Tm-Doped Fibre Laser Pumped Cr^2＋：ZnSe Poly-Crystal Laser

Demonstrations of cw lasing in Cr^2＋：ZnSe poly-crystal are reported. The laser consists of a 1.7-mm-thick Cr^2＋ ：ZnSe poly-crystal disc pumped by a Tin-silica double-clad fibre laser at 2050nm. Using a concave high- reflection mirror with a radius of curvature of 500mm as the rear mirror, the laser delivers up to 1030mW of radiation around 2.367μm.     

Polarization and Angular Distribution of Ll X-Ray Following Inner-Shell 2p3/2 Photoionization of Magnesium-Like Ions

The inner-shell 2pa/2 photoionization and the subsequent decay of Mg-like Fe^14＋, Cd^36＋, W^62＋ and U^80＋ ions are studied theoretically within the multiconfiguration Dirac-Fock method and the density matrix theory. Special attention is paid to exploring the influence of the non-dipole terms which arise from the multipole expansion of the electron-photon interaction in the photoionization process. The results show that the non-dipole contribution to the total cross section, the magnetic sublevels cross section of the photoionization process, the degree of linear polarization and angular distribution of the subsequent characteristic x-ray radiation become more important with the increase of photons energy and atomic nuclear Z. Especially for the cross section and the degree of linear polarization, the non-dipole contribution arrives at 50% for U^80＋ at four time energy threshold units. However, for the angular distribution, the maximum contribution does not exceed 4%, even for U^80＋ ions.     

矿化剂浓度和温度对水热法合成氧化锌晶体形态的影响

采用水热法，通过改变矿化剂浓度和温度合成了具有不同形态的氧化锌晶体。在较低的温度(350℃)，填充度为35％。矿化剂KOH浓度小于2mol／L时，只合成了氧化锌微晶。当矿化剂KOH浓度大于3mol/L时，合成出多种形态氧化锌晶体，大的晶体达到几十到几百微米，小晶体仅几微米。当矿化剂KOH浓度从4mol／L增加到5mol／L时，晶体的大小没有明显改变。在高矿化剂条件下合成的晶体显露完整的晶面结构，主要显露柱面m{1010}、锥面p{1011}、负极面O面{0001}，有时也显露Zn面{0001}。晶体表面出现斑坑，显示出晶体的表面缺陷。在430℃，填充度为35％，矿化剂KOH浓度大于1．5moL／L时。合成了多种形态氧化锌晶体，大晶体有几十到几百微米，小晶体仅几微米。当矿化剂KOH浓度为2mol／L，KBr浓度为lmol/L时，最大晶体的长度达到1mm。矿化剂KOH浓度为4mol/L时，晶体没有增大。粒度较大的氧化锌晶体形状多为六棱锥体，显露柱面m{1010}、锥面p{1011}、负极面O面{0001}。晶体表面光滑，完整性好。质量高于350℃时合成的晶体。     

SBN晶体中Eu^3＋激光态^5D0的无辐射跃迁

通过测量＾５Ｄ０→７Ｆ２发射带的荧光寿命与晶体温度的依赖关系，研究了Ｅｕ＾３＋激发态＾５Ｄ０的无辐射跃迁。结果表明，＾５Ｄ０→Ｆ２带的温度淬灭效应主要是由于电荷转移态的最低能量太低，＾５Ｄ０态易被热激活至电荷转移，然后通过电荷转移无辐射驰豫至＾７Ｆ０态。     

Charge state effect on the K-shell ionization of iron by xenon ions near the Bohr velocity

Fe K-shell ionization cross sections induced by 2.4–6.0 MeV Xe20+are measured and compared with different binaryencounter-approximation(BEA)models.The results indicate that the BEA model corrected both by the Coulomb repulsion and by the effective nuclear charge(Zeff)agrees well with the experimental data.Comparison of Fe K-shell X-ray emission induced by 5 MeV xenon ions with different initial charge states(20+,22+,26+,30+)verifies the applicability of the effective nuclear charge(Zeff)correction for the BEA model.It is found that Zeffcorrection is reasonable to describe direct ionization induced by xenon ions with no initial M-shell vacancies.However,when the M shell is opened,the Zeffcorrected BEA model is unable to explain the inner-shell ionization,and the electron transfer by molecular-orbital promotion should be considered.     

级联二阶非线性铌酸锂全光开关的研制

以基于准位相匹配和频与差频级联二阶非线性[X^(2)：X^(2)]基础上的全光开关的理论分析作指导,进行了周期极化铌酸锂晶体(PPLN)和退火质子交换光波导(APE)的实验制备,利用所研制的PPLN-APE器件,以自行研制的工作波长为1．54μm的被动调Q掺钴铝酸镁激光器作为控制光源,以工作波长为1．5μm的连续二极管激光器为信号光源进行了级联二阶非线性全光开关实验。当控制光峰值功率为3kw,信号光功率为1mW时,实现13％的开关效率,分析了进一步提高全光开关性能的途径。     

富于开拓 锐意创新——记学部委员闵乃本教授

 1991年秋,一位富于开拓、锐意创新的学者,应聘担任了“八五”期间国家基础性研究重大关键项目之一的“光电功能材料的结构、性能、分子设计及制备过程”项目的首席科学家.他就是南京大学物理系教授闵乃本先生.他今年57岁,是我国自己培养的优秀中年科学家.1959年,他毕业于南京大学物理系,后留校任教,师从我国著名物理学家冯端教授.长期以来,闵乃本教授致力于晶体物理学的研究,尤其在晶体缺陷、晶体生长以及晶体物理性能等领域作出了许多开创性的工作.在他30多年的科研生涯中,取得了一系列令人瞩目的卓越成就.     

RPIC/ICP-MS测定水中的Cr(Ⅲ)和Cr(Ⅵ)

建立了反相离子对色谱-电感耦合等离子体-质谱(RPIC/ICP-MS)联用技术测定水中痕量三价铬Cr(Ⅲ)和六价铬Cr(Ⅵ)的分析方法。通过对流动相的组成、浓度、pH值等色谱条件的实验,确定当流动相组成为0.25mmol.L-1乙二胺四乙酸二钠和2mmol.L-1四丁基氢氧化铵,5%(V/V)甲醇,pH=7.0时,成功分离了Cr(Ⅲ)和Cr(Ⅵ)离子。ICP-MS测定时选用碰撞反应接口技术(CRI)消除40Ar12C+与35Cl16OH+对52Cr+的质谱干扰,Cr(Ⅲ)和Cr(Ⅵ)的检出限分别为0.50、0.34μg.L-1,RSD<10%(n=5)。应用于湖北黄冈、黄石、襄阳等地企业废水中Cr(Ⅲ)和Cr(Ⅵ)含量的测定,加标回收率为86.1%—100.1%。与分光光度法比对,实验证明本方法能克服用分光光度法测定水中六价铬由样品本身带来的干扰。