锂铝硅磷酸盐玻璃结构与紫外透过性能的关系

利用傅里叶红外光谱仪(FT-IR)、紫外分光光度计(UVPC)和魔角变换核磁共振(MAS-NMR)等方法对锂铝硅磷酸盐玻璃的局部结构和紫外透过性能进行了研究和表征。添加适量Li2O替换P2O5构成新的玻璃网络。通过核磁共振光谱分析表明,玻璃中的硅和磷分别处于四配位和三配位的配位态,而铝则有四配位、五配位和六配位三种不同的配位态。随着Li2O含量的增加,铝的平均配位数逐渐降低,这表明体系中的铝从网络修饰体变成了网络形成体。通过红外光谱分析表明,铝氧四面体中的铝和硅形成了Si-O-Al键,也使P-O-Al键逐渐增多。这些提高了玻璃的联通性,使玻璃结构更加完整。因此,玻璃在200nm处的透过率逐渐升高,这得益于Al-O-T(T=Si,P)键由非桥氧键变成桥氧键。     

在硅酸盐矿物,玻璃和熔体中Si和Al的配位与局部结构:K-边X射线吸收光谱研究

本文采用同步辐射的Si K-边X-射线吸收近边结构(XANES)谱研究了Si在SiO2-P2O5和Na2O-SiO2-P2O5的低压磷硅酸盐玻璃中结构与配位,以及Si的配位几何随玻璃中P2O5含量而变化:同步辐射的Al K-边XANES谱研究了Al在铝硅酸盐成分为NaAlSi2O6-NaAlSi3O8的玻璃和熔体中的配位和局部结构,并提供了直接的实验证据来证明该成分的玻璃体系中由于压力的变化所诱导Al配位的变化.     

高掺杂稀土PBA玻璃的制备及其化学稳定性研究

稀土掺杂磷酸盐玻璃具有优异的光学和光谱特性,在激光介质材料、有色滤光材料等领域中有着重要的应用。在研究P2O5-BaO-Al2O3-Sm2O3(PBAS)玻璃形成能力的基础上,借助NMR、红外吸收光谱等分析手段,研究了玻璃的结构特点以及在各种化学介质条件下玻璃的化学稳定性能、玻璃的组成和结构对化学稳定性的影响。结果表明:玻璃结构主要由磷氧四面体[PO4]3-和铝氧八面体[AlO6]3-构成;Al3+含量越高,玻璃结构越稳定,玻璃的耐水性和耐酸性也越好;玻璃结构中阳离子的极化能力越强,玻璃的耐酸性越好,侵蚀过程中玻璃表面形成的“缺碱层”在一定程度上减缓了化学介质的侵蚀程度;在碱性介质中,磷酸盐长链末节的金属离子被水化,产生P—O—P断键,形成正磷酸盐溶解到溶液中,稀土离子含量的增加,在一定程度上恶化了玻璃的耐碱性能。     

Eu2+掺杂硼硅酸镁玻璃的发光性能

利用高温固相法合成了Eu2+掺杂的新型蓝色硼硅酸盐发光玻璃,讨论了不同掺杂浓度下硼硅酸镁玻璃体系中Eu-O键共价性的变化以及氧原子周围不同配位环境对MgO-SiO2-B2O3玻璃发光性能的影响.利用X射线衍射仪和荧光光谱仪对该玻璃体系进行了结构表征和性能测试.在紫外-可见光激发下,Eu2+掺杂硼硅酸镁玻璃的荧光发射光谱...     

TeO_2-ZnO-ZnF_2三元碲酸盐玻璃的Raman光谱和X射线光电子能谱研究

采用高温熔融法制备了组分为TeO2-ZnO-ZnF2碲酸盐玻璃,利用Raman光谱和X射线光电子能谱研究了TeO2-ZnO-ZnF2三元碲酸盐玻璃的结构.结果表明,体系中存在[TeO4]双三角锥中Te-O-Te键或者O-Te-O键的振动、带有桥氧键的[TeO4]双三角锥振动、[TeO3]三角锥体中Te与非桥氧连接的Te-O键的对称伸缩振动,且随着氧化锌的加入,体系中[TeO4]双三角锥体向[TeO3]三角棱锥转化.     

