物理掺杂用纳米Fe粉的制备与结构表征

 根据惯性约束聚变靶材料研究的需要采用自悬浮定向流技术制备了金属纳米Fe粉，通过透射电子显微镜和X射线衍射分析技术研究了颗粒的形貌、粒度和相组成。结果表明，所制备的纳米Fe粉为规则的球状颗粒，其粒径分布在30~70 nm之间，在空气中颗粒表面有氧化膜生成，其氧化产物为Fe₃O₄。     

Synchrotron-Radiation Photoemission Study of Growth and Stability of Au Clusters on Rutile TiO2(110)-1×1

利用同步辐射高分辨光电子能谱研究了金团簇在部分还原TiO₂-(1×1)表面的生长和稳定性．价带谱实验结果观察到非常少量金团簇的沉积导致了Ti3+的3d峰完全消失，表明金团簇成核在TiO₂-(1×1)表面的氧缺陷位．Au4f芯电子光电子能谱实验结果证明了TiO₂-(1×1)表面氧缺陷位向金团簇转移电荷．还对比研究了化学剂量比和部分还原的TiO₂-(1×1)表面上金团簇的热稳定性．当金团簇尺寸相近时部分还原的TiO₂-(1×1)表面上金团簇要比化学剂量比的TiO₂-(1×1)面上金团簇稳定；在相同的表面上尺寸大的金团簇要比尺寸小的金团簇稳定．     

铂基团簇Pt3X(X=Al，Si，Cu)催化水制氢及其水解副产物氧化CO

本文基于第一性原理研究了利用具有幻数结构特点的Pt₃X(X=Al，Si，Cu)团簇仅通过一步反应就能催化分解水制氢的反应过程. 吸附物H₂O@Pt₃X团簇在波长300∽760 nm的紫外和可见光范围内有强吸收，表明太阳光可以方便地用于Pt₃X的催化水解制氢的反应. 此外，水解后滞留在团簇上的O原子可在反应活化能为0.34∽0.58 eV内与CO氧化反应生成CO₂. 这个通过氧化消除“毒性”CO的结果表明了反应副产物有能作催化剂的循环再利用能力. 本文发现生成的CO₂分子还可以在323 K的温度下脱离Pt₃X小团簇.     

银催化合成Tb(BO2)3纳米棒

采用固相反应银作催化剂成功合成出棒状结构的稀土硼酸盐Tb(BO₂)₃发光材料. 利用X射线衍射和区域电子衍射研究了产物的结构特性,在700 oC煅烧时,Tb(BO₂)₃纳米棒具有良好晶形. 透射电镜分析表明,Tb(BO₂)₃纳米棒直径为100～200 nm,厚度为30～50 nm,长约3 μm. 基于Ag纳米颗粒附在Tb(BO₂)₃纳米棒的顶端和中部的事实,探讨了Tb(BO₂)₃纳米棒的生长机理. 荧光光谱研究表明,在369 nm紫外光激发下,Tb(BO₂)₃能发出Tb³⁺的特征绿色荧光,发射主峰位于546 nm,归属于⁵D₄→⁷F₅跃迁. 同时,也探讨了煅烧温度对产物的结构、形貌以及发光性质的影响.     

介孔SiO2纳米棒的制备及其表面锚接金纳米粒子

 以正硅酸乙酯为硅源，十六烷基三甲基溴化铵为模板剂，聚乙二醇为分散剂，采用溶胶-凝胶法制备出SiO₂纳米粒子，应用透射电镜、扫描电镜、X射线衍射仪、红外光谱仪和X射线能谱仪研究了粒子的性能。结果表明：所得产物是具有周期性规则介孔的棒状粒子，长径比随着硅源、模板剂和分散剂浓度的降低而减小；向反应体系中引入乙醇，随着乙醇与水的体积比例的增加，粒子由棒状向球状转变，进而形成不规则絮状凝聚体。用硅烷化技术对SiO₂纳米棒表面进行修饰后吸附平均粒径3.7 nm的金种子，再用多轮生长法使种子长大，经过30轮生长，种子平均粒径增大至59 nm，得到了SiO₂-Au复合纳米体系。透射电镜和紫外-可见分光光度计分析结果表明：金纳米粒子锚接在SiO₂纳米棒表面的某些点位，呈分散分布；复合体系表现出强烈的金的表面等离子体共振吸收峰，该峰随着金粒子的粒径增大，在500~700 nm波段内红移。     

B12N12纳米笼：潜在的二氧化氮检测传感器

利用密度泛函理论通过计算吸附能量、HOMO/LUMO能隙变化、电荷转移、结构扭曲等研究二氧化氮分子在B12N12纳米笼的吸附．此外,通过计算B₁₂N₁₂的电子结合能、Gibbs自由能、态密度和分子表面的静电势研究其稳定性和其它特性．B₁₂N₁₂纳米笼吸附二氧化氮显示三种构型．B₁₂N₁₂团簇的HOMO/LUMO能隙变化对二氧化氮分子的存在非常敏感,从自由团簇的6.84 eV降为NO₂/团簇稳定团簇的3.23 eV．团簇的导电性被极大地提高,表明B₁₂N₁₂纳米簇可能是潜在的二氧化氮气体分子检测传感器.     

