999 resultados para AC-2
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胚胎干细胞(ESC)培养是ESC研究的基础,饲养层的选择是ESC培养的一个重要方面。本实验曾对不同的猕猴饲养层进行研究,显示能够更好的支持猕猴ESC生长的饲养层FGF-2表达量也较高。FGF-2,又名bFGF(碱性成纤维生长因子),是ESC生长所需的重要因子,但其中的分子机制现在并未完全了解。本文一方面对ESC相关研究进展进行了综述,另一方面对以下内容进行了研究:用转基因和RNA干(RNAi)扰的方法建立不同FGF-2的表达量猕猴耳部皮肤细胞(MESF)系五组:过表达FGF-2(f1),过表达的阴性对照组(f2),FGF-2 RNA干扰组(f3),RNA干扰的阴性对照组(f4)以及未作任何处理的对照组(f5),这五组MESF的FGF-2表达量相对值为f1:f2:f3:f4:f5=4:2:1:2:2;c-fos,TGF-β1,INHBA,Gremlin1在f1中表达量上升,在f3中表达量下降;BMP4,TGF-β2在f1中表达量下降,在f3中表达量上升;表明内源FGF-2能够作用于MESF的TGF-β信号通路,引起相关基因表达量的变化。用这些细胞作为饲养层分别培养两种ESC(猕猴ESC,R366. 4和兔ESC,RFESC) ,连续培养了10代,其中在f1上培养的两种ESC增殖速度都比对照组快,并且c-fos,TGF-β1,INHBA,Gremlin1,OCT-4,Nanog,Sox2表达量均上升,BMP4表达下调;在f3上培养的猕猴ESC增殖较慢,BMP4表达上调,c-fos,TGF-β1,INHBA,Gremlin1,OCT-4,Nanog,Sox2表达下调;f3上的兔ESC没有变化。表明ESC中的TGF-β信号通路也受到调节。五组猕猴和兔的ESC形成的EB均表达各胚层早期标记基因(marker),但表达量有差异,f1上ESC形成的EB所有marker都低表达。实验结果表明饲养层中的FGF-2含量高低不仅影响自身相关基因的表达,还对ESC的增殖和维持自我更新有一定的作用。
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一、大鼠海马-前额叶回路在学习记忆中的作用 解剖学研究证实大鼠和猴的海马结构(hippocampal formation, HF;本文‘海马 (hippocampus, Hip)’一词即指海马结构)和前额叶 (prefrontal cortex, PFC) 之间存在一条单向、同侧和单突触的神经回路,即海马-前额叶回路(Hip-PFC回路)。Hip和PFC均参与学习记忆等多种认知功能,PFC是工作记忆的关键脑区,而Hip是空间参考记忆的关键脑区。虽然人们已经对PFC和Hip进行了广泛深入的研究,但对Hip-PFC回路参与哪些认知功能还知之甚少。本研究的目的就是通过暂时阻断Hip-PFC回路,探讨其在学习和记忆中的作用。 在大鼠,Hip-PFC回路中的纤维主要从Hip腹部 (ventral hippocampus, VH)发出,投射到PFC的前边缘皮质(prelimbic cortex, PLC)、下边缘皮质 (infralimbic cortex, ILC) 和外侧前额叶 (lateral prefrontal cortex) 等亚区,其中PLC是Hip-PFC主要投射的区域。我们通过给动物安装慢性导管向脑内注射GABAA受体激动剂muscimol (MU) 阻断Hip-PFC回路。注射位点包括 ①双侧PLC,②双侧VH,③一侧VH和对侧PLC (VH-PLC)。我们首先观察了在PLC或VH局部注射MU对自由活动大鼠PLC和VH脑电功率的影响,并以此确定在行为实验中所用蝇蕈醇的剂量。然后采用T-迷宫空间交互延缓作业 (spatial delayed alternation task) 测试Hip-PFC回路被阻断的动物的空间工作记忆功能;采用被动回避作业 (passive avoidance task) 测试其情绪相关记忆的能力(训练前给药;24 h后重测试);采用Morris水迷宫作业 (Morris water maze task) 测试其空间参考记忆的能力(每天训练前给药;训练期(3 d)结束24 h后重测试)。