分子动力学模拟不同组分下CaO-Al2O3-SiO2系玻璃微观结构的转变

采用分子动力学模拟的方法研究了CaO-Al2O3-SiO2系玻璃的微观结构,发现Ca/Al=1/2时CaO-Al2O3-SiO2系玻璃(网硅酸盐体系)并不像传统理论认为的那样是一个完整的三维网络,而是存在一定量的非桥氧,从而从理论上进一步证实了Stebins等人的实验结果.同时也发现不同的Ca/Al比对Si和Al键接方式产生重要影响,在Ca/Al＞1/2时,Al比Si容易成为网络的中间体,其首先插入网络体中间;在Ca/Al＜1/2时,Si比Al容易成为网络中间体.虽然在能量上Al-O-Si占有扰势,但当Ca/Al从大于1/2变化到小于1/2时,仍有部分Al-O-Si转变成Al-O-Al和Si-O-Si,丰富了Al自回避规则的内容.     

温度对CaO-MgO-Al_2O_3-SiO_2系纳米晶玻璃陶瓷结构影响的拉曼光谱研究

采用熔融法制备了CaO-MgO-Al2O3-SiO2系纳米晶玻璃陶瓷材料。在-190~310℃温度范围,利用显微共聚焦拉曼光谱测量分析了该体系纳米晶玻璃陶瓷硅氧四面体结构的变化规律。结果表明,随着温度的降低具有不同非桥氧键的硅氧四面体结构单元变化并不一致,位于三维硅氧四面体结构边缘的具有二个非桥氧键的硅氧四面体(Q2)和具有三个非桥氧键的硅氧四面体(Q1),以及完全独立于三维硅氧网络结构外的具有四个非桥氧键的硅氧四面体(Q0)受温度影响明显,其拉曼光谱均向高波数移动,键的力常数变强,硅氧键长变短。为丰富外环境对纳米晶玻璃陶瓷材料结构与性能影响的研究提供了实验依据,也为控制该体系纳米晶玻璃陶瓷材料的膨胀系数提供了一定的实验依据。     

分子动力学模拟不同组分下CaO-Al2O3-SiO2系玻璃微观结构的转变

采用分子动力学模拟的方法研究了CaO-Al₂O₃-SiO₂系玻璃的微观结构，发现Ca/Al=1/2时CaO-Al₂O₃-SiO₂系玻璃(网硅酸盐体系)并不像传统理论认为的那样是一个完整的三维网络，而是存在一定量的非桥氧，从而从理论上进一步证实了Stebins等人的实验结果.同时也发现不同的Ca/Al比对Si和Al键接方式产生重要影响，在Ca/Al>1/2时，Al比Si容易成为网络的中间体，其首先插入网络体中间；在Ca/Al<1/2时，Si比Al容易成为网络中间体.虽然在能量上Al—O—Si占有扰势，但当Ca/Al从大于1/2变化到小于1/2时，仍有部分Al—O—Si转变成Al—O—Al和Si—O—Si，丰富了Al自回避规则的内容. 关键词： 2O₃-SiO₂')" href="#">CaO-Al₂O₃-SiO₂ 玻璃 微观结构 分子动力学     

铝硅酸盐Raman活性分子振动解析

分别测定了蓝晶石、红柱石和硅线石三种铝硅酸盐天然矿物晶体以及K₂O-Al₂O₃-SiO₂三元铝硅酸盐玻璃的Raman光谱。构建了一组硅铝四面体聚集体结构模型,采用量子化学自洽场分子轨道从头计算的方法计算了其Raman振动频率。分析研究了上述Raman光谱振动特征,确定了特征谱峰的归属,解析了铝对铝硅酸盐Raman活性分子振动特征的影响。结果表明,随四配位铝的增加,导致800～1 200 cm-1波数区间内谱峰频率降低,该区间的谱峰是Si—O_nb间非桥氧对称伸缩振动引起的,其中不含Al—O振动;700～800 cm-1区间内出现的谱峰归属于Al—O_nb间非桥氧的对称伸缩振动。     

