多波段紫外太瓦级CPA系统

基于啁啾脉冲放大(CPA)技术和频率变换技术,构建了一个多波长紫外太瓦量级CPA系统.该系统实现了5种频率的精确同步,可同时输出1 Hz,5 Hz和10 Hz的高能量多波段紫外脉冲.时间抖动小于3 ns的时间同步系统和能量不稳定性小于0.5%rms的kHz预放大系统保证了CPA系统输出的能量不稳定性小于2%rms.最后,通过共线相位匹配方案,得到了64 mJ/400 nm,16 mJ/267 nm和5 mJ/205 nm紫外脉冲输出,对应峰值功率达到太瓦量级. 关键词： 啁啾脉冲放大 光学频率变换 紫外脉冲     

Two Polymorphs of the Inclusion Compound [（n-C4H9）4N] ＋（C13H9O3）-H2O

Two polymorphs of the inclusion compound [(n-C4H9)4N]+·(C13H9O3)-·H2O havebeen prepared and characterized by X-ray crystallography. Polymorph 1: triclinic P 1 , a =13.4982(2), b = 13.5743(2), c = 17.1996(2) , α = 67.045(1), β = 77.845(1), γ = 88.762(1)°, V =2830.43(7)3, Z = 4, R = 0.0491, wR = 0.1276; Polymorph 2: tetragonal P43, a = b = 13.53690(1) , c = 30.8491(8) , V = 5653.02(16)3, Z = 8, R = 0.0448, wR = 0.0984. In these two crystalstructures, the hydrogen-bonded ribbons built of 4,4 -dihydroxybenzophenone (DHBP, C13H10O3)anions and water molecules are orderly arranged to generate two-dimensional host layers, withtetrabutylammonium cations contained between the layers to form the sandwich-like inclusioncompounds. The structures of 1 and 2, which exist as two polymorphs, both display the similarpacking pattern and hydrogen-bond linking model.     

Efficient implementation of x-ray ghost imaging based on a modified compressive sensing algorithm

Towards efficient implementation of x-ray ghost imaging (XGI), efficient data acquisition and fast image reconstruction together with high image quality are preferred. In view of radiation dose resulted from the incident x-rays, fewer measurements with sufficient signal-to-noise ratio (SNR) are always anticipated. Available methods based on linear and compressive sensing algorithms cannot meet all the requirements simultaneously. In this paper, a method based on a modified compressive sensing algorithm with conjugate gradient descent method (CGDGI) is developed to solve the problems encountered in available XGI methods. Simulation and experiments demonstrate the practicability of CGDGI-based method for the efficient implementation of XGI. The image reconstruction time of sub-second implicates that the proposed method has the potential for real-time XGI.     

Dynamics of Incoherent Photovoltaic Spatial Solitons

Propagation properties of bright and dark incoherent beams are numerically studied in photovoltaic-photorefractive crystal by using coherent density approach for the first time. Numerical simulations not only exhibit that bright incoherent photovoltaic quasi-soliton, grey-like incoherent photovoltaic soliton, incoherent soliton doublet and triplet can be established under proper conditions, but also display that the spatial coherence properties of these incoherent beams can be significantly affected during propagation by the photovoltaic field.     

利用原子的塞曼光谱对半导体激光器进行稳频

中性原子的超精细能级在磁场中产生塞曼分裂 ,另外 ,左旋和右旋圆偏振光激发下原子的跃迁选择定则不同 ,因此 ,原子在超精细塞曼能级间的吸收谱峰相对无磁场条件下的吸收谱峰有一定的移动。利用这一点 ,验证了一种简单、灵活的方法对半导体激光器进行稳频 ,使激光器的线宽稳到小于 1MHz。通过对实验结果的分析 ,发现由左旋和右旋圆偏振光激发引起的原子吸收谱峰移动之和与饱和吸收峰半高宽相等时 ,稳频效果最好     

多树枝结构和立方结构PbS的水热合成及形成机理

在无模板条件下,用Pb(NO₃)₂做铅源,(CH₄N₂S)做硫源,用水热法在160 ℃反应24 h制备了结晶度好的多树枝结构PbS。利用XRD、SEM、EDX、TEM对产物进行了表征,结果表明所得产物为面心立方多树枝状结构,单个树枝的长度为1.0～3.0 μm。此外,在碱性条件下丙三醇/水体系中制备了具有不同凹面的立方结构PbS,边长为2.0～5.0 μm。对2种不同形态PbS的影响因素进行了讨论,并提出了形成机理。同时对其荧光及紫外性质进行了研究,结果表明立方结构的PbS在309和373.5 nm处出现了2个荧光峰,在211和232 nm处出现了2个紫外吸收峰。     

