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.     

阳离子对硅酸盐玻璃激光拉曼光谱影响的研究

运用拉曼光谱技术研究了Na2O(K2O)—CaO(MgO)—SiO2,Na2O(K2O)—Al2O3—SiO2,Na2O(K2O)—B2O3—SiO2,Na2O(K2O)—PbO—SiO2和PbO—BaO—SiO2五个系统的玻璃。结果表明,阳离子对玻璃近程结构的改造会引起拉曼特征的变化。部分样品是根据古玻璃平均成分在实验室烧制的,这项研究对于运用激光拉曼光谱区分不同系统的古代硅酸盐玻璃有重要意义。     

惯性约束聚变靶丸玻璃微观结构的分子动力学模拟北大核心CSCD

使用分子动力学方法模拟惯性约束聚变(ICF)玻璃微球靶丸材料的碱金属硼硅酸盐玻璃,研究了不同SiO2与B2O3和不同Na2O与B2O3物质的量比的微观结构,包括键长、键角、配位数以及空穴的分布情况。通过模拟发现,在不同组分的碱金属硼硅酸盐玻璃中,硅原子的网络体结构相对稳定,硼原子的结构会随着成分的变化发生明显变化。同时,针对实际的ICF实验中对玻璃微球充入惰性气体氩的问题,模拟发现,当SiO2与B2O3物质的量比为40.5,Na2O与B2O3物质的量比为17.4,8.5,4.2时,玻璃中存在有较多的供氩扩散的空穴。     

二元钠硅酸盐玻璃及其熔体微结构的高温拉曼光谱及核磁共振研究

本文采用拉曼光谱研究不同配比的二元钠硅酸盐玻璃,结果显示碱金属阳离子的浓度影响结构中桥氧的含量,且不同初级结构Qi具有不同的特征峰。对Na2O·3SiO2玻璃进行高温拉曼和核磁共振研究,分别采用精细结构Qjklmi(m1h,m2q,m3t)和Qjklmi取代初级结构Qi进行解谱拟合和结构分析得到得到初级微结构单元的实际分布,结合量化分析结果计算其拉曼散射截面,定量分析Na2O·3SiO2玻璃及熔体在升温状态下结构随温度的变化。从室温到到熔态,Qi结构之间存在动态平衡,Na2O·3SiO2玻璃随着温度的升高从玻璃态到高弹态,最后经历粘流态到熔态。     

以Eu-苯甲酸-1,10-菲咯啉为掺杂剂的SiO2,SiO2-B2O3和SiO2-B2O3-Na2O体系材料的结构及Eu3+的发光性质

用溶胶-凝胶法制备以Eu-苯甲酸-1,10-菲咯啉为掺杂剂的SiO2,SiO2-B2O3和SiO2-B2O3-Na2O为基质的发光材料.材料经1000℃退火处理后,结构十分稳定.通过激发光谱和发射光谱、红外光谱、TEM、XRD研究了基质结构对Eu3 发光性能的影响.结果显示:在589和614 nm处显示Eu3 的特征发射带,对应于Eu3 的5D0→7Fj(j=1,2)跃迁;与直接掺入EuCl3的玻璃材料相比,以Eu-苯甲酸-1,10-菲咯啉为掺杂剂的玻璃材料,虽然Eu的掺杂量较小,但Eu的发光强度较大.与以SiO2为基质的玻璃材料相比,以SiO2-B2O3为基质的玻璃材料Eu3 的发光减弱,其红外光谱显示形成Si-O-B键,说明该结构对Eu3 的发光有猝灭作用,以SiO2-B2O3-Na2O为基质的玻璃材料Eu3 的发光明显增强,其红外光谱显示不存在SiOB键的振动吸收,可能是Na取代B的位置,形成Si-O-Na键,此结构对Eu3 的发光有一定的增强作用.     

偏磷酸钙玻璃陶瓷的Raman光谱分析

测量了Ca/P摩尔比为0.45的偏磷酸钙玻璃及其在300~700℃下结晶化处理获得玻璃陶瓷的拉曼光谱,对谱峰的振动模式进行了指认,利用拉曼振动频率计算了P—O键长。光谱分析发现偏磷酸钙玻璃在300℃已经开始了结晶相变,不同温度下,sν(PO2)和sν(POP)谱带的振动频率基本不变,随着温度提高,谱峰强度增加,并出现了精细的指纹结构;玻璃陶瓷的表面和内部的结构不同,表面结晶化程度高于内部;结晶过程中,P—O键平均键长会发生变化,随着结晶化程度的提高,骨架上(POP)的P—O键平均键长减小,由159.96 pm变为158.27 pm,侧链(PO2)上的P—O键长增大,由147.90 pm变为149.02 pm。     

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。     

碲酸盐玻璃的拉曼光谱研究

本文测试了TeO2-ZnO和TeO2-BaO两种二元系统不同金属氧化物浓度下玻璃的拉曼光谱,通过比较这两种碲酸盐玻璃系统拉曼光谱的异同,表明碲酸盐玻璃系统中随着金属氧化物浓度的增加,使玻璃网络中的TeO4双三角锥向TeO3三角棱锥转化,并且在TeO2-BaO二元玻璃中出现了非桥氧键。同时初步研究了TeO2-ZnO-Na2O三元玻璃的拉曼光谱,发现当TeO2-ZnO二元玻璃中加入5mol%的Na2O时,其结构并没有发生显著的变化。     

