lengths at 300 K and 77 K temperatures are calculated based on the shallow water wave instability theory.The results provide a reference for the research and preparation of In P-based HEMT THz detectors.     

过渡金属Co2+离子掺杂ZnS硫化物纳米晶制备与中红外发光特性研究

利用不含有机相的简单水热法制备了Co^2+∶ZnS纳米晶,纳米晶具有立方闪锌矿结构,平均晶粒尺寸约为8.3 nm,在808 nm激光泵浦下具有2~5μm波段的中红外荧光发射,中心波长位于3400 nm和4700 nm,分别对应Co^2+离子的4T2(F)→4 A 1(F)和4T1(F)→4T2(F)的能级跃迁.进一步将制备的纳米晶在还原气氛下进行800℃热处理,获得立方闪锌矿和纤锌矿混合晶型的纳米晶,平均晶粒尺寸增大到22.5 nm左右,热处理后的纳米晶表面羟基含量更低,中红外荧光发射强度显著提高.该Co^2+∶ZnS纳米晶的制备方法简单、在制备过程中不引入有机相等荧光淬灭中心,同时证明通过后热处理过程可以进一步减少表面缺陷及羟基含量,使荧光强度得到大幅提升.     

液体速凝剂的制备及性能

通过对多种市售有碱和无碱液体速凝剂产品的性能分析,分析总结了行业上速凝剂产品存在的不足之处。自制了一种无碱和一种有碱速凝剂产品,研究了不同辅料对速凝剂体系的协同增效作用,研究了环境温度、湿度、用水量、水泥种类等测试条件对速凝剂凝结时间的影响,总结了速凝剂在应用过程的注意事项及调整产品适应性的方法。     

Matlab软件在高等数学教学中的应用

Matlab是当今最优秀的科技应用软件之一。基于Matlab在科学计算中的强大功能,本文探讨了Matlab软件在高等数学教学中的应用。针对高等数学中的极限、导数、积分、极值等问题,在教学中融入Matlab辅助计算,把所学理论转化为实践,不仅大大地提高了教学的实效性,并且为学生今后运用所学知识解决专业、实际等问题奠定了基础。     

用于农田土壤监测的高光谱成像仪

土壤光谱分析技术具有分析速度快、成本低、无危险、无破坏、可同时反演多种成分等特点,基于高光谱成像技术可以快速获取土壤性质及其空间分布特征。本文针对农田土壤监测的需求,设计了一种无人机载高光谱成像仪,选择Offner凸光栅光谱成像系统实现了无谱线弯曲和无色畸变的设计结果。400～1 000nm波长范围内的衍射效率为15%～30%,对地成像效果清晰,在3 km飞行高度可以获得覆盖宽度为0.6km、地面分辨率为0.6 m的地物目标高光谱图像,可提供0.4～1.0μm波长范围内120个谱段的高光谱图像,光谱数据准确、稳定。结果表明,该高光谱成像仪满足设计要求且可以快速获得高精度成像光谱信息,适合用于对农田土壤的监测。     

Effects of effective attractive multi-body interaction on quantum phase and transport dynamics of a strongly correlated bosonic gas across the superfluid to Mott insulator transition

We theoretically investigate quantum phases and transport dynamics of ultracold atoms trapped in an optical lattice in the presence of effective multi-body interaction.When a harmonic external potential is added,several interesting phenomena are revealed,such as the broadening and the emergence of a central insulator plateau and the phase transition between superfluid and Mott insulator phase.We also study the transport of the system which runs across the superfluid–insulator transition after ramping up the lattice,and predict a slower relaxation which is attributed to the influence of the multi-body interaction on the mass transport.     

Transport dynamics of an interacting binary Bose Einstein condensate in an incommensurate optical lattice

We investigate the transport dynamics of an interacting binary Bose-Einstein condensate in an incommensurate optical lattice and predict a novel splitting of a matter wavepacket induced by disorder potential and inter-species interaction. The effect of atomic interaction on the dynamics of the mobile and localized atoms are also studied in detail. We also discuss the behavior of the balanced and inbalanced mixtures in the incommensurate optical lattice.     

Analysis of secondary electron emission using the fractal method

Based on the rough surface topography with fractal parameters and the Monte–Carlo simulation method for secondary electron emission properties, we analyze the secondary electron yield(SEY) of a metal with rough surface topography. The results show that when the characteristic length scale of the surface, G, is larger than 1 × 10^-7, the surface roughness increases with the increasing fractal dimension D. When the surface roughness becomes larger, it is difficult for entered electrons to escape surface. As a result, more electrons are collected and then SEY decreases. When G is less than 1 × 10^-7,the effect of the surface topography can be ignored, and the SEY almost has no change as the dimension D increases. Then,the multipactor thresholds of a C-band rectangular impedance transfer and an ultrahigh-frequency-band coaxial impedance transfer are predicted by the relationship between the SEY and the fractal parameters. It is verified that for practical microwave devices, the larger the parameter G is, the higher the multipactor threshold is. Also, the larger the value of D,the higher the multipactor threshold.