MOCVD生长的II-VI族化合物固溶体组分的热力学分析.2.Hg（1-x）CdxTe体系

对MOCVD生长Hg_(1-x)Cd_xTe进行了热力学分析.所用的起始原材料为Hg、DM-Cd和R_2Te.计算结果一方面表明CdTe优先并入倾向使得在通常的DAG工艺中x值非常不易控制.另一方表明即使在Hg存在的情况下,也可以沉积几平纯的CdTe,这对实现IMP工艺非常有利,计算结果还表明II/VI比对HgCdTe的组分控制起着关键性的作用.在DAG工艺中,较低的II/VI比可以改善对x值的控制能力,LMP-DAG工艺是降低II/VI比的较好途径.还计算了生长温度和反应室压力对固相组分的影响以及LMP-DAG工艺中生长温度与HgCdTe组分对最低汞分压的影响.

Syntheses and structures of Na-2[Zn-II(ida)(2)].7H(2)O and Na-4[Hg-II(nta)(2)].7H(2)O

The title complexes were synthesized and the crystal structures of their salts were determined by single-crystal X-ray structure analyses. Na-2[Zn-I(ida)(2)]. 7H(2)O: Triclinic, P1, a=0.523 4(2) nm, b=0.897 10(10) nm, c=1.069 10(10) nm, alpha=85.910(10)degrees, beta= 76.380(10)degrees, gamma=83.52(2)degrees, V=0.484 2(2) nm(3), Z=1. The complex anion [Zn-I (ida)(2)](2-) has a pseudo-octahedral structure in which the two N atoms: are in a trans configuration. Na-4[Hg-I(nta)(2)]. 7H(2)O: Monoclinic, C-c, a = 1.795 0(4) nm, b = 0.892 9(2)nm, c = 1.575 4(2) nm, beta = 92.78 (3)degrees, V = 2.526 2(9) nm(3), Z = 4. The complex anion [Hg-I (nta)(2)](4-) has a pseudo-bicapped-octahedral structure in which the two N atoms are in a trans configuration.

基于EPC Class-1 Gen-2标准的防冲突算法与改进

针对RFID读写器识别多标签过程中出现的冲突问题,研究并实现了EPC Class-1 Gen-2标准中的防冲突算法,即时隙随机算法(SR算法),同时针对SR算法的不足提出改进算法。改进算法采用不避让冲突时隙的处理方式,降低了由时隙的随机选取所导致的标签间冲突的概率。实验结果证明,改进后的算法在通信次数和吞吐率方面均优于原算法,有效提高标签识别效率。

A new protein structure of P-II class snake venom metalloproteinases: it comprises metalloproteinase and disintegrin domains

A new metalloproteinase-disintegrin, named Jerdonitin, was purified from Trimeresurus jerdonii venom with a molecular weight of 36 kDa on SDS-PAGE. It dose-dependently inhibited ADP-induced human platelet aggregation with IC50 of 120 nM. cDNA cloning and sequencing revealed that Jerdonitin belonged to the class II of snake venom metalloproteinases (SVMPs) (P-II class). Different from other P-II class SVMPs, metalloproteinase and disintegrin domains of its natural protein were not separated, confirmed by internal peptide sequencing. Compared to other P-II class SVMPs, Jerdonitin has two additional cysteines (Cys219 and Cys238) located in the spacer domain and disintegrin domain, respectively. They probably form a disulfide bond and therefore the metalloproteinase and disintegrin domains cannot be separated by posttranslationally processing. In summary, comparison of the amino acid sequences of Jerdonitin with those of other P-II class SVMPs by sequence alignment and phylogenetic analysis, in conjunction with natural protein structure data, suggested that it was a new type of P-II class SVMPs. (C) 2003 Elsevier Inc. All rights reserved.

Two Mn(2)(II)Ln(4)(III) (Ln = Gd, Eu) hexanuclear compounds of p-tert-butylsulfinylcalix[4]arene

Two 3d-4f heterometallic compounds of p-tert-butylsulfinylcalix[4] arene were synthesized by the solvothermal method and characterized by some hinged double-dumbbell-like subunits in which two perpendicular dumbbell entities were constructed by an in-between isosceles triangle Mn(II)Ln(2)(III), and two tail-to-tail calixarene molecules, and hinged by the lanthanide-sulfinyl group bonding. The magnetic properties of the title compounds were examined.

