Determination of the tilt and twist angles of curved GaN layers by high-resolution x-ray diffraction

The full-width at half-maximum (FWHM) of an x-ray rocking curve (XRC) has been used as a parameter to determine the tilt and twist angles of GaN layers. Nevertheless, when the thickness of GaN epilayer reaches several microns, the peak broadening due to curvature becomes non-negligible. In this paper, using the (0 0 l), l = 2, 4, 6, XRC to minimize the effects of wafer curvature was studied systematically. Also the method to determine the tilt angle of a curved GaN layer was proposed while the Williamson-Hall plot was unsuitable. It was found that the (0 0 6) XRC-FWHM had a significant advantage for high-quality GaN layers with the radius curvature of r less than 3.5 m. Furthermore, an extrapolating method of gaining a reliable tilt angle has also been proposed, with which the calculated error can be improved by 10% for r < 2 m crystals compared with the (0 0 6) XRC-FWHM. In skew geometry, we have demonstrated that the twist angles deriving from the (2 0 4) XRC-FWHM are in accord with those from the grazing incidence in-plane diffraction (IP-GID) method for significantly curved samples.

Effects of grain size on the mosaic tilt and twist in InN films grown on GaN by metal-organic chemical vapor deposition

The structural property of InN films grown on Ga-face GaN layers by metal-organic chemical vapor deposition has been studied by high-resolution x-ray diffraction. The mosaic tilt and twist are found to be strongly dependent on the surface lateral grain size. The twist decreases with increasing grain size and finally approaches to a constant level. On the other hand, the mosaic tilt increases substantially when the grain size becomes large enough and exceeds the width of step terraces on the GaN surface, showing an important mechanism for the defect generation in the InN/GaN system with large out-of-plane lattice mismatch. (c) 2006 American Institute of Physics.

Double twist in helical polymer "soft" crystals

In natural and synthetic materials having non-racemic chiral centers, chirality and structural ordering each play a distinct role in the formation of ordered states. Configurational chirality can be extended to morphological chirality when the phase, structures possess low liquid crystalline order. In the crystalline states the crystallization process suppresses the chiral helical morphology due to strong ordering interactions, In this Letter, we report the first observation of helical single lamellar crystals of synthetic non-racemic chiral polymers. Experimental evidence shows that the molecular chains twist along both the long and short axes of the helical lamellar crystals, which is the first time a double-twist molecular orientation in a helical crystal has been observed.

Expression of a twist-related gene, Bbtwist, during the development of a lancelet species and its relation to cephalochordate anterior structures

Mesoderm formation plays a crucial role in the establishment of the chordate body plan. In this regard, lancelet embryos develop structures such as the anteriorly extended notochord and the lateral divertecula in their anterior body. To elucidate the developmental basis of these structures, we examined the expression pattern of a lancelet twist-related gene, Bbtwist, from the late gastrula to larval stages. In late-gastrula embryos, the transcripts of Bbtwist were detected in the presumptive first pair of somites and the middorsal wall of the primitive gut. The expression of Bbtwist was then upregulated in the lateral wall of somites and the notochord. At the late-neurula stage, it was also expressed in the anterior wall of the primitive gut, as well as in the evaginating lateral diverticula. No signal was detected in the left lateral diverticulum when it was separated from the gut, while in the right one, the gene was expressed later during the formation of the head coelom in knife-shaped larvae, and in the anterior part of the notochord in the same larvae. In 36-h larvae, only faint expression was detected in the differentiating notochordal and paraxial mesoderm in the caudal region. These expression patterns suggest that Bbtwist is involved in early differentiation of mesodermal subsets as seen in Drosophila and vertebrates. The expression in the anterior notochord may be related to its anterior expansion. The expression in the anterior wall of the primitive gut and its derivative, the lateral diverticula, suggests that lancelets share the capability to produce a mesodermal population from the tip of the primitive gut with nonchordate deuterostome embryos. (C) 1998 Academic Press.

Vortex dislocation in wake-type flow caused by local spanwise nonuniformity

DNS of spatiotemporal evolution of a wake-type flow is performed. In the incoming flow, a local spanwise nonuniformity in momentum defect is initially imposed. Results show that the spanwise nonuniformity leads to a series of symmetric twist vortex dislocation in downstream of the flow. Vortex line variations and substantial transition of vorticity from spanwise to the streamwise and vertical directions clearly feature the generation of a vortex dislocation and the real vortex linking in the dislocation. Dynamical process and the mechanism responsible for the vortex dislocation are described.

