Tl2Ba2Ca2Cu3Oy超导体磁通钉扎能的分布

描述一种测量高温超导体磁通钉扎能U₀及其分布的新方法,此方法主要之点是测量磁化后样品的零场临界电流随时间的变化,利用这一方法测量Tl₂Ba₂Ca₂Cu₃O_y的U₀值分布(T=78K)。根据所得结果,对已报道的U₀值的分散性提出一种新解释。 关键词：     

掺Ba的Bi-Sr-Cu-O单晶Raman散射研究

利用Ｒａｍａｎ散射研究了Bi₂Sr_2-xBa_xCuO_y（ｘ＝０，０．２，０．４）单晶样品的声子振动性质。实验结果表明，在Bi₂Sr_2-xBa_xCuO_y体系的Ｒａｍａｎ谱中主要出现以下几个频率的特征振动模，即１９６，３００，４６０，６２５和６６０ｃｍ^－１；而频率为１９６，３００，６２５，６６０ｃｍ^－１<     

小型企业规模的有效性分析

在当代企业纷纷追求规模的不断扩大的同时，统计数据却显示企业平均规模不断下降的事实趋势。论根据数学、经济学与博弈论的有关理论对企业规模小型化的内在要求进行了探讨，分析的结论一致证明：粘型化规模在当代经济环境中是充分有效的。     

有理逼近的一些最新进展

作为非线性逼近的一个重要特殊情形，有理函数逼近（即有理逼近）无论在实践中还是在应用中有都有重要的意义，有理逼近日益成为逼近论的一个重要和具有很强生命力的课题。近年来，在这一方面的研究成果不断涌现，其中许多都是非常有意义的。本文将对此作一个总结，特别对其中涉及我们自己的工作作一个回顾。     

脉冲电场对木瓜蛋白酶影响的荧光光谱分析

木瓜蛋白酶溶液在电场强度为50 kV·cm-1,频率1 500 Hz,脉冲宽度40 μs的脉冲电场下接受19 800个脉冲处理后,其活性降低了56.5％。文章采用荧光偏光光谱对处理前后的样品进行了分析。 处理后酶样的荧光强度明显大于处理前,在峰值位置其荧光强度增加超过50％,峰位从342 nm移到了346 nm左右,其荧光偏振幅度明显减小。由此推断出木瓜蛋白酶经脉冲电场处理后酶蛋白的α-螺旋结构松散拉伸,分子内部的氨基酸残基暴露于分子表面,并有部分发生离解游离于溶液中,导致活性部位的结构发生变化,最终导致酶失活。     

空气呼吸模式CO2激光等离子体光谱观察

为了了解采用脉冲CO₂激光推进空气呼吸模式时光船参数等对产生等离子体的影响，介绍了利用实验室自行研制的紫外预电离TEA CO₂激光器进行的激光等离子体实验。实验采用底面直径为60mm、焦距为5mm和10mm的抛物面光船。介绍了空气呼吸模式激光等离子体的谱和明显的特征谱线，以及等离子体的时间演化过程。结果表明：空气呼吸模式等离子体的持续时间约为20μs，在6μs左右时信号强度达到最大值；激光脉冲作用后，信号迅速衰减；10mm光船产生的等离子体信号峰值和持续时间均略长于5mm光船的。     

All-Optical RZ-to-NRZ Format Conversion with a Tunable Fibre Based Delay Interferometer

All-optical format conversion from return-to-zero （RZ） to non-return-to-zero （NRZ） is demonstrated with temperaturecontrolled all-fibre delay interferometer （DI） at 20 Gb/s. The operation principle is theoretical analysed with the help of numerical simulation and spectra analysis. Theoretical analysis results are consistent well with the experimental results. The format conversion can be achieved with power penalty of 0.54 dB and with output extinction ratio 20 dB.     

Local Modulation of Double Electromagnetically Induced Transparency Spectrum

The double electromagnetically induced transparency induced by two coupling fields can be realized in a fourlevel tripod-type atom. Such double transparency spectra can be locally modulated by using the weak coherent fields to perturb the coupling transitions. These investigations within this scheme can be independent of Doppler broadening by properly orienting these fieds.     

Manipulation of Particles with Counter-Propagating Evanescent Waves

Two counter-propagating evanescent beams are used to align and manipulate polystyrene particles on a prism surface. Since the radiation pressure transferred laterally from the evanescent wave is negated on both sides, particles can be stably aligned. By projecting a circular and a linear beam spot onto the interface, both multiple and single arrays of particles are achieved. Arrays of particles trapped on the interface can be easily moved adjusting the intensity of incident beams on either side. We also simulate electromagnetic distribution of scattering light that is converted from the evanescent wave using the FDTD method. The results show that scattering light converts from an evanescent wave propagating through a particle array and has a distance longer than that propagating from a normal evanescent wave.     

Further Acceleration of MeV Electrons by a Relativistic Laser Pulse

With the development of photocathode rf electron gun, electrons with high-brightness and mono-energy can be obtained easily. By numerically solving the relativistic equations of motion of an electron generated from this facility in laser fields modelled by a circular polarized Gaussian laser pulse, we find the electron can obtain high energy gain from the laser pulse. The corresponding acceleration distance for this electron driven by the ascending part of the laser pulse is much longer than the Rayleigh length, and the light amplitude experienced on the electron is very weak when the laser pulse overtakes the electron. The electron is accelerated effectively and the deceleration can be neglected. For intensities around 10¹⁹ W•μm²/cm², an electron's energy gain near 0.1 GeV can be realized when its initial energy is 4.5 MeV, and the final velocity of the energetic electron is parallel with the propagation axis. The energy gain can be up to 1 GeV if the intensity is about 10²¹ W•μm²/cm². The final energy gain of the electron as a function of its initial conditions and the parameters of the laser beam has also been discussed.