“绿色”液体激光介质的非线性光学特性研究

利用氧化钕和盐酸为原料制得Nd(phen)2Cl3(三氯二邻菲罗啉合钕),测得其光谱特性并以稀土氧化钕、苯甲酸和邻菲罗啉为原料制得绿色液体激光介质钕离子的配合物——NdB3 phen(三苯甲酸-邻菲罗啉合钕).利用飞秒激光器,采用单光束Z-扫描法研究了NdB3 phen的三阶非线性光学特性.结果表明:当入射飞秒激光脉冲...     

蒽二酮类化合物的合成及结构-非线性光学性能关系的研究

设计合成了6个新的蒽二酮类化合物,用紫外可见吸收光谱、傅里叶变换红外光谱、1H 核磁共振和元素分析表征了结构.采用飞秒激光,运用简并四波混频法,研究了化合物在非共振状态下的三阶非线性光学性能.它们的三阶非线性光学极化率χ(3)为2.62～3.55×10－13 esu,非线性折射率n2为4.82～6.52×10－12 esu,分子二阶超极化率γ为2.57～3.25×10－31 esu,响应时间τ为91～116 fs.探索了化合物的分子结构对三阶非线性光学性能的影响.增长共轭链,形成供吸供构型,增大取代基的供电子能力,提高共轭体系的共平面程度等因素有利于获得较大的三阶非线性光学性能.     

飞秒激光脉冲诱导透明介质的非线性吸收和折射率改变轮廓研究

实验研究了飞秒激光脉冲诱导熔融石英的非线性吸收特性,利用激光诱导自由电子等离子体浓度取决于多光子吸收系数和入射光强的关系;数值模拟了激光诱导折射率变化区域的大小,结合非线性吸收机理和飞秒激光脉冲与介质的相互作用,解释了飞秒激光脉冲超精细加工不受衍射极限的约束,可实现纳米级加工的机理结果表明,电介质的电离能越大,飞秒脉冲诱导的折射率变化区域就越小,但要求的激光脉冲能量也越大;为飞秒激光脉冲超精细加工的材料和激光参量选择提供了理论依据.     

富勒烯有机-无机杂化材料的非共珍三阶非线性光学特性

采用中心波长800 nm、脉宽30 fs的超短激光脉冲,通过飞秒光开关技术（Optical Kerr Shutter,OKS）对富勒烯有机-无机杂化材料的飞秒超快非线性特性进行了实验研究.获得270 fs的开关时间,所得的富勒烯有机-无机杂化材料的三阶非线性系数χ(3)约为4.5×10－14 esu,比C60分子的三阶非线性系数χ(3)高一个数量级.通过实验测定的光克尔信号强度与激发光和探测光偏振方向夹角的依赖关系表明：30 fs的超短激光脉冲激发富勒烯有机-无机杂化材料的克尔信号主要是源于光诱导双折射效应,而非用200 fs的超短激光脉冲时来自瞬态栅的自衍射效应.     

适用于全光开关的[(C3H7)4N][Au(C3S5)2]三阶非线性光学性质研究

合成了一种金属有机配合物[(C3H7)4N][Au(C3S5)2].配制了浓度为1×10－3 mol/L的[(C3H7)4N][Au(C3S5)2]/乙腈溶液,并用旋涂法制备了掺杂浓度质量比为1%的[(C3H7)4N][Au(C3S5)2]/PMMA复合薄膜.运用Z扫描方法,分别研究了样品溶液和薄膜在波长为1 064 nm,脉宽为20 ps条件下的三阶非线性光学性质.研究发现薄膜的三阶非线性极化率χ(3)比溶液高出三个数量级.其中,薄膜的非线性折射率n2为－1.76×10－15 m2/W、三阶非线性极化率χ(3)为9.37×10－10 esu.结果表明,该材料在全光开关方面具有潜在的应用价值.     

稀土铕-芳香羧酸-邻菲罗啉三元有机配合物的合成、表征及发光性能

分别以4种芳香羧酸—对甲基苯甲酸(PMBA)、对氯苯甲酸(PCBA)、对溴苯甲酸(PBr BA)、对氨基苯甲酸(PABA)—作为第一配体,邻菲罗啉(phen)为第二配体,采用溶剂热法合成了4种稀土铕离子(Eu3+)的三元有机配合物。通过元素分析、红外光谱、热重分析等手段确定配合物的化学结构,结果表明,4种配合物的组成可表示为Eu L3phen·H2O(L=PMBA、PCBA、PBr BA、PABA),芳香羧酸配体和邻菲罗啉均与稀土Eu3+配位;铕配合物在318℃以上才开始出现明显失重,表明其具有良好的热稳定性。研究了4种芳香羧酸配体对紫外光的吸收性能。通过荧光光谱研究了配合物的发光性能,4种配合物均发出Eu3+的特征荧光,5D0→7F2电偶极跃迁发射峰强度顺序为:Eu(PBr BA)3phen·H2OEu(PMBA)3phen·H2OEu(PCBA)3phen·H2OEu(PABA)3phen·H2O;其国际照明委员会(CIE)色坐标均落在红光区域,能发出纯正的红光。     