Additional angles to calculate the deformation of RNA helices induced by bulge loops

Bulges are common features of folded RNA structures. The RNA axial kinking caused by bulges has been confirmed by many experiments. Usually, a kinking angle zeta and a bending angle theta are used to describe the kinking and twisting of RNA molecules containing bulges. Here, we present two additional angles (twist angle zeta(1), twist angle zeta(2)) to describe the deformation of RNA helices induced by bulge loops because only two angles (a kinking angle zeta and a bending angle theta) are not enough to define the deformation of RNA induced by bulges. (C) 2002 Elsevier Science B.V. All rights reserved.

Microstructure and strain analysis of GaN epitaxial films using in-plane grazing incidence x-ray diffraction

This paper investigates the major structural parameters, such as crystal quality and strain state of (001)-oriented GaN thin films grown on sapphire substrates by metalorganic chemical vapour deposition, using an in-plane grazing incidence x-ray diffraction technique. The results are analysed and compared with a complementary out-of-plane x-ray diffraction technique. The twist of the GaN mosaic structure is determined through the direct grazing incidence measurement of (100) reflection which agrees well with the result obtained by extrapolation method. The method for directly determining the in-plane lattice parameters of the GaN layers is also presented. Combined with the biaxial strain model, it derives the lattice parameters corresponding to fully relaxed GaN films. The GaN epilayers show an increasing residual compressive stress with increasing layer thickness when the two dimensional growth stage is established, reaching to a maximum level of -0.89 GPa.

Thickness dependent dislocation, electrical and optical properties in InN films grown by MOCVD

InN thin films with different thicknesses are grown by metal organic chemical vapor deposition, and the dislocations, electrical and optical properties are investigated. Based on the model of mosaic crystal, by means of X-ray diffraction skew geometry scan, the edge dislocation densities of 4.2 x 10(10) cm(-2) and 6.3 x 10(10) cm(-2) are fitted, and the decrease of twist angle and dislocation density in thicker films are observed. The carrier concentrations of 9 x 10(18) cm(-3) and 1.2 x 10(18) cm(-3) are obtained by room temperature Hall effect measurement. V-N is shown to be the origin of background carriers, and the dependence of concentration and mobility on film thickness is explained. By the analysis of S-shape temperature dependence of photoluminescence peak, the defects induced carrier localization is suggested be involved in the photoluminescence. Taking both the localization and energy band shrinkage effect into account, the localization energies of 5.05 meV and 5.58 meV for samples of different thicknesses are calculated, and the decrease of the carrier localization effect in the thicker sample can be attributed to the reduction of defects.

Evolution of mosaic structure in InN grown by metalorganic chemical vapor deposition

Mosaic structure in InN layers grown by metalorganic chemical vapor deposition at various temperatures has been investigated by X-ray diffraction (XRD). With a combination of Williamson-Hall measurement and fitting of twist angles, it was found that variation of growth temperature from 450 to 550 degrees C leads to the variation of the lateral coherence length, vertical coherence length, tilt and twist of mosaic blocks in InN films in a, respectively, monotonic way. In particular, mosaic tilt increases whereas mosaic twist decreases with elevating temperature. Atomic force microscopy shows the morphological difference of the InN nucleation layers grown at 450 and 550 degrees C. Different coalescence thickness and temperature-dependent in-plane rotation of InN nuclei are considered to account for the XRD results. (c) 2006 Elsevier B.V. All rights reserved.

The methane hydrate formation and the resource estimate resulting from free gas migration in seeping seafloor hydrate stability zone

It is a typical multiphase flow process for hydrate formation in seeping seafloor sediments. Free gas can not only be present but also take part in formation of hydrate. The volume fraction of free gas in local pore of hydrate stable zone (HSZ) influences the formation of hydrate in seeping seafloor area, and methane flux determines the abundance and resource of hydrate-bearing reservoirs. In this paper, a multiphase flow model including water (dissolved methane and salt)-free gas hydrate has been established to describe this kind of flow-transfer-reaction process where there exists a large scale of free gas migration and transform in seafloor pore. In the order of three different scenarios, the conversions among permeability, capillary pressure, phase saturations and salinity along with the formation of hydrate have been deducted. Furthermore, the influence of four sorts of free gas saturations and three classes of methane fluxes on hydrate formation and the resource has also been analyzed and compared. Based on the rules drawn from the simulation, and combined information gotten from drills in field, the methane hydrate(MH) formation in Shenhu area of South China Sea has been forecasted. It has been speculated that there may breed a moderate methane flux below this seafloor HSZ. If the flux is about 0.5 kg m-2 a-1, then it will go on to evolve about 2700 ka until the hydrate saturation in pore will arrive its peak (about 75%). Approximately 1.47 109 m3 MH has been reckoned in this marine basin finally, is about 13 times over preliminary estimate.

