钕离子同位素移位和超精细结构光谱

原子光谱中,同位素移位和超精细结构光谱是少数几个能够将原子物理和原子核物理这两个不同的物理分支联系起来的课题之一.利用共线快离子束-激光光谱学方法测量了单电荷态钕离子4f45d6G3/2→(26041)°5/2跃迁(波长577.21 nm)的共振光谱,得到了所有7个稳定同位素(A=142～146,148,150)之间的能量移位和2个奇同位素(A=143,145)的超精细结构光谱.     

高非线性光子晶体光纤中飞秒脉冲的传输特性和超连续谱产生机制的实验研究及模拟分析

用实验和数值模拟两种方法研究了高非线性光子晶体光纤中飞秒激光脉冲的传输特性和超连续谱的产生机理，给出了抽运脉冲在三种不同中心波长情况下输出光谱展宽并形成超连续谱的实际测量及理论模拟结果.研究表明：在零色散波长抽运时，光谱展宽以自相位调制为主，同时三阶色散的影响明显，传输脉冲在时域内出现振荡次峰.而在反常色散区抽运时，光谱展宽的初期以自相位调制为主，随后根据抽运功率的不同孤子自频移、高阶光孤子的裂变和四波混频效应会逐渐增强，进而成为光谱展宽的主要原因.与此相应，在时域中能明显看到孤子的形成和红移，飞秒传输脉 关键词： 光子晶体光纤 高非线性光子晶体光纤 飞秒脉冲激光 超连续谱     

超热电子输运背向光辐射的实验研究

在100TW掺钛蓝宝石飞秒激光器上利用光学CCD相机和光学多道分析仪,分别在靶背法线方向测量了超热电子光辐射的空间分布和光谱.测量结果显示：光辐射空间分布图案呈圆环状,而辐射区域有发散角和光强分布,且包含多种辐射成分.光辐射光谱在800nm附近出现尖峰,是激光的基频(ω₀)波,这一现象归因于超热电子束在输运的过程中产生的微束团而引起的相干渡越辐射(CTR).随着激光能量的增加,CTR光谱峰向红光方向移动,基频波红移的主要原因是由于等离子体临界面的迅速膨胀.如果考虑超热电 关键词： 超热电子 光辐射 共振吸收 红移     

皮秒级时间分辨超快高能脉冲激光光谱

介绍了一种利用光电摄谱法和条纹管相结合测量ps级时间分辨超快高能脉冲激光光谱的方法。论述了条纹相机工作原理和平面衍射光栅的分光原理,分析指出利用介绍的装置,可以实现波长300 nm ～1 600 nm、脉宽＞2 ps超快高能脉冲激光的光谱测量。采用1 054 nm超快高能脉冲激光器,实验得到了条纹像,对条纹像进行数据处理后得到测量光谱曲线,通过能量标定后,得到了超快高能脉冲激光器实际光谱曲线,验证了ps级时间分辨超快高能脉冲激光光谱方法。讨论了系统中耦合透镜组对光谱测量和光纤色散角对条纹图像的影响,论述了ps级时间分辨超快高能脉冲激光光谱的作用。随着条纹管制造技术的飞速发展,该方法可用于fs级激光光谱的测量。     

双折射光子晶体光纤中基于孤子分裂的超连续光谱产生

利用亚纳焦量级、脉冲宽度为100 fs的激光脉冲在双折射光子晶体光纤中获得了450—1050 nm 的超连续光谱,且超连续光谱具有明显的分立峰状结构.分析了光谱中分立峰状结构产生的物理机制,抽运光波长处于接近零色散波长的反常色散区,形成高阶光孤子,由于高阶非线性和高阶色散的影响,高阶孤子分裂成多个基孤子,使初始光谱上演化出红移的光孤子成分和蓝移的色散波成分.理论模拟了飞秒激光脉冲在光纤中的色散特性和传输特性,较好地解释了实验结果. 关键词： 光子晶体光纤 超连续光谱产生 孤子分裂 脉冲俘获     

飞秒激光离焦抽运熔融石英产生超连续白光的实验研究

利用飞秒激光在熔融石英介质中传输产生能量达数毫焦、波长范围覆盖400-900 nm 且光谱分布较为均匀的超连续白光,实验过程中将熔融石英介质离焦放置以避免被击穿. 研究了入射激光能量以及介质离焦距离对超连续白光特性的影响. 结果表明采用高能量的入射激光脉冲离焦抽运介质的方法能够有效避免介质 击穿损伤并提高超连续白光脉冲的能量输出.     

