30 resultados para Scale [ca. 1:4,800,000]None

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A facile, mild and rapid solid phase synthetic route free of column chromatographic purification to the synthesis of soluble monodisperse long-chain oligo(1,4-phenyleneethynylene)s is presented.

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The Ce6-xYxMoO15-delta solid solution with fluorite-related structure have been characterized by differential thermal analysis/thermogravimetry (DTA/TG), X-ray diffraction (XRD), IR, Raman, scanning electric microscopy (SEM) and X-ray photoelectron spectroscopy (XPS) methods. The electric conductivity of samples is investigated by Ac impedance spectroscopy. An essentially pure oxide-ion conductivity of the oxygen-deficiency was observed in pure argon, oxygen and air. The highest oxygen-ion conductivity was found in Ce5.5Y0.5MoO15-delta ranging from 5.9 X 10(-5)(S cm(-1)) at 300 degrees C to 1.3 X 10(-2)(S cm(-1)) at 650 degrees C, respectively. The oxide-ion conductivities remained stable over 80 h-long test at 800 degrees C. These properties suggested that significant oxide-ionic conductivity exists in these materials at moderately elevated temperatures.

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Negative differential resistance (NDR) and memory effect were observed in diodes based on 1,4-dibenzyl C60 (DBC) and zinc phthalocyanine doped polystyrene hybrid material. Certain negative starting sweeping voltages led to a reproducible NDR, making the hybrid material a promising candidate in memory devices. It was found that the introduction of DBC enhanced the ON/OFF current ratio and significantly improved the memory stability. The ON/OFF current ratio was up to 2 orders of magnitude. The write-read-erase-reread cycles were more than 10(6), and the retention time reached 10 000 s without current degradation.

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Monodisperse oligo[(1,4-phenyleneethynylene)-alt-(2,5-thiopheneethynylene)]s, new candidates for molecular wires, were rapidly synthesized via an iterative divergent/convergent doubling strategy in solution as well as on Merrifield's resin.

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用 Siemens P4四圆衍射仪,测得了1,4-二丙氧基-2,3-二氰基萘的晶体结构。晶体属单斜晶系,空间群为 C2/C。晶格参数 a=14.987(3)A,b=10.527(2),c=11.755(2),β=118.98°(3),晶胞体积 V=1622.4(6)3,Z=4,Dc=1.205Kg/m~3,μ(MoK_α)=0.079mm~(-1),F(000)=624,T=293(2)K_o晶体结构应用直接法,解出最后的偏离因子 R=0.0554[1425个Ⅰ≥2σ(Ⅰ)衍射点]。结构分析表明,萘环的1,4和2,3位碳原子上的氢原子分别被丙氧基和氰基所取代,由于取代基的引入使萘环的结构有所改变。

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An extended Goldman-Shen pulse sequence was used to observe indirectly the proton spin diffusion in the blends of polystyrene (PS) with poly(2,6-dimethyl-1,4-phenylene oxides) (PPO). The results indicate that the average distance between PS and PPO is less than 5 angstrom in the intimately mixed phase, but there are heterogeneous domains on a 100-angstrom scale. The data of spin relaxation of carbons, T1(C), for homopolymers and their blends suggest that there is a strong pi-pi electron conjugation interaction between the aromatic rings of PS and those of PPO, while the aromatic rings of PPO drive the aromatic rings of PS to move cooperatively. It is the cooperative motion that markedly improves the impact strength of PS.

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提出了一种精确测量1/4波片相位延迟量的新方法。测量光路由激光器、起偏器、被测1/4波片、光弹调制器、检偏器和光电探测器构成。起偏器和检偏器的透光轴相互垂直。被测1/4波片的快轴与光弹调制器的振动轴平行,且与起偏器和检偏器的透光轴分别成±45°夹角。准直激光束依次经过起偏器、被测1/4波片、光弹调制器和检偏器的探测光强由光电探测器接收。利用探测信号的直流分量与二次谐波分量精确计算出被测1/4波片的相位延迟量。实验验证了这种测量方法的有效性,改变初始光强过程中相位延迟量测量结果的复现性为0.012°,检偏器

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提出了一种基于基频分量消光的波片快轴标定方法,并利用琼斯矩阵对其标定原理进行了分析。激光器、起偏器、相位调制器、待标定1/4波片、检偏器和光电探测器构成标定光路,起偏器、检偏器的透光轴与相位调制器的振动轴分别成+45°和0°夹角。准直激光束依次经过起偏器、相位调制器、待标定1/4波片和检偏器,由光电探测器接收。理论分析表明该标定方法标定精度主要取决于检偏器的定位误差。实验验证了该标定方法的有效性,1/4波片快轴标定结果的最大偏差为0.043°,标准差为0.012°,标定精度为0.05°。

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提出了一种基于同步移相技术的1/4波片快轴方位角的实时测量方法。由正交光栅、光阑、检偏器组和四象限探测器实现同步移相功能。检偏器组由4个不同方位角的检偏器组成。通过检偏器组的四束光束的光强由四象限探测器同时测量。1/4波片的快轴方位角由这四光束的光强得到。由于该方法不需旋转偏振器件,从而实现的1/4波片的快轴方位角的实时测量。

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提出了一种基于同步移相技术的1/4波片相位延迟量的快速测量方法。由正交光栅、光阑、检偏器组和四象限探测器实现同步移相功能。检偏器组由4个不同方位角的检偏器组成。通过检偏器组的四束光束的光强由四象限探测器同时测量。1/4波片的相位延迟量由这四光束的光强得到。该方法中波片的快轴不需被事先确定。另外光源光强的波动对测量结果没有影响。通过实验验证了该方法的有效性。

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By use of a laser diode as a pump source, a self-Q-switched laser from a Cr,Nd:YAG crystal is demonstrated. The output Q-switched traces are very stable, the threshold pump power is 3.5 W, the pulse duration is 50 ns, and the slope efficiency is as high as 20%. In addition, the pulse width remains constant while the pulse repetition rate Varies with pump power. (C) 2000 Optical Society of America OCIS codes: 140.0140, 140.2020, 140.3380, 140.3480, 140.3540, 140.3580.

