基于三重态吸收的C60/PMMA光子开关

应用泵浦-探测方法,观察了C₆₀/PMMA三重态吸收光子开关效应.     

固体C60/PMMA的激发态吸收光限幅研究

应用五能级模型计算了C₆₀/PMMA的激发态吸收光限幅特性;采用调Q倍频Nd:YAG脉冲激光测量了C₆₀/PMMA的激发态吸收光限幅效应。理论和实验结果基本符合。     

Co2+:ZnAl2O4晶体电子光谱及其2E态双重谱线结构的Jahn-Teller效应研究

在中间场耦合图象中,利用Racak不可约张量算符法和Wigner－Eckart定理,建立了3d⁷(C_3v)电子组态的完全能量矩阵;利用该矩阵研究了Co²⁺:ZnAl₂O₄晶体的电子光谱,理论与观测十分吻合．首次定量地解释了2E态的双重谱线结构,并从理论上预言了⁴A₂基态2.93cm^-1的零场分裂(ZFS)．研究结果定量地表明,Jahn－Teller效应所致Co²⁺:ZnAl₂O₄晶体Co²⁺中心局域结构的畸变假设是合理的．     

C60高压X射线衍射研究

 采用同步辐射X光源和能量色散法对高纯C₆₀粉末样品进行高压原位X光衍射实验。由金刚石对顶压砧高压装置（DAC）产生高压,用已知状态方程的Pt粉末作内标,由Pt的衍射数据确定样品压力,最高压力达30 GPa。实验结果表明：室温常压下原始C₆₀样品为面心立方结构,晶格常数a=1.420 86 nm。高压下C₆₀的结构有所变化：从p=13.7 GPa开始,(311)线发生劈裂,形成低对称相;随着压力增加,衍射线逐渐变宽,强度逐渐变弱,压力超过25 GPa,衍射背底隆起,C₆₀开始转化成非晶相;在30 GPa左右,衍射线条完全消失,标志着向非晶相转化过程的完成。人们也对C₆₀样品不同压力的高压“淬火”相进行了X光衍射实验。采用非静水压的装样方式,最高压力达44 GPa,结果在30 GPa以上,C₆₀也转变为非晶相。最后我们对C₆₀晶体的压致非晶化现象进行了初步的讨论。     

激光光控超导YBa2Cu3Ox薄膜开关的研制

在对光控热电效应开关进行理论分析的基础上,木文提出用YBa₂Cu₃O_x薄膜制作光控开关,并测试了在液氮温度下薄膜开关在不同激光波长下的特征参数,测试的最好结果是响应度R_v(632.8nm,10kHz,1Hz)为217V/W,归一化探测率D_*(632.8nm,10kHz,1Hz)为2.3×10¹¹cm.Hz^1/2/W,响应时间τ为0.21ms.     

低重复率的Ti:Al2O3飞秒激光放大器研究

本文报道了重复频率为10Hz的Ti:Al₂O₃飞秒激光放大器的研究.基于脉冲啁啾放大技术和采用再生/多通放大装置,得到了能量为8mJ的放大光脉冲,在该放大系统中,激光脉冲获M净增益约8×10⁷.     

辅助光对NaCl(OH-)和KCl(Na+,OH-)晶体中的类F2+型色心激光输出的影响

文中报进了有关辅助光对NaCl(OH^-):(F₂⁺)_H及KCl(Na⁺,OH^-):(F₂⁺)_AH色心激光输出功率影响的主要研究结果。初步探讨了辅助光作用的物理机制。     

Zn0.83Mn0.17Se和ZnSe/Zn0.84Mn0.16Se超晶格材料中Mn2+的压力光谱研究

 采用压力光谱技术在低温下观测到了Mn²⁺离子的⁴T₁→⁶A₁跃迁,该谱线在Zn_0.83Mn_0.17Se和ZnSe/Zn_0.84Mn_0.16Se超晶格样品中有不同的压力行为,体材料中其压力系数为-42.4 peV/Pa,超晶格中为-29.5 peV/Pa。用晶体场理论计算得到体材料Zn_0.83Mn_0.17Se中Mn²⁺离子⁴T₁→⁶A₁谱线的压力系数为-38.3 peV/Pa,与实验结果基本一致。结合材料中发光峰积分强度随压力的变化关系进行分析,证实Mn²⁺离子的发光性质主要与其近邻的晶体场环境有关。     