软骨组织工程构建中的生物力学

关节软骨是关节表面具有弹性的承重组织, 其结构复杂, 由固体相和液体相组成. 固体相包括胶原纤维、蛋白多糖等, 属纤维增强型复合结构; 液体相包括水、电解质等.关节软骨提供了一个低磨损和低摩擦的光滑界面, 起缓冲振动和传递载荷等支撑作用. 由于膝关节承受的运动量大、应力高, 关节软骨损伤在临床上较为常见. 但软骨内没有血管, 代谢缓慢, 其损伤后难以实现自我修复. 组织工程从理论上建立了一种治疗软骨缺损的理想方法, 但尚未成为临床上常规的治疗选择. 如何获得结构和功能相匹配, 同时适用于临床治疗的工程软骨, 至今仍是亟需解决的问题.在体外构建功能化工程软骨, 关键在于运用生物反应器对组织施加合适的力学载荷: 首先保证工程软骨复合体内信号分子、营养和废物的有效运输; 其次对支架内种子细胞产生特定的力学刺激; 同时促进细胞外基质结构与功能的适应性发展.本文对力学载荷在软骨组织工程构建中的应用进展加以综述: 按照作用于组织层面的力学载荷传递所需的介质属性, 将其分为液体介导、固体介导和其他媒质介导三种类型, 重点关注不同载荷对工程软骨功能化构建的作用和效果; 分析讨论软骨组织工程构建中存在的关键生物力学问题; 总结和展望软骨组织工程未来的发展趋势.软骨组织工程体外培养需要考虑力学载荷和生化刺激的耦合作用; 在合适的生化条件下进行滚动、滑动和压缩复合加载, 将有利于工程软骨的体外功能化构建.      

Temporal behaviour of open-circuit photovoltaic solitons

Based on the time-dependent band-transport model in a photorefractive medium, dark open-circuit photovoltaic (PV) solitons are investigated both theoretically and experimentally. Compared with those of the time-independent models, our theoretical results revealed that quasi-steady-state and steady-state PV solitons can both be obtained. Our results also revealed that when r < 1 (r is the normalized intensity at infinity), the full width at half maximum (FWHM) of solitons decreases monotonically to a constant value; when r > 1, however, the FWHM of solitons first decreases to a minimum before it increases to a constant value. Moreover, the FWHM of steady solitons decreases with increasing intensity ratio for r < 1, and increases with increasing intensity ratio for r > 1. We further observed dark PV solitons in experiments, and recorded their evolution. These results indicated that steady solitons can be observed at low optical power, while quasi-steady-state solitons can only be generated at higher optical power. Good agreement is found between theory and experiment.     

Incoherently coupled soliton pairs in nonlocal nonlinear media

We show that incoherently coupled soliton pairs can exist in nonlocal Kerr-type nonlinear media. Such solitons can propagate in bright--bright, dark--dark, and gray--gray configurations. When the nonlocal nonlinearity is absent, these bright--bright and dark--dark soliton pairs are those observed previously in local Kerr-type nonlinear media. Our analysis indicates that for a self-focusing nonlinearity the intensity full width half maximum (FWHM) of the bright--bright pair components increases with the degree of nonlocality of the nonlinear response, whereas for a self-defocusing nonlinearity the intensity FWHM of the dark--dark and gray--gray pair components decreases with the increase in the degree of nonlocality of the nonlinear response. The stability of these soliton pairs has been investigated numerically and it has been found that they are stable.     

含四氮杂大环的双(O,O''''-二(2-苯乙基)二硫代磷酸根)合镍(II)或铜(II)配合物的合成和晶体结构

合成了含四氮杂大环hmta(hmta = meso-5,7,7,12,14,14-六甲基-1,4,8,11-四氮杂环十四烷 )和O,O-二(2-苯乙基)二硫代磷酸根的配合物 [Ni(hmta){SSP(OCH2CH2Ph)2}2] 1和 [Cu(hmta){SSP(OCH2CH2Ph)2}2] 2 , 并测定了它们的晶体结构。配合物1属单斜晶系,空间群为P21/c,晶胞参数为: C48H72N4O4P2S4Ni, a = 9.827(3), b = 19.430(6), c = 13.932(3) ? b = 99.99(2), Mr = 1017.99, V = 2620(1) 3, Z = 2, Dc = 1.285 g/cm3, = 0.635 mm-1, F(000) = 1076, 最终的偏离因子为R = 0.0434, wR = 0.1078, 相应的可观测反射数为2306; 配合物2属单斜晶系, 空间群为P21/c, 晶胞参数为: C48H72N4O4P2S4CuO25, a = 9.730(4), b = 19.513(4), c = 14.031(3) ? b = 99.97(3), Mr = 1022.82, V = 2624 (1) 3, Z = 2, Dc = 1.295 g/cm3, = 0.681 mm-1, F(000) = 1086, 最终的偏离因子为R = 0.0465, wR = 0.1222, 相应的可观测反射数为2492。结构测定表明:两配合物中的配体 (PhCH2CH2O)2PS2-均为单齿配体,金属离子与硫和氮形成了六配位的拉长的八面体配合物,配合物分子具有中心对称性; 同时晶胞中配合物的两配体之间形成了2种N-H贩稴氢键。