两个冠醚分子在简正坐标分析及NRCC程序在微机上的移植

本文用加拿大国立研究院(National Research Council of Canada) Fuhrer等人编制的FORTRAN语言程序（以下简称NRCC程序），对两个冠醚类化合物进行了简正坐标分析，这两个化合物分子是二氧六环(C_4H_8O_2)和12－冠－4(C_8H_(16)O_4)。作者用Synder和Zerbi提出的一般价力场，计算了二氧六环的36个简正振动频率，精化四次后的结果误差为14.04 cm~(-1)，得到了二氧六环的精化力场和势能分析矩阵；做了12－冠－4－的中红外光谱(3200-5000cm~(-1))。远红外光谱(500-70cm~(-1))和拉曼光谱(3200-50 cm~(-1)，从而归属出12－冠－4的78个简正振动频率实验值；利用二氧六环的精化力场作为初始力场，计算了12－冠－4的简正振动频率，对78个简正振动频率进行了精化计算，精化三次后的结果误差为13.99 cm~(-1)，精化后得到12－冠－4的精化力场和势能分布矩阵；将NRCC程序以BASIC语言移至TRS-80微型机上，对二氧六环进行了计算，结果良好，首次给出二氧六环一般价力场的势能分布。一、对二氧六环的处理 二氧六环分子式C_4H_8O_2，合14个原子，有3N－6＝36个简正振动频率。分子结构系由二个乙氧基(-CH_2-CH_2-O-)单元组成的含有四个碳，两个氧的六元环，平衡态分子为椅式构象，属于C_(2h)点群，36个简正振动频率分为四个对称类Ag、Au、Bg和Bu，分布是：Ag 10个，Bg 8个，Au 9个，Bu9个。二氧六环的分子结构及坐标示意图见28而图5，定义了14个伸缩内坐标，26个弯曲内坐标，6个扭曲内坐标，共46个，C－C键长1.54A，C-O键长1.41 A，C－H键长1.096A，键角都用109°28'。用CART程序（NRCC程序之一）计算二氧六环14个原子的笛卡尔坐标，用GMAT程序（NRCC程序之二）计算其B矩阵和G矩阵，用FPERT程序（NRCC程序之三）计算其简正振动频率、精化力场，计算用一般价力场，引入V矩阵对称化，将46个坐标化为46个（内）对称坐标，10个多余坐标在FPERT程序计算中除去。二、对12－冠－4的处理 12－冠－4分子式C_8H_(16)O_4，含28个原子，共3N－6＝78个简正振动频率，分子结构为四个乙氧基(-CH_2-CH_2-O-)单元组成的含八个碳、四个氧的12元环，自由分子的12－冠－4属于C点群。结构数据引自Groth的X光衍射分数和坐标，自己编制了BASIC语言程度将分数坐标化为笛卡尔坐标，用GMAT程序计算B矩阵和G矩阵，FPERT程序计算78个简正振动频率、精化力场、计算势能分布矩阵，引入U矩阵将92个内坐标化为92个对称坐标，14个多余坐标在FPERT程序中自动除去。三、结果 势能分布矩阵给出分子的振动归属，对这两个冠醚类分子的3N－6个简正振动频率，可以划分为五个振动区域。1．C－H伸缩振动区（3000－2800 cm~(-1)） 在该区中，二氧六环有八个值：2974、2966、2854和2867 cm~(-1)各两个，12－冠－4有16个值：2935、2923、2915和2907 cm~(-1)各两个，2860 cm~(-1)8个，高于2900 cm~(-1)者为反对称伸缩振动，低于2900 cm~(-1)者为对称伸缩振动。2．亚甲基弯曲振动之一(1500-1400 cm~(-1)) 该区的主要振动是亚甲基剪式振动(Scissor)，其它振动小于10％二氧六环在该区有四个频率：1443、1461、1451和1457 cm~(-1)，12－冠－4有八个频率：1466、1450、1450和1405 cm~(-1)各两个。3．亚甲基弯曲振动区二(1400-1200 cm~(-1))该区的主要振动模式为亚甲基的颤动(wag)、卷曲(twist)和摆动(rock)振动，其它振动小于13％。