基于固体介质的倍频程连续光谱产生的研究进展

超快激光经过透明介质时由于非线性作用光谱会得到展宽,甚至能够产生超过一个倍频程的相干超连续光谱,这样的光源能够压缩得到几个甚至单个光周期的超短脉冲,并在现代超快科学的各个领域得到了广泛应用.实验中已经在气体、液体和固体中都观测到了光谱的展宽,目前较为成熟的方法是使用充满惰性气体的空芯光纤和具有高非线性效应的固体材料展宽光谱.但空芯光纤由于芯径限制无法用于高能量激光脉冲的光谱展宽,而固体材料又容易被高功率密度的脉冲激光损坏.随着激光技术的发展其脉冲能量不断提高,一种新的、利用多片薄固体介质实现光谱展宽的方式被提出.多片薄的非线性介质可以实现光谱展宽的逐片累积,而且避免了激光在介质中因自聚焦产生过高功率密度带来的损坏.目前使用这种方法已经在实验上得到了近毫焦尔量级的倍频程光谱,覆盖了近紫外到中红外的整个区域,并实现了脉冲压缩.本文简要回顾了超快激光在固体中光谱展宽的发展历程,概述了新型薄片固态介质产生超连续光谱的原理,对近年来使用此新方法的实验进行了简要分析,并对其发展前景进行了展望.     

超快激光的光电应用

超快激光一般是指脉冲宽度短于10ps的脉冲激光,主要指短皮秒和飞秒(10-15s)激光。这个时间尺度短于激发态电子向晶格弛豫能量的所需时长,使光与物质相互作用呈现了与通常光激发显著不同的特性,也促成了其崭新的光电应用。围绕飞秒激光与物质相互作用快(作用时间短)、强(瞬态功率高)、精(非线性使作用区体积小,用作加工分辨率高)的特点,开展了系列研究,包括飞秒激光超快光谱用于光/电-电/光转换动力学探索,激光诱导气体成丝用于近程遥感探测,及飞秒激光微纳加工用于新原理、新材料微纳集成器件的制备。介绍了相关研究的进展。     

双色场下紫外超短脉冲的频谱展宽

当共线传输的双色强激光脉冲满足时间重叠时,其等离子体通道间将出现强烈的耦合作用,由此引起的交叉相位调制可产生强烈的非线性效应,使紫外超短脉冲的频谱展宽效应得到增强.将由钛宝石激光系统经三倍频得到的能量为045 mJ、带宽为15 nm的紫外脉冲和能量为71 mJ的近红外脉冲共线聚焦后,在氩气样品池中分别诱导产生等离子体通道,发现紫外脉冲光谱受到明显调制.调制后的光谱半高全宽增至64 nm,为聚焦前谱宽的4倍,是单束紫外脉冲成丝时谱宽的25倍.实验着重研究在不同时间延迟、耦合位置和气体压强情况下,双 关键词： 紫外超快脉冲 双色光丝 非线性效应 光谱展宽     

百飞秒级脉宽的宽带超连续谱光源的产生

实现了一种适合于相干拉曼光谱探测的宽带超连续谱光源的方法,使用1 064nm飞秒激光泵浦全正色散光子晶体光纤,并用光栅对对脉冲进行压缩,最终获得了脉宽178fs,频谱范围处于760～1 300nm的超连续谱光源.对超连续谱脉冲的时间频谱结构进行了分析,未经过压缩的超连续谱的脉冲宽度达到1.43ps,不同频率的成分之间延迟较大,但基本上呈线性平滑分布,因此可以使用光栅对进行色散补偿;此外,提高泵浦光的功率虽然能够增加光谱展宽,但会引入高阶色散,并不利于色散补偿.最后,使用该超连续谱搭建的三色相干反斯托克斯拉曼散射光谱探测系统,测量了苯甲腈溶液的相干反斯托克斯拉曼散射信号光谱,同时获得了3 200cm~(-1)范围内的所有振动模式,验证了该超连续光谱的性能.     

