量子阱中电子-LO声子相互作用引起共振喇曼散射的不对称线形

提出在量子阱中,由于连续态电子与LO声子相互作用,通过对量子阱进行某种设计,并以特定的激光频率入射,可以导致Raman谱中很强的Fano现象.以GaAs-Al_2Ga_(1-x)As为例计算了几种量子阱结构下的不对称参量q,并给出了相应的Fano线形 关键词：     

新基本粒子的重大发现

根据1983年2月7日美国“时代周刊”报道,欧洲核子研究中心最近发现了一个新的重要的基本粒子——中间矢量玻色子. 长期以来,物理学家认为,自然界中至少有四种物质间的基本相互作用,即引力相互作用、电磁相互作用、强相互作用和弱相互作用.前两种相互作用存在于一切宏观世界和微     

交直场共存下抛物势阱中的量子力学解析解及n-i-p-i量子阱光学谐波理论

严格处理外场下量子力学问题对于研究非线性光学问题是十分重要的。我们得到了抛物势阱中交直流电场共存下粒子波函数的严格解析解,并将其引入了n-i-p-i量子阱的光学谐波理论。     

GaAs/AlxGa1-xAs超晶格子带间光跃迁的研究

运用Kronig-Penney模型的新形式,研究了超晶格子带间光跃迁的频率、带宽和跃迁强度,用GaAs/Al_xGa_1-xAs多量子阱材料做了关于红外吸收的实验,理论与实验符合较好。 关键词：     

QUANTUM PERCOLATION AND BALLISTIC CONDUCTANCE IN A SYSTEM OF DOUBLE-COUPLED CHAINS

The quantum-mechanical calculation of electronic conductance in double-coupled chains as a function of the interchain bonding probability p is presented. The calculated results show that one still can see the basic plateaus in the ensemble-averaged conductance curves as a function of the Fermi energy for the weak disorder. In addition, dense irregularly oscillating structures are superimposed upon each plateau. The characteristics of the conductance are very sensitive to the presence of the interchain broken bonds. For the strong disorder (p≈0.5) the conductance quantization breaks down. The accuracy of the quantization conductance rapidly drops down as the value of p approaches 0.5. The ensemble-averaged value of the logarithmic conductance as a function of the sample length exhibits a linear variation, determining a localization length. Both the localization length and the root-mean- square (RMS) value of the conductance fluctuations depend on p and the Fermi energy of electrons. The variations of the localization length and RMS with p are both of an approximate parabolic function around p≈0.5. No percolation transition is found for this quasi-one-dimensional system, as expected.     

阶梯量子阱子带跃迁二次谐波产生的研究

本文理论上利用二能级近似下的传递矩阵法,给出了GaAs/Al_xGa_1-xAs二阶非线性光学系数X_2ω⁽²⁾的解析表达式,通过数值计算,设计了具有较大X_2ω⁽²⁾的阶梯多量子阱(SMQW)结构,其特点是单共振泵浦,实验上验证了该结构确实具有比体材料大3个量级的X_2ω⁽²⁾值,为了提高二次谐波(SHG)的转换效率,我们分别设计了两种新型的实验方案,分别使SHG转换效率较Brewster角入射下大10倍和100倍。     

隧穿展宽对超晶格子带间光吸收饱和的影响

本文运用Kronig—Penney模型新形式,研究超晶格子带间光吸收的三阶非线性效应,发现不论量子阱参数(如阱宽、垒宽和垒高等)如何改变,光吸收饱和强度与隧穿谱宽之间存在着一种较普遍的关系,并阐明了这种依从关系的物理机制。     

YBa2 Cu3 O7-δ/SrNb0.01 Ti0.99 O3 p-n结的制备及其特性

采用脉冲激光沉积技术,在n型SrNb0.01Ti0.99O3(SNTO)单晶基片上生长p型YBa2Cu3O7-δ(YBCO)薄膜,制备出YBCO/SNTO p-n结.YBCO薄膜是高度c轴织构的超导薄膜,且具有良好的超导电性.YBCO/SNTO p-n结具有较好的整流特性和很好的温度与磁场稳定性.     

Nonlinear optical properties of Au/PVP composite thin films

Colloidal Au and poly（vinylpyrrolidone） （PVP） composite thin films are fabricated by spin-coating method. Linear optical absorption measurements of the Au/PVP composite films indicate an absorption peak around 530 nm due to the surface plasmon resonance of gold nanoparticles. Nonlinear optical properties are studied using standard Z-scan technique, and experimental results show large optical nonlinearities of the Au/PVP composite films. A large value of χ^（3）/α up to 0.56× 10-^10esu·cm is obtained, which is comparable to the best values reported in metal/oxlde composite films.     

The mechanism research of the Cr^4＋Nd^3＋：YAG laser

The 946nm diode-pump microchip self-Q-switched laser of a chromium and neodymium codoped yttrium aluminum garnet crystal material (Cr^{4+}Nd^{3+}:YAG) is studied, especially about its physical mechanism of operation. The {}^4F_{3/2}→{}^4I_{9/2} transition of Nd^{3+} ion is beneficial to achieving laser oscillation in a quasi-three-level system based on coating the cavity mirrors of the microchip with films that suppress the 1064nm operation and enhance the 946nm laser. The Cr^{4+} ion is a saturable absorber. The initial loss N_{t1} is high, which acts as the threshold for laser oscillation. The stable loss N_{t2} is low because the Cr^{4+} ion is acceleratively bleached by the fast enhancement of the oscillating laser. The high N_{t1}, small N_{t2} and fast progresses permit the oscillating laser of the Cr^{4+}Nd^{3+}:YAG to have a good self-Q-switched property whose full width at half maximum is about 4.2ns. Its highest laser power is about 5.7mW. Its peak power is about 150W. Its good fundamental transverse TEM_{00} mode results from the absorption bleaching established by both the pump and oscillating lasers, which suppress other transverse mode and allow the oscillation only in the fundamental transverse TEM_{00} mode.