二氧六环在该区有八个频率：1334、1303、1396、1216、1367、1264、1377和1296 cm~(-1)，12－冠－4有十六个频率：1388、1363、……1229 cm~(-1)（其中1288、1307cm~(-1)非简并，其余皆两重简并）。4．环的骨架伸缩振动区(1200-600 cm~(-1))该区振动模式复杂，除环的骨架伸缩振动外，还有亚甲基的wag、twist、rock以及环的骨架弯曲振动，而且这些振动的势能分布值都不小。二氧六环在该区有十一个频率，从1127至610 cm~(-1)，12－冠－4有二十个频率，从1135至184 cm~(-1)且大都是二重简并的。5．低频区(600-50cm~(-1))这两个分子在低频区的势能分布略有差别。二氧六环在该区有五个频率：503、486、427、276和224 cm~(-1)，主要振动模式为骨架弯曲振动和扭曲振动，C－O、C－C的扭曲振动在三个最低频率中分布占10－30％。12－冠－4在该区有18个频率，除570和547cm~(-1)处，都是二重简并的，六个最低频率的振动模式完全属于C－O、C－C键的扭曲振动，其它振动小于10％，所以200 cm~(-1)以下可称为12－冠－4的扭曲振动区，在600－200cm~(-1)之间的12个频率主要是骨架的弯曲振动，也有一定量的亚甲基wag、twist、rock振动。12－冠－4的简正坐标分析尚未有人做过。二氧六环的计算结果与Snyder和Zerbi的分析相吻合，12－冠－4和二氧六环两分子势能分布的相对一致性证明了对12－冠－4的简正坐标分析基本是正确的。本文比较了二分子的力常数和振动频率，探讨了环的大小对振动光谱的影响。四、NRCC程序简介 NRCC程序由CART、GMAT和FPERT三个程序组成，即可联一起运用，亦可分开独立进行运算。该程序功能强，所占内存大，适于大、中型计算机使用。CART程序之名字取自Cartisian Co-or-dinates的前四个字母，功能系由分子结构参数（键长、键角）计算分子内各原子的笛卡尔坐标。GMAT程序之名字取自G matrix的前四个字母，功能系由分子内各原子的笛卡尔坐标，原子质量和内坐标定义计算分子内各原子的坐标交换矩阵B和Wilson振动动能矩阵G。FPERT程序之名字取自F Perturbation的前五个字母，功能系由分子振动功能矩阵G、势能常数即力常数矩阵F计算分子的简正振动频率和势能分布矩阵，再通过实验频率精化势能矩阵F。NRCC程序可对含30个原子、60个内坐标的分子进行简正坐标分析，扩充后容量增大一倍。该程序可选用一般价力场(General Valence Force Field, 简称GVFF)和UBS力场(Urey-Bradley-Shimanouchi Force Field)，简称UBSFF或UBFF)。可选用对称化U矩阵，可自行决定力场精化次数和阻尼常数以限制精化结果的收敛性。五、NRCC程序在TRS－80微型机上移植试尝（该部分曾在第三届长春夏季化学讨论会上宣读）针对NRCC程序占内存空间大、难以在微型机上实现的情况，作者将NRCC程序改编为BASIC语言，改变程序的原来结构，形成一组BASIC语言程序：CART／BAS、GMAT／BAS和VIFR／BAS，改编后的BASIC程序在TRS－80微型机调试通过，TRS－80机字长8位，New Dos系统内存32K。改写后的程序只保持了原程序的基本原理，在内存，语句上改动很大，以适于微型机使用。数据在程序中直接嵌入，利于修改替换，且BASIC语言简单易学，便于操作。CART／BAS程序可计算含30个原子以内的分子的笛卡尔坐标，GMAT／BAS程序可计算含20个原子、45个内坐标的分子的G矩阵，VIFR／BAS程序可计算含15个原子的分子的简正振动频率。利用这组程序，作者以二氧六环分子为例做了一些试尝运算，误差14.4 cm~(-1)，相对误差1.8%，结果较理想。

