聚乙二醇二丁二酸酯的合成

聚乙二醇在药物合成上有很广泛的用途,但其端羟基的活性相对较低,直接应用受到限制.若将羟基活化为羧基则可以扩大其应用范围;尤其是在合成二聚物时,将疏水链换成亲水的聚乙二醇二丁二酸酯链可以增加桥链的亲水性.为此,以聚乙二醇、丁二酸酐为反应物,以吡啶为溶剂,分别合成了一缩二乙二醇二丁二酸酯、二缩三乙二醇二丁二酸酯、三缩四乙二...     

胶束毛细管电动色谱法在线富集联用技术灵敏检测乳制品和饲料样品中的三聚氰胺

建立了胶束毛细管电泳(MEKC)在线富集技术灵敏检测三聚氰胺的方法,采用场放大进样(FASS)联用胶束扫集(Sweep)测定多种样品中的三聚氰胺.试样用乙腈反复提取3次,在优化实验条件下,三聚氰胺的检测灵敏度提高了约1000倍,检出限由原来的2 mg/L降到1.8 μg/L(S/N=3).本方法用于配方奶粉和动物饲料中...     

1064 nm纳秒脉冲激光诱导硅表面微结构研究

利用Nd:YAG纳秒激光(波长为1064 nm)在不同气氛(空气、N₂,真空)中对单晶硅进行累积脉冲辐照,研究了表面微结构的演化情况.在激光辐照的初始阶段,与532和355 nm纳秒脉冲激光在硅表面诱导出波纹结构不同,1064 nm脉冲激光诱导出了微孔结构和折断线结构,并且硅的晶面取向不同,相应的折断线结构也不同.对于Si(111)面,两条折线交角为120°或60°,形成网状;而对于Si(100)面,两条折断线正交,从而将表面分成了15—20 μm的矩形块.结果表明,微孔结构的生长过程主要与相爆炸有关,而折断线的形成主要是热应力作用的结果.不同气氛对微结构形成的影响表明,刻蚀率和生长率与微结构的形成有密切的关系. 关键词： 纳秒激光 硅的微结构 相爆炸 热应力     

夹持方式对KDP晶体三倍频转换效率的影响

 针对压条固定方式、粘胶固定方式和全外围夹持方式进行理论建模和数值计算分析,并讨论了不同夹持方式的优缺点及其对KDP晶体面形和三倍频转换效率的影响。研究结果表明：晶体面形形变对高斯光束三倍频转换效率的影响明显小于平面波时的情况。当入射基频光光强为6 GW·cm^-2时,对于平面波的情况,压条固定方式、粘胶固定方式和全外围夹持方式3种夹持方式相对于不考虑夹持作用时的三倍频转换效率分别减小7.5%,9.0%和7.2%;对于高斯光束的情况,三倍频转换效率分别减小了1.3%,1.0%和1.5%。     

Dispersion compensation based on the combination of coupled ring resonator and photonic crystal structures

An optical delay line of coupled resonator optical waveguide(CROW) compensated by photonic crystal waveguide(PhCW) is proposed. In the structure,etching the periodic holes around the waveguide of the ring resonator waveguide does not increase the size of the CROW. Theoretical studies and numerical models indicate that through careful design,CROW and PhCW exhibit different group velocity dispersion(GVD) properties at a certain frequency range. Optical signal can not only be compensated in terms of GVD,but can also be delayed with longer time period. Due to the propagation mode mismatch of the two structures,optical loss becomes inevitable.     

Bright blue photoluminescence from a mixed tin and manganese oxide xerogel prepared via solben hydrothermalben gel process

A new blue photoluminescent material, a mixed tin and manganese oxide xerogel, is prepared via sol-hydrothermal-gel process assisted by citric acid. The composition xerogel exhibits strong blue emission at room temperature, with an emission maximum at 434 nm under short (234 nm) or long-wavelength (343 nm) ultraviolet excitation. The photoluminescent excitation spectrum of the mixed tin and manganese oxide xerogel, monitored at an intensity maximum wavelength of 434 nm of the emission, consists of two excitation peaks at 234 nm and 343 nm. With heat treatment temperature increasing from 110 ℃ to 200 ℃, the blue emission intensity increases remarkably, whereas it is almost completely quenched after being treated at 300 ℃. The carbon impurities in the mixed tin and manganese oxide xerogel, confirmed by Fourier transform infrared spectroscopy and X-ray photoelectron spectroscopy, should be responsible for the bright blue photoluminescence.     