二维Rh-C60聚合相的制备和表征

 利用高压合成装置在6 GPa压力、700 ℃温度条件下合成了二维C₆₀聚合相,并用X射线衍射（XRD）和高分辨核磁共振（NMR）等方法对样品进行了表征。XRD分析结果表明,C₆₀分子在高温高压下发生了聚合反应,晶体结构由面心立方结构变为菱形结构,通过［2+2］加环反应在邻近分子间形成sp³杂化共价键。¹³C核磁共振魔角谱 （¹³C MAS NMR）在δ145和δ72处出现了两个共振峰,其中在δ145附近的峰展宽并有两个边带。δ145附近的峰的展宽与分裂主要是由于C₆₀分子上出现了不等价的sp²杂化碳和高温高压条件下产生的结构无序,边带的形成说明了其结构的各向异性;位置为δ72附近的峰证明了聚合物内C₆₀分子之间出现了sp³杂化键。     

ns脉冲激光对K9玻璃的破坏实验

 采用高速PIN光电探测器和高带宽的数字存储示波器，实时检测透射光脉冲和散射光脉冲的变化特征，并将之用作材料破坏的光学判据，测量得到K9玻璃在1.06μm纳秒脉冲激光作用下的能量损伤阈值约18mJ，相应的能量密度阈值为1.0kJ/cm²。通过分析透射光脉冲和散射光脉冲的特征，给出了材料的破坏时刻，并推断出K9玻璃所能承受的极限光强为10¹⁵W/m²。研究了能量透过率与泵浦能量的关系，并初步探讨了透明材料的破坏机理。结果表明：在多纵模激光的作用下，透明光学材料破坏是电离击穿与自聚焦效应综合作用的结果。     

光致变色二芳基乙烯抗疲劳特性实验研究

提出了一种简单直观的方法研究光致变色材料二芳基乙烯/PMMA膜的抗疲劳特性.通过测量样品在漂白和呈色过程中探测光的透过率,分析该样品光致变色过程的最佳曝光量,在此基础上测量样品的抗疲劳特性.结果显示:在漂白和呈色过程中,激发红光和紫光的最佳曝光量为分别为1 900 J/cm2和600 mJ/cm2,表明该材料对红光不敏感,对紫光比较敏感.定义漂白-呈色过程中,探测光透过率稳定值差下降为第一次循环的50%时样品已经疲劳.通过交替的漂白-呈色循环,测得这种二芳基乙烯材料的擦写次数为27次.     

Fluorination of polymethylmethaacrylate with tetrafluoroethane using DC glow discharge plasma

Fluorination of polymer surfaces has technological applications in various fields such as microelectronics, biomaterials, textile, packing, etc. In this study PMMA surfaces were fluorinated using DC glow discharge plasma. Tetrafluoroethane was used as the fluorinating agent. On the fluorinated PMMA surface, static water contact angle, surface energy, optical transmittance (UV-vis), XPS and AFM analyses were carried out. After the fluorination PMMA surface becomes hydrophobic with water contact angle of 107° without losing optical transparency. Surface energy of fluorine plasma-treated PMMA decreased from 35 mJ/cm² to 21.2 mJ/cm². RMS roughness of the fluorinated surface was 4.01 nm and XPS studies revealed the formation of C-CF_x and CF₃ groups on the PMMA surface.     