非洲爪蟾Nkx6.3在原肠运动和神经嵴诱导调控中的功能及爪蟾神经管腹侧图式形成的研究

神经嵴（neural crest）是一类脊椎动物特有的多潜能迁移细胞。这一类细胞历经“表皮—间充质”转换（EMT），与神经管背侧的其它细胞分离，经由不同路线迁移，定位于胚胎外周各处，后分化为不同的细胞类型包括外周神经系统、颅面骨骼系统及色素细胞等。神经嵴的发育是一个多途径多步骤的过程，受多种信号通路及转录因子调控。这些调控因子相互调节形成精密网络，可被划分为三个主要层次类群：分泌性信号分子（BMP、Wnt、FGF、Delta）、神经板边界特异基因（Msx、Pax3/7、 Zic1、Dlx3/5）、神经嵴特异基因（Snail/Slug、AP-2、FoxD3、Twist、Id、cMyc、Sox9/10）。本文第一章主要概述不同组织来源的各种分泌信号在神经嵴诱导中的作用以及他们之间的整合调控。 Nkx6家族蛋白是一类进化上保守的转录因子，在脊椎动物中枢神经系统（CNS)的图式形成和胰腺的发育中有重要作用。在第二章，我们描述了非洲爪蟾中Nkx6家族基因的克隆及其表达图式。与小鼠和鸡中的同源基因类似，爪蟾的Nkx6家族基因在胚胎发育过程中主要表达于中枢神经系统和前部内胚层组织。其中Nkx6.1和Nkx6.2在神经胚期神经板表达重合，晚期都表达于后脑和脊髓的腹侧。Nkx6.3从卵裂期到神经胚早期都表达于非神经外胚层，而尾芽期表达于后脑后部和腮弓。在内胚层中，Nkx6.2在尾芽期表达于底索。在蝌蚪期，Nkx6家族的三个基因分别表达于前部内胚层的衍生物，包括胰腺、胃、食道和肺。 Nkx6.3是最近发现的Nkx6家族新成员，它在爪蟾中的表达与Nkx6.1和Nkx6.2有了较大分歧。在第三章，我们通过功能获得及功能缺失实验来探讨Nkx6.3在爪蟾早期发育中的功能。我们发现原肠期前过量或抑制Nkx6.3表达都会影响胚胎原肠运动的正常进行。我们通过动物帽延伸实验证明Nkx6.3参与了细胞运动。半定量RT-PCR结果显示，Nkx6.3可以调控一些粘附分子的表达。以上结果说明Nkx6.3通过调控粘附分子的转录而参与细胞运动的调控。我们还发神经嵴（neural crest）是一类脊椎动物特有的多潜能迁移细胞。这一类细胞历经“表皮—间充质”转换（EMT），与神经管背侧的其它细胞分离，经由不同路线迁移，定位于胚胎外周各处，后分化为不同的细胞类型包括外周神经系统、颅面骨骼系统及色素细胞等。神经嵴的发育是一个多途径多步骤的过程，受多种信号通路及转录因子调控。这些调控因子相互调节形成精密网络，可被划分为三个主要层次类群：分泌性信号分子（BMP、Wnt、FGF、Delta）、神经板边界特异基因（Msx、Pax3/7、 Zic1、Dlx3/5）、神经嵴特异基因（Snail/Slug、AP-2、FoxD3、Twist、Id、cMyc、Sox9/10）。本文第一章主要概述不同组织来源的各种分泌信号在神经嵴诱导中的作用以及他们之间的整合调控。 Nkx6家族蛋白是一类进化上保守的转录因子，在脊椎动物中枢神经系统（CNS)的图式形成和胰腺的发育中有重要作用。在第二章，我们描述了非洲爪蟾中Nkx6家族基因的克隆及其表达图式。与小鼠和鸡中的同源基因类似，爪蟾的Nkx6家族基因在胚胎发育过程中主要表达于中枢神经系统和前部内胚层组织。其中Nkx6.1和Nkx6.2在神经胚期神经板表达重合，晚期都表达于后脑和脊髓的腹侧。Nkx6.3从卵裂期到神经胚早期都表达于非神经外胚层，而尾芽期表达于后脑后部和腮弓。在内胚层中，Nkx6.2在尾芽期表达于底索。在蝌蚪期，Nkx6家族的三个基因分别表达于前部内胚层的衍生物，包括胰腺、胃、食道和肺。 Nkx6.3是最近发现的Nkx6家族新成员，它在爪蟾中的表达与Nkx6.1和Nkx6.2有了较大分歧。在第三章，我们通过功能获得及功能缺失实验来探讨Nkx6.3在爪蟾早期发育中的功能。我们发现原肠期前过量或抑制Nkx6.3表达都会影响胚胎原肠运动的正常进行。我们通过动物帽延伸实验证明Nkx6.3参与了细胞运动。半定量RT-PCR结果显示，Nkx6.3可以调控一些粘附分子的表达。以上结果说明Nkx6.3通过调控粘附分子的转录而参与细胞运动的调控。我们还发现，在爪蟾胚胎中Nkx6.3的过表达或抑制表达都导致神经嵴标记基因表达降低。进一步研究发现，32细胞期在不同部位注射Nkx6.3 mRNA可以异位诱导或抑制Slug的表达。动物帽实验显示，Nkx6.3单独过表达可以诱导神经嵴发生，而迄今为止转录因子中只有Snail1具有这一单独诱导能力。在爪蟾胚胎及动物帽中，过表达Nkx6.3都可以诱导Fgf8、Wnt8而抑制BMP4的转录，而且Nkx6.3对这些分泌因子的调控方式是不同的。4细胞期过表达Nkx6.3的胚胎，在促进Fgf8和Wnt8而抑制BMP4的同时，却抑制神经板边界特异基因Msx1、Pax3和神经嵴特异基因Slug的表达，说明Nkx6.3对神经嵴的诱导调控在神经板边界基因层次还存在抑制作用。32细胞过表达Nkx6.3会细胞自主性抑制以及细胞非自主诱导Msx1、Pax3、Slug的表达。Nkx6.3异位诱导Dlx5却抑制Dlx3的表达，说明Dlx5可能是Nkx6.3负调控的直接靶基因。由此，我们提出Nkx6.3的神经嵴诱导调控分为两个层次：分泌信号分子水平的正调控和神经板边界决定水平的负调控。在脊椎动物的神经发生过程中，神经管背腹不同层次形成不同的神经元。这些神经元细胞的命运由背腹起源的多种形态发生素决定。形态发生素通过浓度梯度确定了一组转录因子在神经管背腹不同层次的特异表达，这些基因的组合调控决定了神经前体细胞的命运。然而，这些转录因子是如何解读形态发生素梯度信号的还不是很清楚。第四章，我们通过对神经管腹侧特异表达的转录因子的调控区进行预测，确定了可能调控这些基因表达的保守区段。此外，我们改进了爪蟾转基因操作，并用这一技术确证了Nkx6.2的调控区域。Dbx1、Nkx2.2及Pax6的转录调控区已在小鼠或爪蟾中报道过。由此我们得到了两对在神经管背腹图式中相互作用的转录因子的调控区域：Nkx6.2和Dbx1、Nkx2.2和Pax6。通过对Nkx6.2和Dbx1的调控保守区的转录因子结合位点的预测，我们发现这四个基因以及Wnt信号之间存在大量的相互调控。然而在这两个基因的调控区，我们没有发现Gli的调控位点，暗示这两个基因可能不受Shh的直接调控。我们还克隆了Dbx家族的两个基因，并检测了它们的时空特异性表达，发现Dbx2是母源性表达的，而Dbx1是合子型基因。这两个基因的表达图式相似，都在神经板中线两侧成线状表达，尾芽期在神经管中部表达。过表达Dbx2抑制神经元的初级分化，说明它可能与Dbx1一样具有维持神经板细胞未分化状态的功能。Dbx2的过表达还抑制Nkx6.2及Dbx1的表达，说明它们可能一起参与了神经管腹侧图式的调控。