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高分子材料一般都具有某种特定的结构,这种结构将直接决定着材料的性能。当高聚物从一种结构变为另一种结构时,其材料的性能将发生改变。近来,M.Hikosaka根据聚乙烯结晶的特点,提出了“链滑移扩散理论”,认为对聚合物热处理时,其晶体片层增厚快慢与分子链的滑移扩散能力有关。反式1,4-聚丁二烯(TPBD)在常压下能以六方相稳定存在,是少有的几种具有六方相结构的聚合物。因为其六方相分子链具有较高的构象数,而各个构象之间由于能垒相差不大,构象之间很容易发生转变;因而分子链运动时相对容易,决定了六方相分子链之间的滑移扩散能力较强。为了验证M.Hikosaka的理论,特对样品在六方相温度范围进行热处理。另外由于TPBD在不同的温度下能以两种晶型稳定存在,这两种晶型之间是怎样转变的也是我们关心的问题,而且通过电镜第一次摄得了单斜相和六方相共存的电子衍射。针对上述问题我们进行了下列研究。(1)以三氯化钒体系,稀土催化剂体系合成了两种分子量的反式1,4-聚丁二烯,用IR,NMR分析高分子量样品的反式1,4结构含量为96.2%,低分子量样品反式l,4结构含量为91.2%。对两种分子量样品进行DSC研究,结果表明低分子量样品的转变温度。熔融温度均比高分子量样品低;用Thomoson-Gibbs方程计算了该样品的片层厚度,并与样品的SAXS实验结果对照,认为这种转变温度和熔点的差异除了与1,2-结构的含量有关外,也与不同分子量具有不同的片层厚度有很大关系。(2)对不同分子量的TPBD进行WAXD实验,研究了其在不同温度下的相行为及单斜相向六方相的相转变过程。以PLM为手段跟踪观察了低分子量样品的相态转变,发现许多晶粒在相转变时从视场中消失。用电镜观察到了单斜相电子衍射,六方相电子衍射及单斜相和六方相共存的电子衍射, 并发现两相结构的形貌没有大的差别。(3)用Cerius~2软件模拟了单斜相结构和六方相结构的分子链堆砌,认为单斜相向六方相发生转变时,六方相分子链构象与单斜相分子链构象相比,有序度较低,从而使其堆砌结构变得松散。同时也模拟了单斜相和六方相在晶带轴为[001]方向的电子衍射,实验观察只能得到计算机模拟所得的单斜相和六方相内层的几个电子衍射点。(4)对低分子量样品在64 ℃热处理1小时后进行的DSC,WAXD,SAXS研究表明,样品的片层厚度显著增大,结晶度也相应提高。(5)研究了高分子量样品在85 ℃和低分子量样品在53 ℃热处理不同时间后,所得的DSC曲线。结果表明随时间增加,TPBD的转变峰温度值明显增加;而且发现在前5分钟内处理样品时,结晶度都有明显增加,处理样品5分钟以后结晶度增长缓慢。对高分子量样品四次升降温时,发现降温曲线有肩峰出现,但升温曲线没有肩峰出现,把肩峰的出现归结于有小尺寸亚稳定晶体的形成。(6)对高分子量样品的六方相等温结晶数据及对由熔体快速冷却到一定温度生成单斜相的等温结晶数据进行处理,得到平衡熔点为476K,比文献值高。并利用Thomoson-Gibbs方程,得到了单斜相和六方相的温度对尺寸倒数的相图,确定了在一定尺寸下单斜相和六方相稳定存在的温度范围。(7)用电镜观察了在70 ℃热处理不同时间后所得形貌图,并讨论了样品在六方相中热处理时,样品聚集体的聚集方式。(8)研究了两种分子量样品溶液结晶时所得的球晶形貌,发现其结晶形貌与分子量有关,而且发现摄得的电子衍射是六方相电子衍射,而不是室温下稳定存在的单斜相电子衍射,认为是由于电子辐照使样品升温而发生了晶型转变。(9)用修饰后的Avrami方程,Ozawa,方程分别处理了TPBD非等温结晶数据,由Jeziorny修饰的Avrami方程分析显示TPBD的非等温结晶明显地分为一次结晶和二次结晶两个阶段,指数值n意味着一次结晶和二次结晶的成核种类,Ozawa方程分析不能很好地适用于TPBD的六方相非等温结晶数据,主要是由于Ozawa理论的不精确假定,如二次结晶,结晶温度对片层厚度相关性及整个结晶过程中恒定的冷却函数等。并由Kissinger方程得到六方相的结晶活化能为167.9kJ/mol。