Au2Gen-/0 (n=1∽8)团簇结构演化和电子性质的光电子能谱和理论计算研究

本文利用尺寸选择的负离子光电子能谱和理论计算探索Au₂Ge_n^-/0 (n=1∽8)团簇的结构演化和电子性质. 通过比较理论模拟谱与实验谱，并使用CCSD(T)理论方法计算异构体的相对能量，从而确定金锗混合团簇的全局最小结构. 本文发现Au₂Ge_n^-/0 (n=1∽8)团簇的两个Au原子具有较高的配位数和较弱的亲金相互作用. 负离子团簇和中性团簇的最稳定结构分别处于自旋双重态和自旋单重态. 除了Au₂Ge₄^-/0和Au₂Ge₅^-/0，负离子团簇和中性团簇的全局最小结构具有相似的结构特点. Au₂Ge₁^-/0团簇是一个C_2v对称的V形结构，而Au₂Ge₂^-/0团簇是一个C_2v对称的双桥连结构. Au₂Ge₁^-负离子团簇是两个Au原子盖帽的Ge₄四面体结构，而Au₂Ge₄中性团簇是两个Au原子盖帽的Ge₄菱形结构. Au₂Ge_5∽8^-/0团簇主要采用三棱柱、四棱柱、及五棱柱结构. Au₂Ge₆是一个C_2v对称的四棱柱结构，并表现出σ和π双键性质.     

脉冲激光沉积的金属原子团簇的电子状态及生长的研究

 介绍了采用X射线光电子谱(XPS)等技术研究脉冲激光沉积在Ni、Mo、C、NaCl(100)表面的Cu、Au原子团簇的电子状态;结合Cu₂p_3/2 X射线光电子谱峰和Cu L₃M_4,5M_4,5俄歇跃迁分离了电子结合能的初态和终态贡献,得出了它们随Cu表面浓度变化的关系,并对之作出了解释。使用XPS、RBS、TEM三项技术研究了Au在NaCl(100)表面的生长过程,通过计算得出了在不同表面浓度下Au原子团簇的平均高度和表面覆盖率。     

[Co(CO2)n]+团簇的红外解离光谱实验和理论研究

本文利用红外光解离光谱研究了一价钴阳离子与二氧化碳之间的相互作用. 通过密度泛函理论计算得到[Co(CO₂)_n]⁺团簇的几何结构，并且模拟了它们的振动光谱与实验数值进行比较. 研究结果表明，在[Co(CO₂)_n]⁺(n=2∽6)团簇中，钴阳离子通过电四极矩静电作用以端点结合的方式与二氧化碳中的氧原子结合在一起. 团簇的红外光谱都集中在二氧化碳反对称伸缩的波数附近，并且随着团簇尺寸的变化出现蓝移，最后把[Co(CO₂)_n]⁺的红外光解离光谱与稀有气体贴附的[Co(CO₂)_n]⁺-Ar的红外光解离光谱进行了比较.     

硼(氮、氟)掺杂对TiO2纳米颗粒光学性能的影响

利用X射线衍射谱、拉曼光谱和紫外-可见光吸收光谱研究了硼(氮、氟)掺杂对TiO₂纳米颗粒光学性能的影响.X射线衍射谱和拉曼光谱结果表明,掺硼(氮、氟)对TiO₂纳米颗粒的锐钛矿相晶体结构无明显影响,而其锐钛矿晶格出现畸变(c/a值增大),这被归因于掺杂原子对TiO₂纳米颗粒表面氧原子缺位沿晶格c轴方向的占据.另外,掺硼(氮、氟)TiO₂纳米颗粒吸收带红移与TiO相似文献   

金纳米粒子掺杂DNA-CTMA-DPFP薄膜的表面增强拉曼散射特性

采用柠檬酸三钠还原氯金酸和离子交换法制备金纳米粒子掺杂DNA-CTMA材料,利用钯催化反应合成9,9-二乙基-2,7-二-(4-吡啶)芴荧光染料(DPFP),将DPFP与DNA-CTMA混合后,旋凃制备金纳米粒子掺杂的DNA-CTMA-DPFP薄膜样品。通过吸收光谱、荧光光谱和拉曼光谱的测量,研究了薄膜样品的光学特性和表面增强拉曼散射(SERS)特性。实验结果表明,薄膜样品在300～360 nm的吸收主要来自DPFP,在500～700 nm的吸收来自样品中金纳米粒子的局域表面等离子共振;样品在370,386,408 nm处的荧光峰分别对应DPFP的S₁₀-S₀₀、S₁₀-S₀₁和S₁₀-S₀₂能级的电子振动跃迁;在785 nm激光激发下,薄膜样品的拉曼散射主要来自DPFP分子,随着金纳米粒子掺杂比的增大,DPFP分子的拉曼散射峰强度逐渐增强。因此,金纳米粒子掺杂DNA-CTMA薄膜适合作为多种染料分子的SERS基底。     