脉冲紫外激光刻蚀聚合物薄膜的发射光谱和形貌学研究

用聚焦的紫外XeCl准分子激光器轰击高分子聚合物薄膜(涤纶薄膜),由OMA系统接收其发射光谱.发现谱线主要为C2的Swan带和CN的红带,并与高压汞灯照射后的聚合物薄膜的发射谱进行了比较,在我们的实验精度内,没有发现区别.实验显示,每个光脉冲能刻蚀掉几分之一到几个微米的薄膜.激光的刻蚀效应存在波长和能量密度两个阈值.对于涤纶薄膜,能量密度的阈值约为40mJ/cm2.同时还作了紫外吸收光谱和SEM照片的分析.     

416 nm纳秒脉冲激光对CCD损伤机理研究

开展了416 nm纳秒脉冲激光对CCD的损伤实验,观察到了CCD从点损伤到线损伤,再到面损伤的过程,并计算出了点损伤、线损伤和面损伤所对应的损伤能量密度阈值分别为16.7 mJ/cm2～71.9 mJ/cm2、61.0 mJ/cm2～207.8 mJ/cm2和352.6 mJ/cm2;通过对不同损伤状态CCD的损伤点表面显微图像的分析,以及不同损伤状态对应的CCD各电极之间电阻值的测量,得出不同损伤状态主要由二氧化硅绝缘层材料相变引起电阻值改变所产生;COMSOL软件仿真显示CCD各层最先产生熔融的是二氧化硅绝缘层,能量密度为420 mJ/cm2,与实验结果相接近。实验结果证明了CCD损伤机理分析方法的正确性。     

Adhesion,morphology, and heat resistance properties of polyurethane coated poly(methyl methacrylate)/fullerene-C60 composite films

Novel polyurethane (PU) adhesive was prepared and coated on poly(methyl methacrylate) (PMMA) and poly(methyl methacrylate)/fullerene (PMMA/Full-C₆₀) composite. Dip-coating technique was employed as facile and cost-effective procedure to coat polyurethane on film substrate. The properties of PU/PMMA and PU/PMMA/Full-C₆₀ composite were studied using Fourier transform infrared spectroscopy, Field Emission Scanning Electron Microscopy, tensile, adhesion, thermal and flammability measurement. Testing polyurethane-coated PMMA exhibited crumpled surface while fullerene addition formed unique pattern of dispersed spherical structures. Fullerene nanofiller loading improved the adhesion and mechanical properties of composite films due to polymer–carbon interaction. In PU/PMMA/Full-C₆₀ 0.5 composite with 0.5 wt.% nanofiller, tensile strength (71.4 MPa) was increased by 18.6% while tensile modulus was increased by 143.85% compared with PU/PMMA. In PU/PMMA/Full-C₆₀ 0.5, T₀ of 473 °C and T_max of 655 °C were observed. Increasing the fullerene content up to 0.5 wt.% decreased the peak heat release rate to 131 kW/m². Novel polyurethane-coated PMMA/Full-C₆₀ composite have potential applications as adhesive coatings in electronic and automotive appliances.     

Ablation and surface modifications of PMMA using a laser-plasma EUV source

Surface modification and micro-structuring of polymers for different application is mainly performed using ultraviolet (UV) radiation from excimer lamps or excimer lasers. In this case, however, the radiation penetration depth may exceed 100 μm, thereby degrading the polymer deep inside. On the other hand, extreme ultraviolet (EUV) radiation is absorbed in a layer approximately 100 nm thick only. In this work, the radiation from a laser-plasma EUV source based on a double-stream gas-puff target is focused with a gold-coated ellipsoidal collector for surface modification of polymethylmethacrylate (PMMA). The spectrum of the focused radiation consists of a narrow feature with maximum at 10 nm and a long-wavelength tail up to 70 nm. The PMMA samples are mounted in the focal plane of the EUV collector or at some distance downstream this plane and irradiated for 10–60 s with 10-Hz repetition rate. The irradiated polymer samples were investigated using a scanning electron microscope. When the EUV fluence exceeds 10 mJ/cm², smooth ablation of PMMA was obtained. For lower fluences but close to this value, strong surface modifications appeared.     