量纲分析

量纲分析是一门非常值得研究和学习的知识，它是探讨科学规律，解决科学和工程的一个有效的工具。熟练掌握量纲分析应当是科学和技术工作者应有的基本训练。
本书内容包括：量纲分析的基本概念；量纲分析在熟知的力学现象中的应用；量纲分析在某些经典的力学问题中的应用以及郑哲敏先生的研究集体近三四十年中在爆炸力学诸多的应用实例等几个部分。 

假根羽藻不同聚集态捕光色素蛋白复合物（LHC II）的纯化与功能分析

应用温和、非变性的液相色谱层析技术以及蔗糖密度梯度分级分离技术，从假根羽藻类囊体膜直接分离、纯化出5种不同聚集态的光系统II捕光色素蛋白复合物(LHC II)，即LHC II单体、同质三聚体、异质三聚体、寡聚体l和寡聚体2。这种分离、纯化LHC II的方法与传统的等电聚焦(IEF)电泳分离方法相比，具有蛋白质提取条件温和，纯化的蛋白质样品纯度高且数量大等优点，为进一步研究LHC II分子的晶体结构和功能创造了有利的条件。 SDS-PAGE电泳分析和MALDI-TOF质谱分析结果表明，纯化得到的LHC II单体和同质三聚体都具有一种分子量为24.3 kDa的脱辅基蛋白质，而异质三聚体和两种寡聚体除含有这个脱辅基蛋白外，还含有另一种分子量为23 kDa的脱辅基蛋白。 采用室温吸收光谱、低温荧光光谱及园二色(CD)光谱技术对LHC II单体、同质三聚体、异质三聚体、寡聚体l和寡聚体2内的叶绿素组成以及叶绿索之间的能量传递特性进行分析研究表明，在同一条组成LHC II的脱辅基蛋白多肽链上结合着Chl a二聚体，二聚体内的两个Chl a分子之间存在偶极子相互作用。在这5种LHC II亚复合物中均具有Chl a-Chl a相Chl biChl a→ Chl a能量传递途径，其中同质三聚体表现出最高的能量传递效率，而寡聚体的传能效率大大低于单体和三聚体，同时出现Chl a的淬灭现象。当LHC II脱辅基蛋白质高度聚集形成寡聚体时，其蛋白质上结合的Chlb大量减少，引起这两种寡聚体吸能和传能能力的急剧下降。 LHC II单体、同质三聚体、异质三聚体、寡聚体1和寡聚体2的二级结构数据表明，自由堆积的脱辅基蛋白的二级结构以8．折叠构象为主，当LHC II蛋白质有序聚集形成三聚体时，可能每条蛋白质多肽链上的叶绿素结合区域形成两个跨膜a-螺旋，对称排列在脂双层膜内，而非叶绿素结合区则形成一条跨膜a-螺旋。当LHC II蛋白质高度聚集形成寡聚体 时，LHC II蛋白质的二级结构似乎对其上结合着的叶绿素的影响不大，而LHC II寡聚体内蛋白质的高密度聚集引起的更高级的蛋白质相互之间的空间结构可能对叶绿素的影响起主要作用，特别是破坏Chlb结合位点。 依据上述的实验结果推测在类囊体膜内，LHC II可能通过其脱辅基蛋白聚集形式的转换，调控其光能吸收和激发能传递的过程和效率。

HLA-DRB1 allele polymorphisms in genetic susceptibility to esophageal carcinoma

AIM: To probe into the genetic susceptibility of HLA-DRB1 alleles to esophageal carcinoma in Han Chinese in Hubei Province. METHODS: HLA-DRB1 allele polymorphisms were typed by polymerase chain reaction with sequence-specific primers (PCR-SSP) in 42 unrelated patients with esophageal cancer and 136 unrelated normal control subjects and the associated HLA-DRB1 allele was measured by nucleotide sequence analysis with PCR.SAS software was used in statistics. RESULTS: Allele frequency (AF) of HLA-DRB1*0901 was significantly higher in esophageal carcinoma patients than that in the normal controls (0.2500 vs0.1397, P=0.028, the odds ratio 2.053, etiologic fraction 0.1282). After analyzed the allele nucleotide sequence of HLA-DRB1*0901 which approachs to the corresponded exon 2 sequence of the allele in genebank. There was no association between patients and controls in the rested HLA-DRB1 alleles. CONCLUSION: HLA-DRB1*0901 allele is more common in the patients with esophageal carcinoma than in the healthy controls, which is positively associated with the patients of Hubei Han Chinese. Individuals carrying HLA-DRB1*0901 may be susceptible to esophageal carcinoma.

Optimization of VI/II pressure ratio in ZnTe growth on GaAs(001) by molecular beam epitaxy

ZnTe epilayers were grown on GaAs(0 0 1) substrates by molecular beam epitaxy (MBE) at different VI/II beam equivalent pressure (BEP) ratios (R-VI/II) in a wide range of 0.96-11 with constant Zn flux. Based on in situ reflection high-energy electron diffraction (RHEED) observation, two-dimensional (2D) growth mode can be formed by increasing the R-VI/II to 2.8. The Te/Zn pressure ratios lower than 4.0 correspond to Zn-rich growth state, while the ratios over 6.4 correspond to Te-rich one. The Zn sticking coefficient at various VI/II ratios are derived by the growth rate measurement. The ZnTe epilayer grown at a R-VI/II of 6.4 displays the narrowest full-width at half-maximum (FWHM) of double-crystal X-ray rocking curve (DCXRC) for (0 0 4) reflection. Atomic force microscopy (AFM) characterization shows that the grain size enlarges drastically with the R-VI/II. The surface root-mean-square (RMS) roughness decreases firstly, attains a minimum of 1.14 nm at a R-VI/II of 4.0 and then increases at higher ratios. It is suggested that the most suitable R-VI/II be controlled between 4.0 and 6.4 in order to grow high-quality ZnTe epitaxial thin films.