非洲爪蛙分泌型叶酸结合蛋白及NKX6.3在早期胚胎神经发育中的功能研究

叶酸是B族维生素的一员，参与体内一系列重要的生命过程包括DNA，氨基酸的合成，调控细胞周期，参与一碳单位供体循环，调节DNA,蛋白质甲基化等。叶酸的许多功能都和叶酸结合蛋白有关，体内有多种跨膜形式的叶酸结合蛋白，比如Folbp1，RFC，HCP等。以前的研究表明这些不同的叶酸结合蛋白具有不同的功能。分泌型叶酸结合蛋白是另外一类叶酸结合蛋白，在人类，小鼠，猪中都有序列报道，但是其功能却知之甚少。 我们在非洲爪蛙中鉴定出一个全新的分泌型叶酸结合蛋白并命名为Secreted Folate Binding Protein(sFBP)。在胚胎和转染细胞系中我们都证明该蛋白是分泌性的，表面等离子共振实验发现sFBP能够结合叶酸。在胚胎早期这个基因表达于粘液腺和神经板区域，神经管闭合后在神经管、粘液腺、眼睛，头部以及鳃弓都有表达。特异morpholino 阻断sFBP翻译后发现粘液腺发育异常，神经管闭合缺陷，前后体轴聚集延伸运动受到抑制，尾芽期胚胎表现出体轴缩短，无眼，小头或无头的表型。进一步研究发现显微注射sFBP morpholino 的胚胎神经板区域细胞发生凋亡，中胚层和神经外胚层的一系列粘附分子表达异常，神经细胞的正常分化也受到抑制。通过显微移植实验我们还发现抑制sFBP的翻译后，神经嵴细胞的正常分化和迁移都受到抑制。但是，显微注射叶酸及其类似物或者显微注射甲基供体S-腺苷甲硫氨酸或者亮氨酸甲基转移酶都不能挽救阻断sFBP造成的表形，由此提示sFBP可能不是通过叶酸传统的参与营养合成或者甲基化的途径发挥作用。我们发现注射sFBP morpholino可以抑制Islet-1mRNA和蛋白质的表达，Islet-1的表达区域与sFBP类似。共同注射Islet-1 mRNA和sFBP morpholino可以极大的挽救sFBP morpholino的表型。最后通过morpholino特异阻断Islet-1的表达后，我们发现其表现出与sFBP morpholino类似的粘液腺发育缺陷，神经板细胞凋亡，小头无眼的表形。由此叶酸是B族维生素的一员，参与体内一系列重要的生命过程包括DNA，氨基酸的合成，调控细胞周期，参与一碳单位供体循环，调节DNA,蛋白质甲基化等。叶酸的许多功能都和叶酸结合蛋白有关，体内有多种跨膜形式的叶酸结合蛋白，比如Folbp1，RFC，HCP等。以前的研究表明这些不同的叶酸结合蛋白具有不同的功能。分泌型叶酸结合蛋白是另外一类叶酸结合蛋白，在人类，小鼠，猪中都有序列报道，但是其功能却知之甚少。 我们在非洲爪蛙中鉴定出一个全新的分泌型叶酸结合蛋白并命名为Secreted Folate Binding Protein(sFBP)。在胚胎和转染细胞系中我们都证明该蛋白是分泌性的，表面等离子共振实验发现sFBP能够结合叶酸。在胚胎早期这个基因表达于粘液腺和神经板区域，神经管闭合后在神经管、粘液腺、眼睛，头部以及鳃弓都有表达。特异morpholino 阻断sFBP翻译后发现粘液腺发育异常，神经管闭合缺陷，前后体轴聚集延伸运动受到抑制，尾芽期胚胎表现出体轴缩短，无眼，小头或无头的表型。进一步研究发现显微注射sFBP morpholino 的胚胎神经板区域细胞发生凋亡，中胚层和神经外胚层的一系列粘附分子表达异常，神经细胞的正常分化也受到抑制。通过显微移植实验我们还发现抑制sFBP的翻译后，神经嵴细胞的正常分化和迁移都受到抑制。但是，显微注射叶酸及其类似物或者显微注射甲基供体S-腺苷甲硫氨酸或者亮氨酸甲基转移酶都不能挽救阻断sFBP造成的表形，由此提示sFBP可能不是通过叶酸传统的参与营养合成或者甲基化的途径发挥作用。