结果表明:在大鼠PLC或VH局部注射0.5 μg/0.25μl MU后30 min显著抑制VH 和PLC的脑电功率 (VH, p < 0.01; PLC, p < 0.05 vs. PBS/baseline)。注射MU (0.5 μg/0.25μl) 到 ①双侧PLC、②双侧VH、③VH-PLC均显著降低动物在空间交互延缓作业 (All p < 0.001, vs. PBS) 和空间Morris水迷宫作业中的成绩 (All p < 0.05, vs. PBS),表明Hip-PFC回路在空间工作记忆(空间短时记忆)和在空间参考记忆(空间长时记忆)中均起重要作用。在空间交互延缓作业中,双侧PLC被抑制的大鼠的成绩显著低于双侧VH或VH-PLC被抑制的动物,说明PFC在空间工作记忆功能中占有主导地位。在被动回避作业中,双侧VH被抑制动物的回避反应的潜伏期显著短于对照动物 (p < 0.05 vs. PBS),说明双侧VH被抑制动物的情绪记忆受损;而双侧PLC或VH-PLC被抑制的动物其回避反应的潜伏期与对照动物无显著差异 (PLC, p > 0.9; VH-PLC, p > 0.3 vs. PBS),表明双侧PLC或VH-PLC被抑制的动物情绪记忆正常。被动回避作业的结果说明VH参与情绪记忆的形成,但Hip-PFC回路在情绪记忆形成中不起重要作用。 以上结果表明,大鼠Hip-PFC回路参与空间工作记忆和空间参考记忆而不是情绪记忆功能。情绪记忆的关键脑结构是杏仁复合体 (amygdala complex, AMC),VH与AMC有密切的纤维联系。VH被抑制的大鼠情绪记忆受损,说明情绪记忆可能与AMC-Hip回路有关。情绪记忆与空间记忆(参考记忆和工作记忆)在解剖上的分离说明,对于不同类型的记忆来说,其在脑内的信息加工过程是并行的。神经回路内部的信息加工过程则是串行的,回路上任何一个结构的破坏均可导致回路功能的损伤。本研究的结果为学习记忆的“多重记忆系统”理论和记忆信息加工的串行并行机制提供了新的实验证据。 二、芬克罗酮改善成年恒河猴空间工作记忆的谷氨酸机制 芬克罗酮是中科院昆明植物所郝小江等合成的取代吡咯烷酮类化合物。中科院昆明动物所蔡景霞等发现芬克罗酮能改善东莨菪碱、育亨宾等导致的多种动物的不同类型的学习记忆障碍,提高老年动物的学习记忆能力,尤其是老年猴的空间工作记忆。已证实芬克罗酮为部分钙激动剂,可使脑缺血沙土鼠脑内升高的谷氨酸降低,而使正常的沙土鼠海马胞外谷氨酸释放增加。那么芬克罗酮能否提高正常动物的学习记忆,其对正常动物学习记忆的提高是否与其增加谷氨酸的释放有关?本研究采用空间延缓反应作业和谷氨酸NMDA受体拮抗剂MK-801在正常成年猴恒河猴上探讨了以上问题。 结果表明,口服芬克罗酮可显著提高成年猴的空间工作记忆,其量效曲线呈倒‘U’形,符合许多促智药的量效特点。0.25 mg/kg和0.5 mg/kg为芬克罗酮的最佳有效剂量 (p < 0.05 vs. 安慰剂)。肌注MK-801 (0.1 mg/kg) 显著降低成年猴的空间工作记忆 (p < 0.01 vs. 安慰剂),而口服2.0 mg/kg和4.0 mg/kg的芬克罗酮则显著改善MK-801导致的工作记忆障碍 (p < 0.05 vs. MK-801)。芬克罗酮的所有测试剂量不影响猴在作业中的反应时 (p > 0.05 vs. 安慰剂),表明芬克罗酮在该剂量范围不影响动物的运动能力。 本研究结果提示,芬克罗酮可能通钙激动作用促进谷氨酸的释放,在一定剂量范围内提高胞外谷氨酸水平,提高正常动物的空间工作记忆等认知功能。 关键词:芬克罗酮,恒河猴,空间工作记忆,空间延缓反应作业,谷氨酸,MK-801
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采用IPCC AR4规定的极端天气事件划分标准,分析1908—2008年广州、香港、
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This work was supported by the National Basic Research Program of China (973 Program) grant No. G2009CB929300 and the National Natural Science Foundation of China under Grant Nos. 60521001 and 60776061.