外界光对ZnCl2溶液激光拉曼光谱的影响

对ZnCl2溶液在不同外界环境光存在下的激光拉曼光谱的影响进行了探讨.研究表明不同的外界环境光,自然光和室内荧光灯光,都会对拉曼光谱产生干扰效应,存在着特征谱线,倒峰或尖锐正峰.虽干扰表现不同,但都有影响,不能忽略.因此,在进行溶液拉曼光谱检测时,需在暗室或暗罩中进行,以完全隔离外界环境光的影响.     

Co-transition absorption property of K2ZnCl4:Co2+ crystal

Single-crystal K(2)ZnCl(4) doped with Co2+ has been grown successfully by use of the Czochralski technique. The absorption spectrum of the crystal was measured. The most intense line, centered at 650 nm, was associated with the transition (4)A(2)-->(4)T(1P), and a novel and important result that corporate transition (co-transition) between (4)A(2)-->(4)T(1F) and (4)A(2)-->(4)T(2) of Co2+ in the region of 1300-2400 nm was found and discussed. The mechanism that caused the phenomenon was explained by energy-level splitting theory. In the tetrahedral approximation, using the quantum and Tanaba-Sugano theories, Racah parameter B and crystal field parameter 10Dq were calculated. The optical energy gap, deduced to be 4.82 eV, was lower than that of pure K2ZnCl4.     

熔体局部结构的分子动力学模拟研究

计算机技术的迅速发展使分子动力学模拟成为可能。这是一种直接方法用以更详细地了解液态的结构。文章介绍在分子动力学模拟产生的一系列平衡瞬态构型基础上的等近邻键序参数方法和使用这一方法对若干熔体局部结构的研究，包括若干碱金属卤化物熔盐，ＣａＦ２快离子态和熔融态，熔融态ＺｎＣｌ２和Ｒｂ２ＺｎＣｌ４，ＢＢＯ熔体和晶体生长母液等。     

Ultrasonic relaxation study of preferential solvation in quasi-two-components aqueous solutions of amides and zinc salts

To investigate the effect of preferential solvation the ultrasonic attenuation (2-50 MHz) and velocities (3 MHz) of ZnCl(2) and 2-chloroacetamide (ClCH(2)CONH(2)) in water and its quasi-binary mixtures with the ratio (ZnCl(2)+ClCH(2)CONH(2)):H(2)O=1:55 at 298.15 K have been measured. The creation of specific complexes in the ClCH(2)CONH(2)-H(2)O-ZnCl(2) system have a relaxational character which, within the measurements of ultrasonic absorption in the frequency range 2-50 MHz, have been observed. On the base of these properties the kinetic and dynamic parameters of the observed relaxation have been calculated. To bring into relief the influence of Cl atom in the 2-chloroacetamide molecules for complexation process it has been investigated also the system AA-H(2)O-ZnCl(2). The next step of searching was to investigate the system of CHAA-H(2)O-ZnBr(2), to reduce the influence of Cl atom within ZnCl(2) molecule at the complexation process. The main aim of presented study was to investigate the possibility of complexation in the aqueous solutions of ZnCl(2) with the part of 2-ClCH(2)CONH(2) (CHAA). With regard of big complexing ability of zinc, there exist a theoretical possibility of attachment CHAA to the inner coordination sphere of zinc through chloride atom. There can create here outer-sphere as well as inner-sphere complexes. As a results the observed relaxation processes have been attributed to creation and disintegration the following complexes: Zn(H(2)O)(2)(CHAA)(4)(2+) and Zn(2+)(H(2)O)(3)(CHAA)Cl(2)(-).     

Study of the protoporphyrin luminescence under selective laser excitation

The structural luminescence spectra of protoporphyrin IX solid solutions in ethanol and hydrochloric acid were obtained under selective laser excitation in the region of the inhomogeneouly broadened pure electronic and vibronic bands at T = 3.8 K. The dependence of the excitation selectivity on the excitation frequency was investigated. The vibrational frequencies of protoporphyrin IX were obtained in the ground and excited electronic states when the excitation frequency has been scanned in the region of pure electronic and vibronic bands, respectively. A universal apparatus is described for the investigation of the absorption and luminescence spectra of polyatomic molecules in the temperature range from 3.5 to 300 K under the dye laser excitation tunable in the spectral region 265–365 nm, 435–730 nm, detection of spectra in the region 300–900 nm with a polychromator and silicon intensified image detector and processing of the spectral information with an optical spectrum analyser controlled with a microcomputer.     

