ZnCdTe-ZnTe多量子阱的光泵受激发射

本文报导了ＺｎＣｄＴｅ－ＺｎＴｅ多量子阱的受激发射机理．阈值时（Ｊｔｈ）受激发射峰相对于激子吸收峰的能量差（１９ｍｅＶ）与激子束缚能接近．激发光强度在３Ｊｔｈ～４．８Ｊｔｈ之间变化时，该能量差随激发光强度的变化规律与激子—激子散射过程的理论结果符合得很好，从而把该材料在上述激发光强内的受激发射机理归结为激子－激子散射过程     

浅杂质注入LEC半绝缘GaAs γ射线辐照缺陷

用深能级瞬态谱（ＤＬＴＳ）和恒温电容瞬态等技术研究了浅杂质注入ＬＥＣ半绝缘ＧａＡｓ的γ射线辐照缺陷。在Ｂｅ－Ｓｉ共注的ＬＥＣ半绝缘ＧａＡｓ中，γ射线辐照引入一电子陷阶Ｅ₂，并且大大增强了原有的Ｅ₀₁（０．２９８）和Ｅ₀₂（０．３４１）等缺陷，同时明显地瓦解了原有的少子陷阱Ｈ₀₃。在单纯注Ｓｉ的ＬＥＣ半绝缘ＧａＡｓ中，γ射线辐阳引进了Ｅ＇₀₁（０．２１６），Ｅ＇₀₂（０．３４１），Ｅ＇₂，Ｅ＇₄和Ｅ＇₅（０．６０８）等缺陷。其中Ｅ₀₁和Ｅ＇₀₁是新发现的和γ辐照有关的ＧａＡｓ缺陷。和低阻衬底同质外延ＧａＡｓ相比，Ｂｅ－Ｓｉ共注ＬＥＣ半绝缘ＧａＡｓ具有较低的γ射线辐照缺陷引入率，与此相反，单纯注Ｓｉ的ＬＥＣ半绝缘ＧａＡｓ具有较高的γ射线辐照缺陷的引入率。 关键词：     

e~＋e~－湮没中L＝1激发态重子的产生比例

用一个简化模型概括的低激发态重子主要衰变分支比和我们在文献［２］中给出的基本关系，得出Ｌ＝１激发态重子对∑（１３８５），∑＋，（１５３０）和的衰变贡献，进而用γ共振能量下的实验值Ｒ１＝（１５３０），Ｒ２＝∑（１３８５）／∑和Ｒ３＝∧（１５２０）／∑（１３８５）作输入，估算了Ｌ＝１的各激发态重子的产生比例．     

多孔硅表面钝化对其发光性能的影响

报道多孔硅（ＰＳ）的表面钝化对其光致发光（ＰＬ）和电致发光（ＥＬ）的影响,ＰＬ和ＥＬ谱表明,经钝化处理的ＰＳ的ＰＬ和ＥＬ强度明显增强,且发光峰位较大蓝移;存放实验表明,经钝化处理的ＰＳ的ＰＬ和ＥＬ发光强度和发光峰位具较好的稳定性;Ｉ～Ｖ曲线显示,经钝化处理的ＰＳ发光器件具有较低的劝电压,结结果表明：用钝化处理的方法是几ＰＬ和ＥＬ强度和稳定性及改善器件性能的有效途径。     

光学非线性LB膜的时间稳定性与光致漂白效应的关系

用光学二次谐波产生（ＳＨＧ），拉曼散射和紫外－可见吸收光谱等方法研究了偶氮，苯腙及半花菁三种有机染料Ｚ型Ｌａｎｇｍｕｉｒ－Ｂｌｏｄｇｅｔｔ（ＬＢ）多层膜的时间稳定性问题，发现：随着放置时间的推延，其中ＬＢ膜的二次谐波产生信号强度下降，然后逐渐达到稳定；在高压汞灯光照射下，粉末样品中Ｎ＝Ｎ（偶氮），Ｃ＝Ｎ（苯腙），Ｃ＝Ｃ（半花菁）键伸缩振动所对应的拉曼峰强度以及这三类染样在ＬＢ膜样品中对所应的生色团     

光泽精－H_2O_2－KCl中性非缓冲体系电生化学发光行为及机理研究

本文用自制的电生化学发光仪，选择光泽精－Ｈ２Ｏ２－ＫＣｌ中性（非缓冲）水溶液作为电生化学发光（ＥＣＬ）体系。该体系具有比前人所研究的ＬＵＣ－Ｏ２的碱性水溶液的ＥＣＬ体系灵敏度高，ＥＣＬ强度大，还原产物不易沉积在阴极上影响发光及所发的ＥＣＬ不与传统的ＣＬ相混淆的优点。光泽精浓度在８×１０－５～４×１０－８ｍｏｌ．Ｌ－１范围内与ＥＣＬ强度成正比，光泽精检测限为１０－９ｍｏｌ．Ｌ－１。此外还对该体系的测定条件及机理进行了研究，并提出了可能的机理。     