我们发现注射sFBP morpholino可以抑制Islet-1mRNA和蛋白质的表达，Islet-1的表达区域与sFBP类似。共同注射Islet-1 mRNA和sFBP morpholino可以极大的挽救sFBP morpholino的表型。最后通过morpholino特异阻断Islet-1的表达后，我们发现其表现出与sFBP morpholino类似的粘液腺发育缺陷，神经板细胞凋亡，小头无眼的表形。由此我们认为sFBP结合叶酸后可能通过细胞膜上的受体传递信号，并且Islet-1可能在sFBP的下游发挥作用。 神经嵴是脊椎动物特有的一群多潜能干细胞，产生于表皮和神经板的边界，在原肠运动之后这群细胞通过表皮间充值转换从神经管背侧迁移到不同的区域，分化成不同的细胞类型，包括外周神经系统，色素细胞，软骨等。神经嵴的发生是一个多步骤多基因参与的精细调控过程。目前理论认为最初由一些分泌性信号分子又叫形态生成素比如BMP,Wnt，FGF，Notch等通过不同浓度梯度的相互作用调节一组在表皮和神经板边界的转录因子（Msx、Pax3/7、Zic1、Dlx3/5等）的表达，即边界决定。这些边界决定因子进一步在预定形成神经嵴的区域激活神经嵴特化基因比如Slug/Snail、FoxD3、Twist、Sox9/10的表达完成神经嵴的特化（Specification）。 Nkx6.3是Nkx6家族的一个转录因子，RT-PCR显示其呈现母源性表达。特异抗体显示Nkx6.3蛋白第9期在整个胚胎都表达，大部分蛋白集中在细胞核，有少部分蛋白定位于细胞膜上；神经板时期主要定位于神经嵴区域的细胞膜上。过表达Nkx6.3会影响细胞粘连分子的表达，由此干扰正常的胚胎原肠运动和Activin诱导的动物帽聚集延伸运动。显微注射Nkx6.3特异morpholino阻断其蛋白表达会抑制神经嵴的marker基因Wnt8，Fgf8，Pax3，Msx1，Zic1，FoxD3，Slug的转录，阻碍神经嵴的发育。在动物帽中单独注射Nkx6.3可以在mRNA水平上诱导Wnt8、Fgf8另一方面抑制BMP4的表达进而诱导神经嵴基因Pax3，Zic1，Slug的表达。报告基因实验也显示Nkx6.3能够激活Wnt信号而在动物帽中抑制BMP信号。Nkx6.3蛋白功能域分析发现其EH1结构域（domain）参与对Wnt8信号的激活，而EH1结构域和HD结构域之间的连接区域（linker domain）参与对FGF的激活和对BMP的抑制。进一步在动物帽和胚胎中分析发现Nkx6.3对Wnt8的激活依赖于FGF家族受体信号但是不依赖于Fgf8。有趣的是4细胞时期过表达Nkx6.3促进Fgf8和Wnt8 mRNA表达，但是抑制边界决定基因Msx1、Pax3和神经嵴特化基因Slug的转录。在32细胞时期显微注射Nkx6.3可以在内源神经嵴发生区域抑制Slug的表达，而异位却诱导Slug的mRNA。我们发现与动物帽中对BMP的调节不同，在胚胎中，过表达Nkx6.3会强烈的激活Smad1蛋白在细胞核中的表达即BMP信号被激活，高的BMP信号会抑制神经嵴的发生。另外我们发现过表达Nkx6.3在胚胎中抑制Dlx5而在动物帽中却不影响Dlx5的表达水平，Morpholino阻断Dlx5会抑制Msx1、Pax3和Slug的表达。BMP信号和Dlx5在动物帽和在整体胚胎中对Nkx6.3的不同响应可以一定程度上解释过表达Nkx6.3在2个系统中对神经嵴基因Slug相反的影响结果。

