薄膜材料的非线性折射率和非线性吸收系数研究

介绍了用单光束纵向扫描技术(Z扫描)测量薄膜材料的三阶非线性光学效应方法,研究了薄膜材料的非线性吸收效应对其非线性折射率测量的影响.当非线性吸收和非线性折射共存时,非线性吸收效应使Z扫描闭孔的测量曲线峰谷不对称,当耦合因子ξ=β     

磁控溅射ZnO薄膜的三阶非线性光学特性

采用磁控溅射技术在SiO_2衬底上制备ZnO薄膜,并通过X射线衍射仪、原子力显微镜、紫外-可见分光光度计和荧光光谱仪对薄膜的晶体结构、表面形貌、带隙宽度和光致发光性质进行测试表征,结合飞秒激光(波长为800nm,脉宽50fs)和Z扫描方法测量该薄膜的三阶非线性光学特性.结果表明,其三阶非线性折射率和非线性吸收系数均为正值,分别为3.50×10-18 m2/W和2.88×10-11 m/W.     

帽顶光束Z扫描特征曲线的非对称参量

研究了描述帽顶光束Z扫描曲线峰谷相对大小的非对称参量A随远场光阑的线性透过率S和三阶非线性折射相移Φ1之间的变化关系.结果表明对于光克尔介质,当S=0.156时,帽顶光束Z扫描特征曲线的峰高等于谷低且与三阶非线性折射相移Φ1无关,实验中取这一特殊值S,可以很方便地对测量的结果进行归一化处理.此外,分析了高阶非线性效应对非对称参量A的影响,发现当S=0.156时,可以从单一Z扫描特征曲线来判断非线性光学介质是否具有高阶非线性效应以及高阶非线性系数的符号.     

二芳基乙烯化合物的光学性质和光限幅效应

用Z-扫描的方法研究了新合成的一种二芳基乙烯化合物(C27H18F6S2)的光学非线性性质.测量的二芳基乙烯化合物在533nm和633nm处的非线性折射系数分别为n2=-7.69×10-6cm2/W和n2=-3.26×10-6cm2/W,非线性吸收系数分别为,β=-6.96×10-4m/W和β=-1-06×10-3m/W.研究了在大光强下折射率的横向空间分布的变化.该样品对533nm的连续光能够起到优良的光限制器的作用,其光限幅的动态范围可达287.     

N,N'-二[2(1-乙酰基丙烯)]乙二胺合镍的共振三阶非线性光学特性

用Z扫描技术研究了一种新的镍单核配合物(N, N'-二[2(1-乙酰基丙烯)]乙二胺合镍)的三阶非线性光学性质,测得其二氯甲烷溶液(1×10-3mol/l)在488.0nm波长激光激发下的非线性折射率系数n2为2.36×10-4 esu,共振三阶非线性极化率为2.67×10-5 esu ,同时测量了这种材料的光限幅特性 .     

Ge/Al-SiO2薄膜材料的非线性光学特性

采用磁控共溅射及后退火技术制备Ge,Al共掺SiO2薄膜,通过X射线衍射谱和傅里叶红外吸收谱对样品进行表征,并采用皮秒脉冲激光器的单光束Z扫描技术研究薄膜的三阶非线性光学特性.研究结果表明:薄膜材料对1 064nm的光具有自散焦和双光子吸收效应,薄膜的三阶极化率χ(3)为3.84×10-16 m2.V-2.薄膜材料的三阶非线性极化率比SiO2和GeO2均有显著的提高,说明薄膜材料中的纳米Ge颗粒的量子限域效应及双光子吸收效应是其产生非线性光学效应增强的主要原因,同时Al的掺杂也促进了材料的三阶非线性光学效应的增强.     

PbTiO3薄膜的非线性光学性质研究

用射频磁控溅射系统在α-Al2O3衬底上制备了具有钙钛矿结构的PbTiO3薄膜. 用光学透射测量方法得到了该薄膜材料的基本光学常数(带隙、线性折射率、线性吸收系数). 利用Z-扫描技术确定的非线性折射系数n2的符号及大小为-2.8×10-7esu,双光子吸收系数为51.8cm/GW.这些结果表明PbTiO3铁电薄膜在非线性光学上具有潜在的应用前景.     