光学二次谐波混沌的控制

用方波控制法对光学二次谐波系统的混沌进行了有效的控制,通过对系统的最大李雅普诺夫指数（ＭＬＥ）的分析,给出了确定可控参数区的方法,证明适当的方波冲激强度和持续时间以及间隔时间可以使混沌得到稳定的控制,被控制系统的轨道是初始系统混沌吸引子中的不稳定周期轨道。     

最新的Van Hove LEED程序库

用低能电子衍射（ＬＥＥＤ）强度－电子能量曲线（Ｉ－Ｖ ｃｕｒｖｅ）确定晶体表面结构是目前国际上广泛采用的一种方法。由于理论计算的复杂性，充分利用世界上现有的计算程序已显得十分必要，本文对Ｖａｎ Ｈｏｖｅ的ＬＥＥＤ程序库及其应范围和特点作一简单的介绍。     

β延迟质子发射先驱核~(87)Mo

实验利用ｐ－γ符合测量技术研究了８７Ｍｏ的衰变，发现８７Ｍｏβ延迟发射的质子布居到８６Ｚｒ的第一（２＋）、（４＋）和（６＋）激发态的强度仅为总的延发质子衰变强度的（１１±６）％、（２±１）％和（２±１）％，以此修正了前人的结果。     

双波长β修正光度法测定铁－二甲酚橙络合物特性参数

双波长β修正光度法是经过大量实验证实的一种有效的痕量金属分析方法，它能完全消除络合物反应中过量络合剂的影响，计算出络合产物的其实吸光度，进而建立络合物特征参数：组成比γ、真实摩尔吸光系数εｐ的计算方程。本文对Ｆｅ（Ⅲ）与二甲酚橙（ＸＯ）络合显色体系进行实验研究，结果表明其组成比γ＝１∶１，εｐ＝１．６３×１０４（Ｌ／ｍｏｌ．ｃｍ）。     

自泵浦位相共轭反射的实验研究

本文通过检测BaTiO_3晶体的二波耦合增益系数P和自泵浦位相共轭反射率R对随入射角的变化关系,经过理论分析指出R的角度依赖性是P的角密依赖性的结果;详细地解释了全内反射自泵浦位相共轭的双区域耦合理论,指出位相共轭输出的频移特性是泵浦光在双区域间“振荡”的结果;并解释了自泵浦形成的阈值特性。     

A novel technique for laser diode to single mode fiber coupling

An optical fiber coupler based on the semi-linear passive phase conjugate mirror is analyzed. The threshold coupling strength is determined from theoretical considerations. An estimate of 50% for the overall coupling efficiency is made, assuming there is good mode matching between the light incident on the fiber and the propagating mode. The coupler exhibits a high degree of alignment insensitivity allowing for simple manufacture.     

Entropy evolution properties in a system of two entangled atoms interacting with light field

In this paper, we use the field entropy as a measurement of the degree of entanglement between the light field and the atoms of the system which is composed of two dipole—dipole interacting two-level atoms initially in an entangled state interacting with the single mode coherent field in a Kerr medium. The influence of the coupling constant of dipole—dipole interaction between atoms and the coupling strength of the Kerr medium with the light field and the intensity of the light field on the field entropy are discussed by numerical calculations. It is shown that when the coupling strength of the Kerr medium with the light field is large enough, and the light field is strong, the degree of entanglement between the atoms with the light field becomes weaker. The degree of entanglement only changes slightly with the change of the coupling constant of dipole—dipole interaction between atoms.     

Synchronization experiments with an atmospheric global circulation model

Synchronization in a chaotic system with many degrees of freedom is investigated by coupling two identical global atmospheric circulation models. Starting from different initial conditions, the two submodels show complete synchronization as well as noncomplete synchronization depending on the coupling strength. The relatively low value of the coupling strength threshold for complete synchronization indicates the potential importance of synchronization mechanisms involved in climate variability. In addition, the results suggest synchronization experiments as a valuable additional method to analyze complex dynamical models, e.g., to estimate the largest Lyapunov exponent. (c) 2001 American Institute of Physics.     

