Terahertz wave emission from water lines

To make further understanding of terahertz(THz)wave generation from liquid water,we study THz wave emission from water lines of different diameters.The water line with a smaller diameter generates a stronger THz electric field for the diameters from 0.2 mm to 0.5 mm.The THz electric field strength and polarity change with the relative position between the incident laser and water line.Moreover,the THz energy has an optimal radiation angle of about 60°.A two-dimensional dipole array model is introduced to illustrate the phenomenon.Our observations contribute to optimizing the scheme of the liquid THz source.     

The High Energy X-ray telescope (HE) onboard the Insight-HXMT astronomy satellite

The Insight-Hard X-ray Modulation Telescope(Insight-HXMT) is a broadband X-ray and γ-ray(1-3000 ke V) astronomy satellite. One of its three main telescopes is the High Energy X-ray telescope(HE). The main detector plane of HE comprises 18 Na I(Tl)/Cs I(Na) phoswich detectors, where Na I(Tl) is used as the primary detector to measure ~ 20-250 ke V photons incident from the field of view(FOV) defined by collimators, and Cs I(Na) is used as the active shielding detector to Na I(Tl) by pulse shape discrimination. Additionally, Cs I(Na) is used as an omnidirectional γ-ray monitor. The HE collimators have a diverse FOV,i.e. 1.1°×5.7°(15 units), 5.7°×5.7°(2 units), and blocked(1 unit). Therefore, the combined FOV of HE is approximately5.7°×5.7°. Each HE detector has a diameter of 190 mm resulting in a total geometrical area of approximately 5100 cm2, and the energy resolution is ~15% at 60 ke V. For each recorded X-ray event by HE, the timing accuracy is less than 10 μs and the deadtime is less than 10 μs. HE is used for observing spectra and temporal variability of X-ray sources in the 20-250 ke V band either by pointing observations for known sources or scanning observations to unveil new sources. Additionally, HE is used for monitoring the γ-ray burst in 0.2-3 Me V band. This paper not only presents the design and performance of HE instruments but also reports results of the on-ground calibration experiments.     

Second harmonic magnetoacoustic responses of magnetic nanoparticles in magnetoacoustic tomography with magnetic induction

Due to the unique magnetic, mechanical and thermal properties, magnetic nanoparticles(MNPs) have comprehensive applications as the contrast and therapeutic agents in biomedical imaging and magnetic hyperthermia. The linear and nonlinear magnetoacoustic responses determined by the magnetic properties of MNPs have attracted more and more attention in biomedical engineering. By considering the relaxation time of MNPs, we derive the formulae of second harmonic magnetoacoustic responses(2H-MARs) for a cylindrical MNP solution model based on the mechanical oscillations of MNPs in magnetoacoustic tomography with magnetic induction(MAT-MI). It is proved that only the second harmonic magnetoacoustic oscillations can be generated by MNPs under an alternating magnetic excitation. The acoustic pressure of the 2H-MAR is proportional to the square of the magnetic field intensity and exhibits a linear increase with the concentration of MNPs. Numerical simulations of the 2H-MAR are confirmed by the experimental measurements for various magnetic field intensities and solution concentrations using a laser vibrometer. The favorable results demonstrate the feasibility of the harmonic measurements without the fundamental interference of the electromagnetic excitation, and suggest a new harmonic imaging strategy of MAT-MI for MNPs with enhanced spatial resolution and improved signal-to-noise ratio in biomedical applications.     

星载海洋激光雷达最佳工作波长分析

星载激光雷达是实现海洋垂直剖面探测的有效工具,也是目前迫切需求的海洋光学遥感手段。对星载海洋激光雷达的波长参数进行评估对保证探测有效性具有重要意义。本文从探测深度和信噪比两方面分析了星载海洋激光雷达探测全球海洋的最佳波长。利用MODIS 10个波段的水体光学特性数据,估算全球海水探测深度及相应的最优波长;并根据太阳夫琅禾费暗线特性,对信号信噪比进行优化。结果表明:在探测深度方面,最优探测波长在488 nm波段的海洋占全球海洋面积的70%左右,并且全球95%以上的海域在488 nm波段的探测深度优于0.8倍的真光层深度;在信噪比方面,相对于488 nm波段,486.134 nm夫琅禾费暗线处采用0.1 nm带宽的滤光片可以将背景光强度降低70%,相应地回波信噪比整体提升了约5.0%。就全球海洋探测来说,使用486.134 nm作为探测波长可以提高探测深度,有效抑制太阳背景光,提高信噪比,因此,486.134 nm是星载海洋激光雷达的最佳工作波长。     

双金属/TiO2纳米管复合结构中增强的光电流

将传统半导体材料与金属微纳结构相结合,利用其表面等离激元共振效应,可有效地增强复合结构的光电转换效率,使其广泛地被用于光电化学和光电探测等领域.本文以氧化铝纳米管为模板,采用原子层沉积技术制备出高有序的TiO2纳米管,并通过电子束热蒸发技术在大孔径的纳米管薄膜中分别负载金、铝和双金属金/铝纳米颗粒,形成金属纳米颗粒/T...     