新型聚吡咯衍生物的大三阶非线性光学效应

制备了一种新型大π共轭高分子聚吡咯 { 2 ,5 二 [(对硝基 )苯甲烯 ]} (PPNB)的纳米薄膜 ,采用激光纵向扫描法研究了其三阶非线性光学性质 .测量了其非线性折射率和三阶非线性极化率 .研究发现该聚合物具有大的三阶非线性光学响应 ,其非线性折射率 (esu)为 1 4 7× 10 - 5,三阶非线性极化率 (esu)为 1 4 4× 10 - 8.从UV vis NIR吸收光谱可知 ,在波长为 532nm的激光照射下 ,PPNB的非线性吸收是双光子吸收 .对比PPNB的纳米薄膜和溶液的三阶非线性极化率和非线性折射率 ,发现纳米薄膜的三阶非线性极化率比溶液的高 2至 3倍 ,而非线性折射率则很接近 ,表明纳米薄膜的双光子非线性吸收比溶液强烈     

掺Cu的SrBi2Ta2O9薄膜的非线性光学特性的研究

以SrBi2Ta2O9陶瓷和高纯Cu片作为靶材,利用射频磁控溅射方法在双面抛光的石英基片上制备了掺Cu金属颗粒的SrBi2Ta2O9复合薄膜.用XRD和AFM表征了薄膜的结晶性能和表面形貌;利用单光束Z扫描技术在波长532 nm处测量了薄膜的非线性光学特性,其三阶非线性光学极化率的实部Reχ(3)=2.26×10-9esu,虚部Imχ(3)=0.62×10-9esu.     

负载硫化铅纳米颗粒介孔氧化硅薄膜的制备及其非线性光学性能

通过离子交换法成功地将硫化铅纳米颗粒引入介孔氧化硅薄膜的孔道内．并用X射线衍射、透射电子显微镜、紫外可见光谱对合成出的硫化铅纳米颗粒负载的复合介孔薄膜进行结构分析,结果表明硫化铅纳米颗粒在孔道分布均匀,平均原子含量为12％．Z扫描测试测试结果表面该复合薄膜具有较高的三阶非线性极化率．     

Absorptive nonlinearity in Er-doped optical fiber

Optical absorptive nonlinearity in Er-doped optical fiber has been discussed and measured at the window wavelength 1.55 μm for optical communications firstly. It is proposed that the mechanism of this absorptive nonlinearity is the induced absorption. The first order nonlinear absorptive coefficient and the imaginary part and the complex value of the third-order susceptibility at that wavelength are obtained from the measured absorptive nonlinearity. Foundation item: Supported by the National Natural Science Foundation of China (69487007) Biography: Song Qian (1937-), female, Professor. Research direction: nonlinear optics and all-optical communications.     

用飞秒光克尔方法测量镶嵌在PVA膜的SnO2纳米晶簇的三阶光学非线性

报道了用飞秒光克尔实验系统测量镶嵌在聚乙烯醇(PVA)薄膜的二氧化锡(SnO2)纳米晶簇的光学非线性的实验结果,平均粒径为10nm和2～3nm的SnO2晶簇的三阶非线性极化率χ(3)分别为4.301×10-14和1.728×10-13esu,并对其原因进行了分析.实验还表明SnO2/PVA薄膜的光学响应是很快的,为50fs.由于聚乙烯醇薄膜的性能稳定,易于生产,上述结果显示它可能成为制作光器件的优良基质.     

掺Nd~(3+)硼硅酸盐玻璃的非线性光学特性

在调Q 纳秒Nd: YAG强激光脉冲下,使用闭孔Z-扫描技术研究了硼硅酸盐基质玻璃及其掺Nd3+玻璃的三阶光学非线性特性.发现基质玻璃具有正的三阶非线性折射系数和非线性吸收系数,属于自聚焦反饱和吸收型的光学介质;而随着Nd3+的掺入,该硼硅酸盐玻璃的三阶非线性折射和吸收系数较基质玻璃有明显的增大,远高于一个量级.用开孔Z-扫描实验与光限幅实验进一步验证了掺Nd3+玻璃具有较高的三阶非线性吸收系数,表明Nd3+的掺入提高了硼硅酸盐玻璃在532 nm处的激光防护性能.     

Third-order optical nonlinearities for lanthanum (Ⅲ) complexes with 1,10-phenanthroline components

The nonlinear refractive indexes n 2 for the ethanol solutions of 1,10-phenanthroline (2.0×10 -3 mol·L -1), [bis(1,10-phenanthroline) lanthanum (Ⅲ)] nitrate (1.0×10 -3 mol·L -1), and [nitrato-fluoracil-bis (1,10-phenanthroline) lanthanum (Ⅲ)] nitrate (1.0×10 -3 mol·L -1) are first measured, the third-order nonlinear optical susceptibilities χ (3) and <γ> are calculated, and the mechanisms of the third-order optical nonlinearities enhanced by lanthanum (Ⅲ) are discussed preliminarily.     