（C_6Me_6）_2Fe·PCNP_2类化合物的导电模型

用ＣＮＤＯ／２Ｍ方法计算了（Ｃ６Ｍｅ６）２Ｆｅ·ＰＣＮＰ２和（１，３，５－Ｍｅ３Ｃ６Ｈ３）２Ｆｅ·ＰＣＮＰ２有机导体分子的电荷密度、键级等量子化学参数．计算表明，（Ｃ６Ｍｅ６）２Ｆｅ·ＰＣＮＰ２分子中两个苯环骨架Ｃ原子和Ｆｅ所带的电荷密度分别大于（１，３，５－Ｍｅ３Ｃ６Ｈ３）万Ｆｅ·ＰＣＮＰ２分子的．负电荷集中于两端的五氰基烯两基阴离子的氮原子上，在此基础上，建立了“净电荷导线模型”，并用此模型阐明了这类有机导体导电性能的差异．     

补气方式对R410A冷藏系统性能的影响

针对普通冷库冷藏系统存在排气温度过高、制冷性能较低等问题,研发了一套采用微通道换热器的变频转子压缩机新型冷藏系统,研究系统在不同压缩机转速情况下、采用不同补气形式对系统制冷性能的影响。结果表明：库外温度为32℃时,压缩机转速从3 000 r/min提升至5 000 r/min过程中,分别与不补气系统对比,低压补气系统时排气温度降低了20.54%～22.61%、压缩机功率提高了0.28%～9.19%、制冷量增加了1.15%～4.52%、COP增加了1.41%～3.43%;中压补气系统排气温度降低了18%～20.42%、压缩机功率提高了8.38%～17.29%、制冷量增加了7.86%～18.48%、COP增加了5.08%～8.97%。     

OCS分子在里德堡F态的真空紫外光解动力学：S(3PJ=2,1,0)产物通道

本文利用可调谐真空紫外光源和时间切片离子速度成像技术研究了OCS分子的真空紫外光解动力学. 在对应OCS里德堡F态的五个光解波长下(133.26 nm∽139.96 nm)实验采集了S(³P_J=2,1,0)产物的离子影像,从中发现了两个解离通道：S(³P_J=2,1,0)+CO(X¹Σ⁺)和S(³P_J=2,1,0)+CO(A³π),其中前者为主要通道. 离子影像中CO产物的振动结构可部分分辨. 从离子影像中提取出了S(³P_J=2,1,0)+CO(X¹Σ⁺)通道的产物总平动能分布、各向异性参数和CO振动态分支比等信息. 发现了对应OCS在F态的几个低振动态下光解的产物各向异性参数取负值,而对应F态的几个高振动态下光解产物的各向异性参数为正值. 另外,同一光解波长下三种S产物S(³P₂)、S(³P₁)和S(³P₀)的各向异性参数也不相同. 经分析,这些现象可能来源于激发区域的其它不同对称性的电子态的贡献,从而导致解离过程中同时存在平行解离和垂直解离. 本工作有利于进一步理解OCS真空紫外光解中的非绝热耦合作用.     

Growth,characterization, and Raman spectra of the 1T phases of TiTe2, TiSe2, and TiS2

High-quality large 1$T$ phase of Ti$X_2$ ($X ={\rm Te}$, Se, and S) single crystals have been grown by chemical vapor transport using iodine as a transport agent. The samples are characterized by compositional and structural analyses, and their properties are investigated by Raman spectroscopy. Several phonon modes have been observed, including the widely reported $A_{1g}$ and $E_g$ modes, the rarely reported $E_u$ mode ($\sim$183 cm$^{-1}$ for TiTe$_2$, and $\sim$185 cm$^{-1}$ for TiS$_2$), and even the unexpected $K$ mode ($\sim$85 cm$^{-1}$) of TiTe$_2$. Most phonons harden with the decrease of temperature, except that the $K$ mode of TiTe$_2$ and the $E_u$ and "$A_{2u}$/Sh" modes of TiS$_2$ soften with the decrease of temperature. In addition, we also found phonon changes in TiSe$_2$ that may be related to charge density wave phase transition. Our results on Ti$X_2$ phonons will help to understand their charge density wave and superconductivity.