Laser-assisted growth of gold nanoparticles: Shaping and optical characterization

We demonstrate that supported gold nanoparticles with a given well-defined shape can be produced by laser-assisted growth. For this purpose, gold nanoparticles with average radii ranging from 1.5 to 13 nm, i.e., coverage between 0.45 × 10¹⁶ and 5.6 × 10¹⁶ atoms/cm², were prepared at room temperature by self-assembly of atoms deposited on quartz and sapphire substrates. For analysis of the samples, the optical spectra of the particles were measured with p-polarized light and photon energies in the range of 1.3 to 3.1 eV. Irradiating the particles during growth with laser light of different wavelengths to stimulate surface plasmon excitation made it possible to stabilize mean axial ratios between 0.19 and 0.98. The influence of the laser fluence on the shape of the nanoparticles was also investigated and shows that the position of the surface plasmon resonance shifts to higher energies as the fluence rises. Optimum growth conditions to shape gold nanoparticles with axial ratios close to unity (spheres) with a relatively low laser fluence of 60 ± 5 mJ/cm² have also been found. The results of our experiments show that laser-assisted growth is a powerfultechnique to control the shape of nanoparticles.     

纳米NiO的制备及其谱学特性研究

以醋酸镍、氢氧化钠为原料, 吐温80为分散剂, 通过固相反应制备了纳米级NiO. 用X射线衍射仪、透射电子显微镜、傅里叶红外光谱、紫外-可见分光光度等方法对材料的粒径、晶格畸变率、形貌以及红外、紫外-可见光的吸收性能进行了表征. 结果表明: 制得的纳米NiO产物为球形、属立方晶系, 粒径大小在9～30 nm左右;晶格畸变率随粒径的增大而减小;纳米NiO红外吸收峰出现在437 cm-1处, 与普通粒径的NiO光谱纯(484 cm-1)相比, 其吸收峰红移了47 cm-1, 体现了纳米NiO的表面效应;不同粒径大小的NiO对紫外-可见光的吸收特性不同. 普通粒径的NiO光谱纯在紫外-可见光区域没有吸收, 颗粒尺寸越小吸收波长越短, 10 nm NiO的紫外-可见光吸收峰位于309 nm处, 直接跃迁的光学能带隙约为4.2 eV, 比体相材料(3.65 eV)增加0.55 eV, 表现出明显的量子尺寸效应. 对纳米NiO的谱学特性研究表明该材料在光电领域具有潜在的应用价值.     

Rapid synthesize of gold nanoparticles by microwave irradiation method and its application as an optical limiting material

We present rapid synthesis of gold nanoparticles by microwave irradiation method. Sample with average particle size 7.7 nm is obtained from TEM. Linear and nonlinear optical studies of the prepared samples are discussed. Reverse saturable absorption (RSA) at longitudinal surface plasmon resonance (SPR) in gold nanoparticles (Au NPs) have been observed using Z-scan and transient absorption techniques with 532 nm laser pulses. Such RSA behavior makes Au NPs an ideal candidate for optical limiting applications.     

硫醇衍生化的纳米金与癌胚抗原相互作用的光学分析

纳米金已在在药物靶向传输体系、疾病检测、分子识别、生物标签等领域有着广泛的应用,但是,由于纳米金的表面效应,大量的表面原子具有巨大剩余成键能力,使得纳米金粒子较容易团聚、沉聚,影响了其稳定性。为了实现对肿瘤靶标之一-癌胚抗原的痕量检测,需要制备出对癌胚抗原检测具有良好的增色效应与荧光增敏效应的纳米材料。该工作采用纳米金的硫醇衍生法制备了一种新型的硫醇衍生化的纳米金材料,并对此新型硫醇衍生化的纳米金材料的特性用透射电子显微镜,紫外-可见吸收光谱,荧光发射光谱和红外光谱等方法进行了研究。紫外-可见吸收光谱,荧光发射光谱的实验结果表明,在新的配体乙二硫醇存在下,有更多的电子从配体的轨道跃迁到与中心离子相关的轨道上,导致荧光增强。这种新型硫醇衍生化的纳米金与癌胚抗原作用时表现出增色效应与荧光增敏效应,而纳米金与癌胚抗原作用时看不到这种增色效应与荧光增敏效应。红外方法的研究结果表明,这种材料的蛋白增色机理为当硫醇衍生化纳米金与癌胚抗原蛋白作用时,体系中蛋白的—OH表现出更多的面外弯曲振动,有利于电子从硫醇衍生化纳米金配合物向蛋白转移而导致其增色和荧光增敏效应。因而这种新的硫醇衍生化纳米金材料比纳米金将具有更好的生物检测应用价值。     