Ratio Between Sensitive Strength to Light Information and Coupling Strength Affects Entrainment Range of Suprachiasmatic Nucleus

The suprachiasmatic nucleus (SCN), an endogenous clock in the brain of the mammals, regulates the physiological and behavioral activities according to the natural 24 h light-darkness cycle. Animals can also entrain themselves to non 24 h light-darkness cycles. The range of the periods which the animal can entrain to is called entrainment range. Previous studies have found that the entrainment range depends on the coupling strength and the sensitive strength to the light for the SCN neurons. However, the effect of the interplay between these two strengths on the entrainment range has not been examined. In the present study, we examine the effect of the ratio of the sensitive strength to the coupling strength on the entrainment range. We find that there is a parabolic-like relationship between the entrainment range and the ratio, and the largest entrainment range is obtained with a suitable ratio. Interestingly, the value of this suitable ratio is related to the comparison in the intrinsic amplitudes between the light information sensitive neurons and the light information insensitive neurons. Our finding will shed light on the interplay between the sensitive strength to the light information and the coupling strength, and the understanding for the diversity of the entrainment range among various species.     

Resonance tongues in a system of globally coupled FitzHugh-Nagumo oscillators with time-periodic coupling strength

We investigate the dynamics of a population of globally coupled FitzHugh-Nagumo oscillators with a time-periodic coupling strength. While for synchronizing global coupling, the in-phase state is always stable, the oscillators split into several cluster states for desynchronizing global coupling, most commonly in two, irrespective of the coupling strength. This confines the ability of the system to form n:m locked states considerably. The prevalence of two and four cluster states leads to large 2:1 and 4:1 subharmonic resonance regions, while at low coupling strength for a harmonic 1:1 or a superharmonic 1:m time-periodic coupling coefficient, any resonances are absent and the system exhibits nonresonant phase drifting cluster states. Furthermore, in the unforced, globally coupled system the frequency of the oscillators in a cluster state is in general lower than that of the uncoupled oscillator and strongly depends on the coupling strength. Periodic variation of the coupling strength at twice the natural frequency causes each oscillator to keep oscillating with its autonomous oscillation period.     

Compilation of coupling constants and low-energy parameters

The double-pomeron coupling strength in the dual resonance model is found in both the inclusive and exclusive regions by comparison with experiments. Double-pomeron coupling occurs in inclusive experiments in the Mueller diagram for the central plateau region. Its strength can also be bounded from its non-observation in the two-particle to four-particle exclusive experiments. The dual resonance model is used to perform the analytic continuation of a six-point amplitude between these regions. The results show that the coupling strength for two forward pomerons in the exclusive region must be less than $\text{1}\text{300}$ of that in the inclusive region. This is experimental evidence for substantial forward double-pomeron decoupling in exclusive processes.     

Properties unique in nuclei far from β stability line

Nucleons with very small binding energies present in nuclei far from the β stability line produce a unique shell structure, which leads to the disappearance of traditional magic numbers or to the creation of new magic numbers and new deformation regions. We study the shell structure in terms of the variation of two important ingredients, the kinetic energy and the spin-orbit splitting, as a function of the orbital angular momentum ℓ, when binding energies of neutrons decrease towards zero. It is also shown that for low-lying threshold strength, a negative sign is possible for the polarization charge coming from the coupling of one-particle to isoscalar shape oscillations. Received: 1 May 2001 / Accepted: 4 December 2001     

Masterequation and Fokker-Planck equation for coupled modes of a laser with axial magnetic field

The distribution function for two circularly polarized modes in a laser with axial magnetic field is calculated. If the resonator has different damping constants for waves polarized in different directions, we find a coupling between the modes. To describe this coupling it is necessary to couple both modes to the same heatbath. Starting from a masterequation describing the damping of the atoms and the light field, we may transform the masterequation to a Fokker-Planck equation by introducing a quasi distribution function. By eliminating the atomic variables adiabatically we find a Fokker-Planck equation for the light field variables only. The solution of the Fokker-Planck equation is given in the stationary case above threshold and in the non stationary case below threshold.     

Loss enhanced phase locking in coupled oscillators

Phase locking, which is achieved by transferring some energy from one oscillator to the others, strongly depends on the coupling strength between the oscillators. Typically, the coupling strength must be above a certain threshold in order to achieve phase locking. Here we show how this threshold can be significantly reduced when phase-dependent losses are introduced into the oscillators. Specifically, the coupling strength can be reduced by at least an order of magnitude, thereby substantially decreasing the needed transfer of energy between oscillators. The resulting enhancement of phase locking does not only influence the laser research area, but also affects many other areas that involve coupled ensembles.