Optical nonlinearity and ultrafast dynamics of ion exchanged silver nanoparticles embedded in soda-lime silicate glass

Ag nanoparticles embedded in soda-lime silicate glass were fabricated by ion-exchange and subse-quently annealing method. Z-scan technique, femtosecond time-resolved optical Kerr effect （OKE） technique and femtosecond pump-probe experiment were used to investigate the effects of laser wavelength and laser pulse duration as well as annealing temperature on the third-order optical nonlinearity and ultrafast dynamics of the composites. It was found that the third-order susceptibility of Ag nanoparticles composite glass measured by 400 nm pulse source is larger than that measured by 800 nm pulse source due to an enhancement effect of local field near surface plasmon resonance of Ag nanoparticles in silicate glass. The third-order optical nonlinearity measured by ns laser source is about two orders of magnitude larger than that measured from fs pulse. The annealing temperature has an important effect on the third-order optical nonlinearity and ultrafast dynamics of the composites. Third-order nonlinear susceptibility up to 10^-l0 esu and fast relaxation process up to 0.2 ps have been obtained in Ag nanoparticles doped glass.     

化合物半导体纳米复合材料的制备和结构及光学特性研究

利用溶胶－凝胶工艺和原位生长技术制备了Ⅱ－Ⅵ族化合物半导体纳米复合材料，得到了ＺｎＳ、ＺｎＴｅ、ＣｄＳ、ＣｄＳｅ、ＣｄｘＨｇ－ｘＴｅ（ｘ＝１＝０．７）纳米微晶与多孔ＳｉＯ２凝胶玻璃的复合材料。用ＸＲＤ研究了不同复合材料的结构特点，利用吸收光谱和透射光谱研究了复合材料的光学特性，发现纳米微晶的禁带宽度大于其相应体材料的禁带宽度，并且复合材料具有明显的非线笥光特性。用简并四波混频测试了样品的三阶非线性     

High-energy ion treatments of amorphous As40Se60 thin films for optical applic ations

The treatment of 100 MeV Ag swift-heavy ion(SHI) irradiation with five different fluences(3 1010, 1 1011, 3 1011, 1 1012, and3 1012ions/cm2) was used to design optical and structural properties of amorphous(a-) As40Se60 chalcogenide thin films. Swanepoel method was applied on transmission measurements to determine the changes in optical bandgap, Tauc parameter and linear optical parameters, i.e., linear optical absorption, extinction coefficient and linear refractive index. Dispersion of the material was determined by Wemple–DiDomenico relation.Changes in nonlinear optical parameters of third-order optical susceptibility and nonlinear refractive index were determined using semi-empirical relations. Changes in surface morphology of the films were investigated using SEM observation, which indicated that fluence 3 1012ions/cm2was upper threshold limit for these films for ion treatment. It is observed that optical bandgap reduces from 1.76 eV to 1.64 eV, and nonlinear refractive index increases from 1.31 10 10[esu] to 1.74 10 10[esu]. Linear refractive index initially increases from 2.80 to 3.52(for fluence3 1010ions/cm2) and then keeps decreasing. The observed changes in optical properties upon irradiation were explained in terms of structural rearrangements by Raman measurement. The study was compiled with the previous literature to propose SHI as an effective optical engineering technique to achieve desired changes according to the need of optical/photonic applications.     

Nonlinear refractive index and absorption coefficient of single-shell semiconductor carbon nanotube

0　IntroductionIn 1991,CNswerediscoveredbyIijima[1 ] fromfullerenesootproducedinanarcdischarge.CNspossessalotofparticularpropertiesduetotheirone dimensionstructureandextraordinarylength radiusratio .Comparedtointrinsicmaterial,CNshavealargerdensityofchargecarrierscausedbythequantumconfine mentofπ electrons,whichleadstoalargerthird orderopticalnonlinearity.Furthermore,theincreaseofsurfaceareaplaysanimportantroleinlightexcitationofchargecarriers,whichleadstoafasterrelaxationtime.Basedontheab…     

Nonlinear optical properties of Eu<Subscript>2</Subscript>O<Subscript>3</Subscript> doped 5ZnO-20Nb<Subscript>2</Subscript>O<Subscript>5</Subscript>-75TeO<Subscript>2</Subscript> glasses

The third-order optical nonlinearities, including third-order nonlinear susceptibility X^(3), nonlinear refractive index (n2) and temporal response, were measured with forward DFWM using Nd:YAG mode-locked pulse laser. The results show that Eu203 doped 5ZnO-20Nb2O5-75TeO2 glasses have large n2 and ultra-fast temporal response. Raman spectra show that Eu2O3 dopant induces the changes in the local structure of glasses. The higher the dopant concentration, the larger the nonlinear refractive n2 and the faster the temporal response. The enhancement on the third-order optical nonlinearities can be attributed to the deformation of the electronic clouds in [TeO4] enhanced by Eu2O3 dopant.