Eu^3+激活氟氧硼酸锗酸盐闪烁玻璃的发光性能

采用传统高温熔融法合成了玻璃组成为B2O3-GeO2-15GdF3-(40-x)Gd2O3-xEu2O3(0≤x≤10)的Eu^3+激活氟氧硼酸锗酸盐闪烁玻璃。在硼锗酸盐玻璃基质中,Gd2O3和GdF3稀土试剂的总含量高达55%,从而确保其密度高于6.4 g/cm^3。闪烁玻璃的光学性能通过光学透过光谱、光致发光光谱、X射线激发发射(XEL)光谱和荧光衰减曲线来表征。玻璃中Gd^3+→Eu^3+离子的能量传递通过激发光谱、发射光谱和Gd^3+-Eu^3+离子间距得到证明,同时也确定了在紫外线和X射线激发下Eu^3+激活氟氧硼酸锗酸盐闪烁玻璃的最佳浓度。Judd-Ofelt理论分析了玻璃中Eu―O键的共价性随Eu^3+掺杂浓度增加而显著增强。Eu^3+激活氟氧硼酸锗酸盐闪烁玻璃在80~470 K温度范围内荧光衰减曲线和发射光谱的温度依赖关系最终证实了其具有较好的发光稳定性。     

含稀土元素的矿渣纳米晶玻璃陶瓷的光谱学研究

利用白云鄂博矿资源废弃物中有价元素以共伴生形成存在的特点制备了高性能的矿渣纳米晶玻璃陶瓷。本文采用电感耦合等离子发射光谱（ICP）、X射线衍射（XRD）、拉曼光谱（Raman）、扫描电子显微镜（SEM）等测试方法对样品的成分和结构进行了深入分析。ICP和XRD、SEM实验结果表明,我们制备的玻璃陶瓷是主晶相为透辉石,晶粒尺寸在45～100nm范围含稀土元素的纳米晶玻璃陶瓷,SEM面扫所显示的元素与ICP成分分析结果较为一致。Raman分析表明,其非晶相主要由具有不同非桥氧键的硅氧四面体结构单元构成的三维网络结构,进一步分析发现稀土微量元素对网络结构有十分明显的影响。我们把矿渣纳米晶玻璃陶瓷与相似成分的玻璃陶瓷的拉曼光谱对比,发现矿渣纳米晶玻璃陶瓷的拉曼谱带普遍比玻璃陶瓷对应的拉曼谱带波数低。相似成分的玻璃陶瓷与矿渣纳米晶玻璃陶瓷的成分差别主要是稀土元素等微量元素。本文的研究方法为研究玻璃陶瓷的成分与结构、性能之间的关系提供了一种研究思路。     

FT-Raman spectroscopy study of solvent-in-salt electrolytes

Cation–anion interaction with different ratios of salt to solvent is investigated by FT-Raman spectroscopy. The fitting result of the C–N–C bending vibration manifests that the cation–anion coordination structure changes tremendously with the variation of salt concentration. It is well known that lithium-ion transport in ultrahigh salt concentration electrolyte is dramatically different from that in dilute electrolyte, due to high viscosity and strong cation–anion interaction. In ultrahigh salt concentrated "solvent-in-salt" electrolyte(SIS-7#), we found, on one hand, that the cation and anion in the solution mainly formed cation–anion pairs with a high Li~+coordination number(≥ 1), including intimate ion pairs(20.1%) and aggregated ion pairs(79.9%), which not only cause low total ionic conductivity but also cause a high lithium transference number(0.73). A possible lithium transport mechanism is proposed: in solvent-in-salt electrolytes, lithium ions' direct movement presumably depends on Li-ion exchange between aggregated ion pairs and solvent molecules, which repeats a dissolving and re-complexing process between different oxygen groups of solvent molecules.     