秸秆超(亚)临界水预处理与水解技术

秸秆的资源化特别是乙醇化技术由于其技术可行性和产物高值化受到了广泛关注。预处理与水解是乙醇化的关键过程。目前针对秸秆的转化已经开展了多种化学或生物技术的研究,其中超（亚）临界技术与传统技术相比显示了独特的优势,如更高的反应速率、不需催化剂、无产物抑制等。本文在总结秸秆传统预处理与水解技术的基础上,对秸秆超（亚）临界水预处理与水解的过程和机理,特别是超临界亚临界组合技术的研究现状、工艺及其相关研究的进展进行了综述和分析,并阐述了超临界亚临界组合技术首先在超临界水中打破纤维结构进行初级水解,再通过亚临界反应将初级水解产物低聚糖进一步水解为葡萄糖的基本原理。最后对超（亚）临界技术在秸秆资源化领域的研究和应用前景进行了展望。     

两性孪联表面活性剂的合成及溶液性质

用C10～C16脂肪醇与2-氯-2-氧-1,3,2-二氧磷杂环戊烷低温反应生成环状磷酸酯的中间产物,再用N,N-二甲基十二胺在亲核溶剂中65℃下开环反应合成了4种含N 和磷酸根阴离子的两性孪联表面活性剂C10-C12、C12-C12、C14-C12和C16-C12,其质量收率分别为32%、54%、18%和28%。产物的结构通过1HNMR和元素组成分析,表明两性离子表面活性剂C、H、O、N的分析值与理论计算值偏差不超过0.3%。四种表面活性剂的临界胶束浓度(cmc)在0.0072~0.0125mmol/L之间,临界胶束浓度时表面张力(γcmc)依次为23.90、25.61、27.68和36.08mN/m。其中,C10-C12、C12-C12和C14-C12有较好的界面活性,加入盐可以使表面活性剂与烷烃间的界面张力下降,但下降程度有限,不能达到超低界面张力(10-3mN/m)。     

双硫腙包覆钛酸锶钡粉体对水中铅的吸附行为

用草酸化学共沉淀法合成了钛酸锶钡(BST)粉体, 以双硫腙为表面修饰剂, 采用静态浸渍法对钛酸锶钡粉体进行表面包覆修饰, 制备出新型固态粉体吸附剂. 利用X射线衍射(XRD)、扫描电镜(SEM)和傅立叶变换红外光谱(FTIR)进行了表征. 研究了该吸附剂对水中铅的吸附行为. 结果表明: 双硫腙通过与钛酸锶钡表面羟基形成氢键作用包覆于该粉体上; 当吸附介质pH值大于4时, 该吸附剂对水中的铅有较强的吸附能力; 室温下, 5 min内吸附达到平衡. 其吸附行为符合Langmuir吸附等温模型和HO准二级动力学方程式, 吸附焓变(ΔH)为19.42 kJ•mol^－1, 活化能(E_a)为22.187 kJ•mol^－1, 该吸附过程是吸热的物理过程. 吸附在双硫腙包覆钛酸锶钡粉体上的铅, 可用1 mol•L^－1的硝酸溶液进行洗脱. 建立了吸附富集、火焰原子吸收法测定水中铅的新方法, 应用于地表水和自来水中铅的测定, 取得了令人满意的结果.     

New conversion of Friendlnder reaction of 3-amino-1H-benzo[f]chromene-2-carbonitriles with cyclohexanone

Two different skeletons of heterocyclic compounds,quinoline and quinazolinone analogs could be obtained by a novel one-pot synthesis from substituted 3-amino-1 H-benzo[f]chromene-2-carbonitrile derivatives and cyclohexanone in DMF in the catalyst of anhydrous zinc chloride under reflux.A plausible mechanism was proposed.     

Vapor-phase synthesis of V-butylaniline from aniline and 1-butanol over Cu/SiO2 catalyst

The Cu/SiO2 catalyst prepared by incipient wetness method exhibited very high activity and selectivity for the vapor-phase synthesis of JV-butylaniline from aniline and 1-butanol. When Cu loading was 0.70 mmol/g-SiO2 and the catalyst precursor was calcined at 500 ℃, 1-butanol conversion reached 99%, and the selectivity of JV-butylaniline exceeded 97%.