苯甲酸含氮杂环镝配合物的合成、表征及发光性质

合成了以稀土镝为中心离子,以苯甲酸、卤代苯甲酸及邻菲啰啉和2,2'-联吡啶为配体的五种固态配合物。对配合物进行了稀土络合滴定,C、H和N的元素分析、紫外光谱、红外光谱和荧光光谱测定,推测其组成分别为Dy (BA)₃(bpy)、Dy (BA)_3(phen)、Dy(ClBA)₃(phen)(EtOH)、Dy(BrBA)₃(phen)(EtOH)和Dy(IBA)₃(phen)(EtOH)(BA=苯甲酸根,bpy=2,2'-联吡啶,phen=邻菲啰啉,ClBA=对氯苯甲酸,BrBA=对溴苯甲酸,IBA=对碘苯甲酸);苯甲酸羧基氧、邻菲啰啉和2,2'-联吡啶的氮原子与镝离子配位。配合物都具有较强的荧光,卤代苯甲酸配合物呈现规律发光,对氯苯甲酸-邻菲啰啉-镝配合物的发光效果较其它两种配合物强,对溴苯甲酸配合物又强于对碘苯甲酸配合物;苯甲酸-邻菲啰啉-镝配合物荧光强于苯甲酸-2,2'-联吡啶-镝配合物。     

一种侧链共轭聚噻吩衍生物薄膜的三阶非线性光学响应

合成了一种侧链共轭的聚噻吩衍生物聚3-（5′辛基-噻吩乙烯基）噻吩（POTVTh）,并通过溶液旋涂制备了聚合物薄膜.吸收光谱显示该聚合物薄膜具有较小的禁带宽度和宽的光谱响应.采用Z扫描技术在800 nm下用飞秒激光器研究了该聚合物薄膜的三阶非线性光学特性,非线性吸收系数为5.63×10^-7cm/W,非线性折射率为-6.38×10^-11 cm²/W,三阶非线性极化率为4.21×10^-9esu,比侧链未共轭的 关键词： 聚噻吩衍生物 侧链共轭 三阶非线性极化率 非线性折射率     

Sb量子点掺杂钠硼硅玻璃的三阶光学非线性

采用溶胶-凝胶法以正硅酸乙酯、硼酸、金属钠为前驱体合成了含Sb量子点的钠硼硅玻璃。紫外-可见(UV-vis)吸收光谱分析表明量子点玻璃的表面等离子体共振吸收峰在566nm附近;利用飞秒激光钛宝石Z-扫描(Z-scan)技术在800nm波长处对玻璃样品的非线性光学性质进行研究,得到了该玻璃的非线性折射率γ,非线性吸收系数β和三阶非线性极化率χ(3)分别为8.59×10-17 m2/W、1.80×10-10 m/W、4.75×10-11 esu;X-射线粉末衍射(XRD)分析表明具有斜方六面体晶相结构的Sb量子点成功的掺入到玻璃基体中;通过透射电子显微镜(TEM)和高分辨透射电子显微镜(HRTEM)对量子点的尺寸大小和颗粒分布进行了表征,结果显示Sb量子点在玻璃中呈规则的球形,并且颗粒尺寸在19~25nm之间。     

新型三元配合物Tb(DPAB)_3IP的制备与发光性能

合成了邻菲罗啉的衍生物咪唑并[5,6-f]邻菲罗啉(IP),并以其为第二配体,二苯胺羰基邻苯甲酸(HDPAB)为第一配体,制备出新型稀土铽三元有机配合物Tb(DPAB)3IP。采用元素分析、红外光谱和紫外光谱对合成的配体及配合物进行了表征。通过荧光光谱研究了配合物的荧光性质,结果表明第二配体IP有较大的共轭体系,在紫外光激发下,配合物中的配体可将吸收的能量传递给稀土Tb3+离子,表现出较强的Tb3+离子的特征发射,且配体Tb(DPAB)3IP的荧光强度明显大于Tb(DPAB)3phen的荧光强度。这说明适宜的第二配体对配合物有很好的敏化发光作用,合成的Tb(DPAB)3IP是一种良好的绿光材料。     

Measurement of the third order nonlinear optical coefficients of GaP and chirp parameter of laser pulse

The spectral resolved femtosecond pump-probe experiment is applied to measure the third order nonlinear refractive index coefficient, two-photon absorption coefficient of GaP crystal, and the chirp parameter of the input laser pulses. The results show that nonlinear refractive index coefficient is 2× 10-18 m2/W, twophoton absorption coefficient is 2× 10-11 m/W at wavelength of 783.5 nm, and the chirp parameter of laser pulse is l× 1025 s-2. Furthermore, the mechanism of nonlinear refraction due to two-photon absorption in GaP crystal and experimental results are discussed.     

Laser ablation of GaAs in liquids: structural, optical, and nonlinear optical characteristics of colloidal solutions

We investigated the optical, structural, and nonlinear optical properties of GaAs nanoparticles prepared by laser ablation in various liquids at the wavelengths of 795 nm and 1,054 nm. The slow-thermal-effect-induced self-defocusing processes were dominating both in the cases of high pulse repetition rate and nanosecond pulses. The two-photon absorption was observed in these colloidal solutions in the case of low pulse repetition rate of picosecond and femtosecond radiation. The nonlinear susceptibility of GaAs nanoparticles ablated in water was measured to be 2× 10^–9 esu.     

