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通过对两栖类动物大蹼铃蟾(B朋b了na勿日对朋)皮肤分泌物及匀浆物的分离,纯化,从其碱性组分中得到了全新的三叶因子多肤(BIn--TFFZ)和膜联蛋白H相关蛋白(BAIIRP),它们分别具有诱导或抑制人血小板活化的全新功能。以血小板膜糖蛋白GPVI受体激动剂stejnulxin为对照,研究了Bm一TFFZ活化人血小板的信号传导途径。哺乳动物的三叶因子(TFF)蛋白的主要功能在于通过修复粘膜损伤,维持粘膜层的完整。它们在肿瘤抑制及癌症侵润方面也有一定程度的作用。我们从两栖类动物大蹼铃蟾皮肤分泌物分离,纯化而得到了一个全新的三叶因子多肤(Bm一TFFZ)。它是单亚基蛋白,表观分子量为13000,并具有全新的诱导人血小板活化的功能,我们研究了其诱导人血小板活化的活性的量效关系。它对血小板的激活涉及血小板整合素a:Ibp3的活化,Bm一TFFZ可诱导经阿斯匹林及三磷酸腺昔"双磷酸酶(Apyrase)处理的血小板的聚集,表明B,TFFZ的活性不依赖于血小板的ADP及血栓嗯烷A2(TXAZ)的自泌正反馈。F工TC标记的B爪一TFFZ蛋白能与血小板膜结合。通过专一性药理学抑制剂的研究,我们初步排除了Bm一TFFZ蛋白作用于血小板膜已知的G一蛋白偶联受体(如ADP,TXAZ及血小板活化因子受体)的可能性。以血小板GPVI激动剂stejnulxin为对照,我们仔细研究了Bm一TFFZ蛋白刺激血小板后的信号传导分子事件,发现其酪氨酸磷酸化图谱明显不同于血小板GPVI激动剂5tejnu1X如,尤其是磷脂酶CYZ并不磷酸化。因此,我们认为Bm一TFFZ蛋白激活血小板的信号传导通路是活化磷脂酶C,并刺激胞内钙离子的释放,活化血小板伪:。p3,进而导致血小板的聚集。从Bm--TFFZ蛋白的cDNA克隆序列推知它由104个氨基酸组成,含有两个三叶因子结构域,与人TFFZ和非洲爪蟾xPZ序列中相同的氨基酸分别占28%及34%。为了确定两栖类的三叶因子蛋白具有诱导人血小板活化的功能,我们仔细地研究了整个分离纯化过程中所有组份的血小板聚集活性并比较了它们的相对活性差异。Bm一TFFZ是第一个来自两栖类动物的血小板激动剂,也是我们第一个报道的具有诱导血小板聚集活性的三叶因子多肤。·我们还通过阴离子交换,凝胶过滤和阳离子交换层析,从大蹼铃蟾皮肤匀浆物中纯化了一个表观分子量为33kD。的单链蛋白。N一末端序列比较分析显示,该·蛋白与来自非洲爪蟾、红色原鸡和人膜联蛋白H的N一末端序列相同的氨基酸分别占70%、64%和56%。该蛋白具有以钙依赖的方式抑制专一性血小板膜糖蛋白VI(GPVI)受体激动剂-Stejnu1Xin诱导洗涤人血小板聚集的生物学功能,最大抑制率达48%。结合其N一末端序列搜索结果及其活性的钙依赖性,推测该蛋白是与膜联蛋白H相关的一类蛋白质。

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A power amplifier MIC with power combining based on AlGaN/GaN HEMTs was fabricated and measured. The amplifier consists of four 10×120μm transistors. A Wilkinson splitters and combining were used to divide and combine the power. By biasing the amplifier at V_(DS) =40V, I(DS)= 0. 9A, a maximum CW output power of 41. 4dBm with a maximum power added efficiency (PAE) of 32. 54% and a power combine efficiency of 69% was achieved at 5. 4GHz.

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We reported a passive Q-switched diode laser pumped Yb:YAG microchip laser with an ion-implanted semi-insulating GaAs wafer. The wafer was implanted with 400-keV As^(+) in the concentration of 10^(16) ions/cm^(2). To decrease the non-saturable loss, we annealed the ion-implanted GaAs at 500 oC for 5 minutes and coated both sides of the ion-implanted GaAs with antireflection (AR) and highreflection (HR) films, respectively. Using GaAs wafer as an absorber and an output coupler, we obtained 52-ns pulse duration of single pulse.

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In a practical coupling system, a cylindrical microlens is used to collimate the emission of a high powerlaser diode (LD) in the dimension perpendicular to the junction plane. Using passive alignment, the LD isplaced in the focus of the cylindrical microlens generally, regardless of the performance of the multimodeoptical fiber and the LD. In this paper, a more complete analysis is arrived at by ray-tracing technique,by which the angle θ of the ray after refraction is computed as a function of the angle θo of the ray beforerefraction. The focus of the cylindrical microlens is not always the optimal position of the LD. In fact, inorder to achieve a higher coupling efficiency, the optimal distance from the LD to the cylindrical microlensis dependent on not only the radius R and the index of refraction n of the cylindrical microlens, but alsothe divergence angle of the LD in the dimension perpendicular to the junction plane and the numericalaperture (NA) of the multimode optical fiber. The results of this discussion are in good agreement withexperimental results.

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The 808nm laser diodes with a broad waveguide are designed and fabricated. The thickness of the Al_(0.35)-Ga_(0.65)As waveguide is increased to 0.9μm. In order to suppress the super modes, the thickness of the Al_(0.55)Ga_(0.45)As cladding layers is reduced to only 0.7μm while keeping the transverse radiation losses of the fundamental mode below 0.2cm~(-1). The structures are grown by metal organic chemical vapour deposition. The devices show excellent performances. The maximum output power of 10.2W in the 100μm broad-area laser diodes is obtained.

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A piece of multimode optical fiber with a low numerical aperture (NA) is used as an inexpensive microlens to collimate the output radiation of a laser diode bar in the high numerical aperture (NA) direction. The emissions of the laser diode bar are coupled into multimode fiber array. The radiation from individual ones of emitter regions is optically coupled into individual ones of fiber array. Total coupling efficiency and fiber output power are 75% and 15W, respectively.

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This paper describes the design and fabrication process of a two-dimensional GaAs-based photonic crystal nanocavity with InAs quantum dots (QDs) emitters and analyzes the optical characteristics of cavity modes at room temperature. The micro-luminescence spectrum recorded from the nanocavities exhibits a narrow optical transition at the lowest order resonance wavelength of about 1137 nm with about 1 nm emission linewidth. In addition, the spectra of photonic crystal nanocavities processed under different etching conditions show that the verticality of air hole sidewall is an important factor determing the luminescence characteristics of photonic crystal nanocaivties. Finally,,the variance of resonant modes is also discussed as a function of r/a ratio and will be used in techniques aimed at improving the probability of achieving spectral coupling of a single QD to a cavity mode.