铕（II）等低价稀土离子在氧化物基质中光谱特征及其变化规律

近年来，围绕低价稀土离子开展的研究工作越来越多，尤其重视铕(II)、钐（II）和镱(II)的研究，以期获得短波可调固体激光晶体或高效率发光材料。由于4f~n到4f~(n-1)5d'组态的d-f跃迁是属于宇称允许的跃迁，所以它的发射要比4f~n壳层内的受迫电偶极跃迁强得多。这可以保证对泵浦的有效吸收，提高光泵效率。而4f~n组态内部的f-f锐线发射可以实现激光振荡，有利于提高储能，降低阀值。所以深入了解4f~n和 4f~(n-1)5d'体系在基质晶场中的行为以及基质环境对稀土离子发光特征的影响，对于寻找和设计新的激光和发光材料有着极为重要的意义。 本文从理论上讨论了晶场效应和化学键性质对铕(II)、钐(II)等稀土离子发光性质的影响。采用高温固相反应的方法合成了一系列铕(II)、钐(II)激活的氧化物基质荧光材料。结合光谱实验数据建立了晶格环境对铕(II)的 4f~65d'能级影响的表观模型和定量计算公式。为了研究4f~65d'激发态的性质，我们采用改进的Slater法计算了铕(II)和配体氧的有关轨道能量。利用静电晶场模型讨论了4f~65d'能带劈裂幅度(△E)与Eu-O键距(R)的关系，量子化学计算表明5d能级在晶场中的劈裂(△E)与R~5成反比。碱金属和碱七金属磷酸盐基质中铕的光谱数据证实了上述结论。在该基质中铕的4f~65d'能带的劈裂幅度随Eu-O键距增加而变小。在MeSO_4:Eu~(2+) (Me = Ca, Sr，Ba)中，随碱七金属离子半径增大，其发射和激发截止波长均有规律地向短波区移动。这是由于当铕(II)占据较大半径阳离子格位时，将受到较小的晶场影响。其体系的荧光寿命数据也证实了这一点。运用统计热力学原理讨论了4f~(n-1)5d'与 4f~n激发态能级的相对位置对低价稀土离子d-f和f-f跃迁发射的影响。在Ba_(1-x)Mg_(1+x)(SO_4):Eu~(2+)中，适当增大Mg~(2+)离子含量，线一带两种发射强度比R = I (f-f)/I(d-f) 明显增大。Ba_(0.4)Mg_(1.6)(SO_4)_2:Eu~(2+)的f-f锐线发射强度最大。在Ba_(1-x)Sr_xMg(SO_4)_2:Eu~(2+)中，铕(II)的f-f强度随x增大而变小，d-f发射峰则随x增加而发生红移。运用“电子云扩展效应”和鲍林化学键原理解释了，在Na_(3-x)(PO_4)_(1-x)(SO_4)_x:Eu~(2+)和Na_(2-x)CaSi_(1-x)P_xO_4:Eu~(2+)体系中，随X值在固溶区内变大，铕(II)的发射光谱逐渐移向短波区的现象。为了研究稀七离子的取代格位对其光谱性质的影响，我们合成了K_2Mg_2(SO_4)_3:Eu~(2+)单晶化合物。并经四圆衍射仪解出了结构。铕(II)在单晶中占据Mg_1~(2+)格位，与KMgF_3:Eu~(2+)相比，它将受到更强的晶场作用使4f~65d'能带劈裂幅度变大，又通过计算可知，Eu-O键的共价性比Eu-F键更强，因而在K_2Mg_2(SO_4)_3中Eu~(2+) 4f~65d'重心更低一些。综上所述，K_2Mg_2(SO_4)_3:Eu~(2+)的发射能级(E_(em)~m)要比KMgF_3:Eu~(2+)的发射能级更低。光谱实验数据证实了这一结论。用245 nm激发， K_2Mg_2(SO_4)_3:Eu~(2+)发兰光，最大中心处于400 nm。而KMgF_3:Eu~(2+)发紫色或近紫外光(E_(em)~m = 363 nm)，并且在后者是观察到Eu~(2+)离子的f-f跃迁锐线发射。采用高温氢气还原法制备了SmF_2和SmCl_2作为离子激活源。钐(II)激活的硫酸盐材料的荧光光谱数据表明，在室温条件下该基质中钐(II)的荧光光谱均为4f~55d' → 4f~6跃迁的宽带发射。论文对铕(II)，钐(II)等低价稀土离子的4f~(n-1)5d'激发态性质和稀七离子在基质中的格位取代以及电荷补偿效应也作了较为详细的讨论。