氟锆酸盐玻璃的γ射线辐照效应

用电子顺磁共振谱研究了在液氮温度及在室温下氟锆酸盐玻璃的γ射线辐照效应.实验结果表明,辐照后的玻璃中形成了Zr~(3+)、F_2、F~0及一种俘获氧杂质的空穴中心(标号为U)等缺陷.在低温辐照时,非桥氟的存在是产生F_2~-和F~0缺陷的原因.温度高于400K时,所有缺陷全部消失.常温下经γ射线辐照过的玻璃,在紫外区出现一个吸收峰.辐照对该玻璃的红外透过率影响不大.     

Influence of MgO on structure and optical properties of alumino-lithium-phosphate glasses

MgO doped lithium alumino phosphate glasses (PLA: P₂O₅+Li₂O+Al₂O₃+MgO) were prepared by melt quenching technique. Raman spectra display three significant peaks at 698, 1164 and 1383 cm⁻¹ attributed to: symmetric stretching vibrations of the bridging oxygen (BO) in the P–O–P chains, symmetric stretching vibrations of the PO₂ groups, and the asymmetric vibrations vas(PO₂) of the non-bridging oxygen (NBO) atoms, respectively. Also, the density, molar volumes and ion concentration have been discussed and correlated with the structural changes within the glassy matrix. Some optical constants such as refractive index and dispersion parameters (E_o: single-oscillator energy and E_d: dispersive energy) of the glasses were determined. Finally, the values of the optical band gap for direct and indirect allowed transitions have been determined from the absorption edge studies. It is deduced that the values of E_opt increase with increasing MgO content. It was assigned to structural changes induced from the formation of non-bridging oxygen. The Urbach energy (ΔE) was found to decrease from 0.578 to 0.339 eV with increasing MgO content from 0.5 to 2 mol.     

Elaboration and characterization of TiO2 nanoparticles incorporated in SiO2 host matrix

Nanometer-scale TiO₂ particles have been synthesized by sol-gel method. It was incorporated in a glass-based silica aerogel. The composite was characterized by various techniques such as particle size analysis, scanning electron microscopy (SEM), atomic force microscopy (AFM), transmission electron microscopy (TEM), X-ray diffraction (XRD), infrared spectroscopy (IR) and photoluminescence (PL). The bulk glass presents a strong luminescence at wavelengths ranging from 750 to 950 nm. This PL was attributed to various non-bridging oxygen hole centers (NBOHCs) defects resulting from thermal treatment and crystallization of TiO₂ at the interface between titania nanoparticles and silica host matrix.     

太赫兹波段金属线栅的紫外光控特性研究

基于氧化铟纳米薄膜及金属线栅的特性,利用紫外激光诱导以金属线栅为衬底的氧化铟纳米结构,研究其对于太赫兹偏振透射的调制特性。实验中在金属线栅上滴入溶于乙醇的氧化铟溶液,并使溶液恰好浸润在金属线栅缝隙中,同时将加热台的温度调至340 ℃,对金属线栅中的氧化铟进行热退火。结果表明,氧化铟-金属线栅线长方向与太赫兹电场偏振方向垂直时,在低强度紫外光的照射下,该样品对太赫兹的透射强度有较为明显的衰减,当紫外光功率密度为7 mW·cm-2时,样品对太赫兹的调制深度可达71%;当氧化铟-金属线栅线长方向与太赫兹电场偏振方向平行时,紫外光激发下的样品对太赫兹的调制效果明显减弱,当紫外光功率密度为7 mW·cm-2时,调制深度约为20%。氧化铟纳米薄膜中存在的氧空位,使该材料对紫外光具有特殊响应。在无紫外光照射下,样品环境中的氧气分子被吸附到氧化铟表面,由于化学反应生成O2-离子态。当用光子能量大于氧化铟禁带宽度的紫外光激发样品时,在氧化铟表面激发出电子空穴对,空穴会被氧化铟表面的O2-离子态和缺陷态束缚,从而释放电子到导带,增强了样品的电导率。在太赫兹波频段内,透过氧化铟样品的太赫兹强度与氧化铟电导率有很好的相关性。金属线栅利用金属表面可存在的自由电子的振荡, 使电场方向与线栅方向平行的太赫兹偏振光激发电子沿线栅方向振荡,当电子与金属晶格中的原子碰撞时,此偏振光发生衰减并伴随辐射;而电场方向与线栅方向垂直的太赫兹偏振光,由于周期性结构的限制,无法激发自由电子振荡, 主要表现出透射特性。结合氧化铟的表面缺陷特性,紫外光可实现作为氧化铟-金属线栅结构的光控偏振开关作用,氧化铟-金属线栅结构偏振器能很好地应用于太赫兹波频段的光控偏振调制。     