Highly photostable solid-state dye lasers based on mixed pyrromethene 567 and coumarin 500

Solid-state dye samples based on polymethyl methacrylate (PMMA) co-doped with pyrromethene 567 (PM567) and coumarin 500 (C500) were prepared. The effects of C500 concentration on the performances of the solid state dye mediums, including spectra property, slope efficiency and photostability were studied. The highest slope efficiency 64.25% was obtained in the sample (PM567: C500 = 2: 8). Pumping the samples at a rate of 5Hz with a pulse energy as high as 100 mJ (the fluence was 0.26 J/cm²), the output energy dropped to half of its initial value after approximate 116130 pulses and the normalized photostability reached 75.48 GJ/mol in the sample (PM567: C500 = 2: 1). Our results have shown that it is possible to obtain a high-efficiency with a long-lifetime for a solid-state dye laser co-doped with PM567 and C500.     

脉宽对中红外激光带内损伤HgCdTe材料的影响

研究了脉宽对于中红外脉冲激光带内损伤碲镉汞（HgCdTe）材料阈值的影响,使用一维自洽模型对激光辐照HgCdTe材料程中的载流子数密度,载流子对数目流,载流子对能流,载流子温度和材料晶格温度等相关参数进行仿真计算。仿真结果表明,波长2.85 μm,脉宽30 ps～10 ns单脉冲激光带内辐照HgCdTe材料的损伤阈值为200～500 mJ/cm2。其中,300 ps～3 ns脉冲激光的损伤阈值相近,均为200 mJ/cm2且低于其他脉宽激光的损伤阈值。搭建实验光路并进行相关实验验证仿真模型的正确性。实验发现,波长2.85 μm、脉宽300 ps的单脉冲激光带内辐照HgCdTe材料的损伤阈值在200 mJ/cm2左右。相同条件下,10 ns单脉冲激光带内辐照HgCdTe材料的损伤阈值约474 mJ/cm2。百皮秒脉冲激光对HgCdTe材料的损伤过程结合了热击穿和光学击穿效应,其独特的毁伤机理加剧了材料的损伤。     

XeCl-laser-generated ablation products from a nitrogen-rich polymer studied by laser-ionization mass spectrometry

Laser-ionization time-of-flight mass spectrometry has been used to probe laser-ablation products from a nitrogen-rich polymer at a wavelength of 308 nm. The ablation products at a laser fluence of 150 mJ/cm² showed, similar to 532 nm ablation studied previously [18], two strong peaks due to neutral species that were assigned to C⁺ and CN⁺, as well as several weak peaks that were assigned to CH⁺, HCN⁺, HCNH⁺, H_nN–CN⁺ (n=1–3), and H₂N–C=N–CN⁺ or H₂N–C=N–CN⁺. The ablation products at 870 mJ/cm² revealed, in addition to a broad signal due to ionic products generated directly by the ablation laser, several peaks due to neutral products that were assigned to C⁺, C ₂ ⁺ , C ₃ ⁺ , CN⁺, HCN⁺, HCNH⁺, and NCCN⁺. The most probable flight velocities for major neutral products are 5.7×10⁴ cm/s at 150 mJ/cm² and 2.3–2.7×10⁴ cm/s at 870 mJ/cm². The results at a laser fluence of 150 mJ/cm² support the finding that the translational energy of the tragments has importance for the collision-induced product generation in the laser plume, as suggested earlier [18]. Furthermore, the product generation at 870 mJ/cm² is interpreted by the ejection of small neutral and ionic fragments, and subsequent reactions among the fragments.     

PDATS对ps脉冲的光限幅效应

应用脉宽为２１ｐｓ脉冲，波长为５３２ｎｍ的激光脉冲研究了新型光限幅材料５－（２－硫甲基－４－甲基－５－嘧啶基）－２，４－戊二炔－１醇的对甲苯磺酸酯的光限幅效应，其优点是限幅幅值和限幅阈值低，分别为Ｅｃ＝１８０ｍＪ／ｃｍ＾２，Ｅｔｈ＝１５０ｍＪ／ｃｍ＾２；可见了光透射率高。