一种新型偶氮化合物的纳秒光限幅特性研究

研究了反式—4—{[p—(N,N—二羟乙基胺基)偶氮苯]乙烯基}吡啶在N,N—二甲基甲酰胺(DMF)中的光限幅性能。实验结果表明,该偶氮化合物的DMF溶液对波长为532nm,脉冲宽度为8ns的激光脉冲具有很强的光限幅特性。理论分析表明,光限幅效应主要起源于材料的双光子吸收。利用双光子吸收模型拟合光限幅实验数据得到材料的双光子吸收系数β=1.6×10-9cm/W。     

基于虚拟仪器的高精度Z扫描实验系统设计

设计了一个表征样品非线性特性的基于虚拟仪器的z扫描实验系统。利用Labview控制数字示波器TDS3012采集两路光强信号，并结合对微位移平台的控制实现Z扫描。以Nd：YAG飞秒放大器产生的800nm的飞秒激光作为探测光，经透镜聚焦后通过薄介质样品；用数字示波器测量样品在透镜焦点附近的透射光强，经过数据处理得到样品的非线性折射率和非线性吸收系数。利用该实验系统，对标准非线性吸收样品Rhodamine 6B进行了测量，计算得到其双光子吸收截面为σ^2=6．8GM（GM：10^-50cm4s photon^-1 molecule^-1），该结果与其他文献利用不同测量方法得到的结果接近，证明该实验系统的测量结果是正确的，可满足非线性测量的精度要求。     

Study on nonlinear optical absorption properties of [(CH3)4N]2[Cu(dmit)2] by Z-scan technique

The third-order optical nonlinearities of an organo-metallic compound, [(CH₃)₄N]₂[Cu(dmit)₂] (dmit²⁻=4,5-dithiolate-1,3-dithiole-2-thione), abbreviated as MeCu, dissolved in acetone are characterized by Z-scan technique with picosecond and nanosecond laser pulses in the near-infrared region. Two-photon absorption has been found when the sample solution is irradiated by 40 ps pulse width at 1064 nm and the two-photon absorption (TPA) coefficient β_TPA is 4×10⁻¹³ m/W. While excited by 15 ns laser pulses at 1053 nm, the Z-scan spectra reveal strong reverse saturable absorption (RSA) and the nonlinear absorption coefficient β_RSA is estimated to be as high as 7.07×10⁻¹¹ m/W which is much larger than β_TPA. An explanation for this enhancement is given. All the results suggest that MeCu may be a promising candidate for the application to optical limiting in the near-infrared region.     

Nonlinear refraction of undoped and Fe-doped KTiOAsO4 crystals in the femtosecond regime

The third-order optical nonlinearities in undoped and Fe-doped KTA crystals have been measured using the Z-scan technique with femtosecond pulses at 780-nm wavelength. The nonlinear refractive index is determined to be 1.7×10⁻¹⁵ cm²/W and 0,9×10⁻¹⁵ cm²/W for undoped and Fe-doped KTA, respectively. No two-photon absorption occurs in these crystals. It is shown that doping with Fe₂O₃ could weaken refractive nonlinearity of KTA, suggesting that Fe:KTA will improve the performance of KTA in high-intensity femtosecond laser applications. In addition, the measured nonlinear index of refraction in KTA crystals is about five times lower than that predicted by the two-band theory. One of the reasons for the discrepancy is given as the applicable limit of the simple theory in which a two-parabolic band model has been assumed in the analysis. Received: 3 June 1999 / Published online: 20 October 1999     

Ultrafast nonlinear optical properties of Bi2O3-B2O3-SiO2 oxide glass

The ultrafast nonlinear optical properties of Bi₂O₃-B₂O₃-SiO₂ oxide glass were investigated using a femtosecond optical Kerr shutter (OKS) at wavelength of 800 nm. The nonlinear response time of this Bi₂O₃-doped glass was measured to be <90 fs. The nonlinear refractive-index n₂ was estimated to be 1.6 × 10⁻¹⁴ cm²/W. Measurements for the dependence of Kerr signals on the polarization angle between the pump and probe beams showed that the Kerr signals induced by 30-fs pulse laser arose mainly from the photoinduced birefringence effect.     

Laser ablation of gallium arsenide in different solutions

The optical, structural, and nonlinear optical characteristics of GaAs nanoparticles obtained by laser ablation in different liquids were investigated. Thermally induced self-defocusing in GaAs solutions was observed using both a high pulse repetition rate and nanosecond pulses. In studying the nonlinear optical characteristics of GaAs solutions using picosecond and femtosecond pulses, two-photon absorption was observed. The nonlinear absorption coefficient of an aqueous GaAs solution measured by the Z-scan technique and the nonlinear susceptibility of GaAs nanoparticles were, respectively, 0.7 × 10^?9 cm W^?1 and 2 × 10^?9 esu at a wavelength of 795 nm.