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The magnetocapacitive response of a double-barrier structure (DBS), biased beyond resonances, has been employed to determine the density of states (DOS) of the two-dimensional electron gas residing in the accumulation layer on the incident side of the DBS. An adequate procedure is developed to compare the model calculation of the magnetocapacitance with the experimental C vs B curves measured at different temperatures and biases. The results show that the fitting is not only self-consistent but also remarkably good even in well-defined quantum Hall regimes. As a result, information about the DOS in strong magnetic fields could reliably be extracted.
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By using a transfer-matrix method on the basis of two-dimensional (2D) Bloch sums in accordance with a tight-binding scheme, a self-consistent calculation on the resonant tunneling in asymmetric double-barrier structures is presented, in which contributions to resonant tunneling from both three-dimensional (3D) electrons in the contacts and 2D electrons in the spacer or accumulation layers are considered simultaneously. The charge buildup effect on the current versus voltage (I-V) curves is evaluated systematically, showing quantitatively how it results in the I-V bistability and enhanced differences between I-V curves for positive and negative bias in an asymmetric double-barrier structure. Special attention is focused on the interaction between 3D-2D and 2D-2D resonant-tunneling processes, including the suppression of 2D-2D resonant tunneling by the charge buildup in the well accompanying the 3D-2D resonant tunneling. The effects of the emitter doping condition (doping concentration, spacer thickness) on the presence of two types of quasi-2D levels in the emitter accumulation layers, and on the formation of a potential bulge in the emitter region, are discussed in detail in relation to the tunneling process.
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The transient charge response Q(t) of a two-dimensional electron gas (2DEG) in GaAs/AlxGa1-xAs heterostructures to a small pulse of the gate voltage, applied between the top gate and source electrodes in a Corbino structure, was employed to directly measure the effective diffusion constant of a 2DEG in the quantum Hall regime. The measured diffusion constant D showed a drastic change as the magnetic field was swept through the integer fillings of the Landau levels.
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A high-resistivity defect layer buried beneath the silicon surface layer by using proton implantation and two-step conventional furnace annealing is described. During the first annealing step (600-degrees-C), implanted hydrogen atoms move towards the damage region and then coalesce into hydrogen gas bubbles at the residual defect layer. During the second annealing step (1180-degrees-C) these bubbles do not move due to their large volume. Structural defects are formed around the bubbles at a depth of approximately 0.5-mu-m. The defect layer results in a high resistivity value. Experiments show that the quality of the surface layer has been improved because the surface Hall mobility increased by 20%. The sample was investigated by transmission electron microscopy.
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The characteristics of the steady-state and the transient response to external light excitation of a common-cavity two-section (CCTS) bistable semiconductor laser is investigated. The results on the relation of light output versus light input, the wavelength match, optical amplification and optical switching are presented. Experimental results are compared to the results of a computer simulation.
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To evaluate the dynamical effects of the screened interaction in the calculations of quasiparticle energies in many-electron systems a two-delta-function generalized plasma pole model (GPP) is introduced to simulate the dynamical dielectric function. The usual single delta-function GPP model has the drawback of over simplifications and for the crystals without the center of symmetry is inappropriate to describe the finite frequency behavior for dielectric function matrices. The discrete frequency summation method requires too much computation to achieve converged results since ab initio calculations of dielectric function matrices are to be carried out for many different frequencies. The two-delta GPP model is an optimization of the two approaches. We analyze the two-delta GPP model and propose a method to determine from the first principle calculations the amplitudes and effective frequencies of these delta-functions. Analytical solutions are found for the second order equations for the parameter matrices entering the model. This enables realistic applications of the method to the first principle quasiparticle calculations and makes the calculations truly adjustable parameter free.