Synthesis and characterization of cobalt/gold bimetallic nanoparticles

Cobalt/gold (Co/Au) bimetallic nanoparticles are prepared by chemically reducing gold (III) chloride to gold in the presence of pre-synthesized Co nanoparticles. Transmission electron microscopy (TEM), ultraviolet-visible (UV-vis) absorption spectrometry, and a superconducting quantum interference device (SQUID) magnetometer have been used to characterize as-prepared bimetallic nanoparticles. Our findings demonstrate Au not only grows onto Co nanoparticles, forming a surface coating, but also diffuses into Co nanoparticles. The introduction of Au alters the crystalline structure of Co nanoparticles and changes their magnetic properties. Dodecanethiols induce a reorganization of as-prepared Co/Au bimetallic nanoparticles.     

光照法在玻璃基底上原位生长金纳米结构及其光谱性质

 以硅烷化后吸附粒径小于10 nm的金种子的玻璃片为基底，聚乙烯吡咯烷酮为还原剂，在荧光灯照射条件下还原氯金酸，制备出表面具有金纳米粒子聚集结构的基底。用原子力显微镜、扫描电镜、X射线衍射、吸收和荧光光谱研究了基底的性质。结果表明：随着光照时间增加至20 h，金种子长大为平均粒径140 nm的不规则状多晶粒子，且出现双层粒子堆叠。基底的吸收光谱上出现了由金粒子的表面等离子体激元偶极子耦合引发的强烈吸收峰，随着粒子粒径增大，耦合峰在600~800 nm波段内连续红移升高，表明耦合程度不断增强。在223 nm紫外光的激发下，基底的荧光光谱上在405 nm处出现发射峰，是由金粒子表面激发电子和空穴的复合辐射造成的，发光强度随着基底上粒子平均尺度增加而减弱。     

Effect of a thioalkane capping layer on the first hyperpolarizabilities of gold and silver nanoparticles

We have measured the first hyperpolarizabilities of thioalkane capped silver and gold metallic nanoparticles. The values found are β(AgC 12-10 nm) = (2.10 ± 0.23) × 10(-26) esu for 10 nm diameter silver nanoparticles and β(AuC 18-18 nm) = (3.37 ± 0.08) × 10(-26) esu for 18 nm diameter gold nanoparticles at the fundamental wavelength of 784 nm. By comparison to the corresponding values reported for citrate capped silver and gold metallic nanoparticles, after size corrections, decreases by factors of 4.3 and 6.5 respectively are observed. These decreases are tentatively attributed to the bonds formed between the gold and silver surface atoms and the sulfur atoms of the capping layer.     

Raman spectroscopy of gold nanoparticles in polycrystalline LiF film

Results of the Raman spectroscopy analysis of a new composite material based on a thin polycrystalline LiF film containing gold nanoparticles are presented. The formation of spherical gold nanoparticles in the film has been confirmed by the X-ray structural analysis and observation of the optical plasmon resonance absorption spectrum with a maximum at 534 nm. The obtained composite layers have been subjected to annealing by ruby laser (λ = 694 nm) in the spectral region on a descending long-wavelength wing of the plasmon absorption band of gold nanoparticles. Raman spectroscopy has been applied for the first time to the investigation of the modification of the shape of gold nanoparticles in LiF during laser annealing. The experimental Raman spectra are compared with calculated modes of in-phase bending vibrations generated in gold nanoparticles.     

Diffraction patterns and nonlinear optical properties of gold nanoparticles

Stable gold nanoparticles have been prepared by using soluble starch as both the reducing and stabilizing agents; this reaction was carried out at 40 °C for 5 h. The obtained gold nanoparticles were characterized by UV–Vis absorption spectroscopy, transmission electron microscopy (TEM) and z-scan technique. The size of these nanoparticles was found to be in the range of 12–22 nm as analyzed using transmission electron micrographs. The optical properties of gold nanoparticles have been measured showing the surface plasmon resonance. The second-order nonlinear optical (NLO) properties were investigated by using a continuous-wave (CW) He–Ne laser beam with a wavelength of 632.8 nm at three different incident intensities by means of single beam techniques. The nonlinear refractive indices of gold nanoparticles were obtained from close aperture z-scan in order of 10^?7 cm²/W. Then, they were compared with diffraction patterns observed in far-field. The nonlinear absorption of these nanoparticles was obtained from open aperture z-scan technique. The values of nonlinear absorption coefficient are obtained in order of 10^?1 cm/W.