Theoretical study on the ClO/ClO- system electron-transfer reactivity by the golden-rule

The structures, properties and electron transfer reactivity of the ClO/ClO- coupling system are studied in this paper at ab initio (UHF and UMP2) levels and the Density Functional Theory (DFT: UB3LYP, UB3P86, UB3PW91) levels employing 6311 + G(3df) basis set and on the basis of the Golden-rule of the time-dependent perturbation theory. Investigations indicate that the results obtained using the UB3LYP method employing 6-311 + G(3df) basis set is in excellent agreement with the experiment. For this coupling system, six stable coupling modes have been found which correspond to six different encounter complexes and denote six different electron transfer mechanism: four O-O directly linked structures (one collinear: D-h, one anti-parallel: C-s, two twist: C-2) and two Cl-O linked structures (cis- and anti- C-s structures). The activation energies, the stabilization energies and the electronic coupling matrix elements have also been calculated for the electron transfer reactions via these six different mechanism at the UB3LYP/6-311 + G(3df) level, and then the electron transfer rates are determined at the same level. The most favorable coupling mode to the electron transfer is the anti-parallel mechanism. The averaged electron transfer rate is about 5.58 X 10(11) M-1 s(-1). It is also implied that the B3LYP method can give more reasonable results for the electron transfer reactivity of this system. (C) 2003 Elsevier B.V. All rights reserved.

Liquid crystalline phases, microtwinning in crystals and helical chirality transformations in a main-chain chiral liquid crystalline polyester

A main-chain nonracemic chiral liquid crystalline polymer was synthesized from (R)-(-)4'-{w-[2-(p-hydroxy-o-nitrophenyloxy)-1-propyloxy]-1-decyloxyl-4-biphenylcarboxylic acid. This polymer contained 10 methylene units in each chemical repeating unit and was abbreviated PET(R*-10). On the basis of differential scanning calorimetry, wide-angle X-ray diffraction, and polarized light microscopy experiments, chiral smectic C (S-C*) and chiral smectic A (S-A*) phases were identified. Both flat-elongated and helical lamellar crystal morphologies were observed in transmission electron microscopy. Of particular interest was the flat-elongated lamellar crystals were constructed via microtwinning of an orthorhombic cell with dimensions of a = 1.42 nm, b = 1.28 nm, and c = 3.04 nm. On the other hand, the helical lamellar crystals were exclusively left-handed, which was opposite to the right-handed helical crystals grown in PET(R*-9) and PET(R*-11) (having 9 and 11 methylene units, respectively). Note that these three polymers had identical right-handed chiral centers (R*-). Therefore, a single methylene unit difference on the polymer backbones on an atomic length scale substantially changed the chirality of the crystals in the micrometer length scale. Furthermore, aggregates of these helical crystals in PET(R*-10) did not generate banded spherulites in polarized light microscopy. Possible reasons for this change and loss of helical senses (handedness) on different length scales in chirality transferring processes were discussed.