Luminescence of polymorphous SiO2

The luminescence of self-trapped exciton (STE) was found and systematically studied in tetrahedron structured silica crystals (α-quartz, coesite, cristobalite) and glass. In octahedron structured stishovite only host material defect luminescence was observed. It strongly resembles luminescence of oxygen deficient silica glass and γ or neutron irradiated α-quartz. The energetic yield of STE luminescence for α-quartz and coesite is about 20% of absorbed energy and about 5(7)% for cristobalite. Two types of STE were found in α-quartz. Two overlapping bands of STEs are located at 2.5–2.7 eV. The model of STE is proposed as Si–O bond rupture, relaxation of created non-bridging oxygen (NBO) with foundation of a bond with bridging oxygen (BO) on opposite side of c or x,y channel. The strength of this bond is responsible for thermal stability of STE. Similar model of STE was ascribed for coesite and cristobalite with difference related to different structure. STE of Silica glass is strongly affected by disordered structure.     

Sputter-deposited network glasses

Thin films of lithium borate, sodium borate, rubidium borate, and lithium silicate glasses are prepared by ion beam sputter deposition in a thickness range between 70 and 1,400 nm. The chemical, structural, and electrical properties of the films are determined by transmission electron microscopy and impedance spectroscopy. A comparison between the thin glass layers and the corresponding bulk glasses, prepared from the melt, shows that both have similar chemical compositions and atomic short range orders. In contrast, the ionic conductivities of the borate glass films are found to be significantly increased compared to the corresponding bulk materials, while the increase depends on the chemical composition of the glasses and is not observed in the case of the silicate system. We propose a modified network structure of the sputter-deposited glass layers, namely, an increased nonbridging oxygen concentration, to be responsible for the elevated ionic conductivity.     

Experimental routes to in situ characterization of the electronic structure and chemical composition of cathode materials for lithium ion batteries during lithium intercalation and deintercalation using photoelectron spectroscopy and related techniques

Three different experimental routes to in situ characterization of electronic structure and chemical composition of thin film cathode surfaces used in lithium ion batteries are presented. The focus is laid on changes in electronic structure and chemical composition during lithium intercalation and deintercalation studied by photoelectron spectroscopy and related techniques. At first, results are shown obtained from spontaneous intercalation into amorphous or polycrystalline V₂O₅ thin films after lithium deposition. Although this technique is simple and clean, it is nonreversible and only applicable to the first lithium intercalation cycle into the cathode only to be applied to host materials stable in the delithiated stage. For other cathode materials, as LiCoO₂, a real electrochemical setup has to be used. In our second approach, the experiments are performed in a specially designed electrochemical cell directly connected to the vacuum system. First experimental results of RF magnetron sputtered V₂O₅ and LiCoO₂ thin film cathodes are presented. In the third approach, an all solid-state microbattery cell must be prepared inside the vacuum chamber, which allows electrochemical processing and characterization by photoelectron spectroscopy in real time. We will present our status and experimental difficulties in preparing such cells.