用非水二甲基溶液作电解液电沉积ZnO纳米晶薄膜

用含ZnCl2的二甲基亚砚溶液做电解液可在Si衬底上电化学沉积纳米晶薄膜。薄膜的粒径尺寸为8.9nm，样品的光致发光谱以紫外发射峰为主。分析表明用本文介绍的方法可以制备高质量的不含-OH的ZnO纳米晶薄膜。     

K5Nd(MoO4)4: a self-tunable laser crystal

We report for the first time to our knowledge an experimental demonstration of wavelength self-tuning in a K5Nd(MoO4)4 broadband-emitting laser crystal (KNM), as well as a theoretical treatment of the system based on its birefringence properties. The self-frequency-tuning of the laser along the full spectral range of the KNM crystal was obtained by rotating a birefringent gain plate in its own plane. The gain plate was placed inside a resonator at Brewster's angle. The tuning characteristics of the spectral filter were obtained by use of the Jones vector formalism. The calculated wavelength-selective tuning precisely matches the experimental observations.     

Pump-dependent luminescence in the Ag nanoparticles doped by Erbium

A substantial spectral shift of the UV-laser induced luminescence in the Ag nanoparticles (NP) doped by Er³⁺ ions attached to ITO substrates was observed at T = 4.2 K. We have established high energy spectral shift of principal luminescent maxima (from wavelength equal to about 1.45 up to 1.15 μm) with increasing of the pumping nanosecond nitrogen laser power density up to 1.1 GW/cm² operating at λ = 337 nm. With increasing Erbium content with respect to Ag the spectral shift and spectral line broadening increase. It may be caused by specific features of trapping level occupation kinetics on interfaces NP/ITO substrate. The observed process is fully reversible. The luminescence is observed only during excitation by the 337 nm laser pulses and is absent for laser pulses operating at other wavelengths (like excimer laser at 218 nm and nitrogen laser at 371 nm).     

Wavelength-stable, narrow-spectral-width oscillation of an AlGaInP diode laser coupled to a BaTiO3:Co stimulated photorefractive backscattering phase conjugator

3 ) stimulated photorefractive backscattering (SPBS) phase conjugator. The SPBS process was successfully achieved by the combination of the short-wavelength diode laser and the highly doped photorefractive BaTiO₃:Co crystal. The spectral width of the diode laser is reduced to 7.2 pm because of the narrow spectral bandwidth of the gratings [with wave number of K=2k(2k gratings)] formed in the SPBS phase conjugator, compared with the transmission grating formed in the conventional cat conjugator, which was used previously. The SPBS phase conjugator was successfully used to suppress self-frequency scanning, and wavelength-stable oscillation of the SPBS phase-conjugator-coupled diode laser was achieved. Received: 4 November 1996/Revised version: 12 February 1997     

Luminescence from Mn-doped PbI2 crystals

Luminescent properties of PbI₂ and PbI₂: 0.5 mol % MnCl₂ crystals under X-ray or N₂-laser excitation are studied experimentally. The measurements are performed at temperatures ranging from 85 to 295 K. For PbI₂ crystals under laser excitation, spectral bands with peaks near 495 and 512 nm, respectively, are observed at 85 K. With X-ray excitation at the same temperature, luminescence is observed in the 515-and 715-nm bands. The doping decreases the intensity in the 515-nm band, increases it for longer wavelengths, and shifts the highest peak to 700 nm. At 85 K, the doping has an insignificant effect on the excitation energy accumulated by trapped electrons. Certain PbI₂ crystals also exhibit a peak in a region of 580–595 nm. This peak becomes much higher if the crystal is treated with an N₂ laser at room temperature or if it is heated to 450–485 K. As the measurement temperature rises from 85 to 295 K, luminescence intensity decreases considerably. With X-ray excitation at room temperature, the yield of PbI₂: Mn luminescence peaked at 660 nm for doped crystals is about three times larger than the yield peaked at 555 nm for nondoped crystals. The spectral curves and underlying radiative processes are discussed.