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。     

共溅射和离子注入制备的SiO_2(Eu)薄膜中Eu~(3 )到Eu~(2 )的转变

采用共溅射方法和Eu离子注入热生长的SiO2 方法得到SiO2 (Eu)薄膜 ,Eu离子的浓度为 4%和 0 .5 % .对样品X射线吸收近边结构 (XANES)的研究和分析表明 ,在高温氮气中发生了Eu3 向Eu2 的转变 .SiO2 (Eu)薄膜高温氮气退火下蓝光的发射证明了这一结论     

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 …

本文采用步辐射的ＳｉＫ－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该成分的玻璃体系中由于压力的变化所诱导Ａｌ配位的     

Investigation of the structural distortion in FeSex crystals by X-ray absorption near edge structures (XANES) spectroscopy

Crystals of the new superconductor FeSe were investigated by X-ray absorption near edge structures spectroscopy (XANES) in the temperature range 300-77 K. Crystals with Se content varying from x=1-0.8 were used. The Fe K-edge spectra show a structure distortion and increase in hole content as x decreases. The Fe K-edge spectra also show changes when the crystals are cooled to 100 K which may be related to the orthorhombic distortion reported in these crystals. The data is examined in conjunction with XRD measurements on the crystals to seek a correlation.     

Combined 17O NMR and 11B-31P double resonance NMR studies of sodium borophosphate glasses

17O enriched sodium borophosphate glasses were prepared from isotopically enriched NaPO3 and H3BO3. These glasses have been studied by 17O, 11B and 31P NMR including 17O and 11B multiple quantum magic angle sample spinning (MQMAS), 11B-31P heteronuclear correlation (HETCOR) NMR and 11B{31P} rotational echo double resonance (REDOR). For comparison, the crystalline borophosphates BPO4 and Na5B2P3O13 were included in the investigations. The latter compound shows three sharp 31P resonances at -0.2, -2 and -8 ppm and two BO4 sites that can only be resolved by MQMAS. The 17O NMR spectra were recorded using both the static echo method at medium magnetic field (9.4 T) as well as MAS and MQMAS methods at high field (17.6 T). In total, five oxygen sites were identified in these borophosphate glasses: P-O-P, Na...O-P, P-O-B, B-O-B, Na...O-B. However, these five sites are not present simultaneously in any of the glasses. The 17O MQMAS spectra prove that P-O-B links play a major role in borophosphate glasses. These results are confirmed by the complementary 11B MAS spectra that show the presence of asymmetric and symmetric trigonal groups BO3a and BO3s and two tetrahedral BO4 units. 11B{31P} REDOR NMR is used to give independent information to assign the 11B lines to structural units present in the glasses. These REDOR measurements reveal that B-O-P bonds are present for each borate unit, including the BO3 groups. Particularly, a structural proposal for the two different BO4 resonances is given in terms of a different number of bonded phosphate tetrahedra. The 31P MAS spectra are usually broad and not well resolved. It is shown by 11B-31P HETCOR NMR that a possible structural assignment of a 31P signal at about -20 ppm to Q2 units as in binary sodium phosphate glasses is wrong and that the phosphate tetrahedron belonging to this resonance must be connected to borate groups.     

Modelling the size of red-colouring copper nanoclusters in archaeological glass beads

The origin of a red colour in ancient soda-lime glasses has been attributed either to the presence of both copper clusters and cuprous oxide or to copper alone. As a contribution to this question, a non-destructive X-ray absorption study at the [ _Cu]K-edge was undertaken on the red layer from a singular “rosette”-type archaeological glass bead dated as pre-XVII century. On comparing with data collected from metallic copper and the mineral cuprite, cubic Cu₂O, XANES spectra of the red glass are identical to the first. Theoretical modelling of Cu 1s XANES spectra was undertaken using the FEFF code based on a multiple scattering formalism. A hypothetical tetragonal structure was simulated for Cu₂O in order to remove the constraints arising from linear O–Cu–O bonds, unstable within the silica glass matrix, and an ideal body-centred array was considered on the basis of real metallic Cu–Cu distances in the metal. Calculations were performed for atom clusters of variable size within real and hypothetical structures. A spherical cluster of about 5 Å radius, capped by 24 copper atoms already provides a calculated Cu 1s XANES spectrum that compares well with data collected from the red glass. Post-edge details are noted in relation to the oxide, considering ionic states and effective valences of copper. The possibility of estimating the size of copper clusters through simulated structures is discussed.     

Structure of alkali borate glasses at high pressure: B and Li K-edge inelastic X-ray scattering study

We report the first in situ boron K-edge inelastic x-ray scattering (IXS) spectra for alkali borate glasses (Li2B4O7) at high pressure up to 30 GPa where pressure-induced coordination transformation from three-coordinated to four-coordinated boron was directly probed. Coordination transformation (reversible upon decompression) begins around 5 GPa and the fraction of four-coordinated boron increases with pressure from about 50% (at 1 atm) to more than 95% (at 30 GPa) with multiple densification mechanisms, evidenced by three distinct pressure ranges for (d[4]B/dP)T. The lithium K-edge IXS spectrum for Li-borate glasses at 5 GPa shows IXS features similar to that at 1 atm, suggesting that the Li environment does not change much with pressure up to 5 GPa. These results provide improved understanding of the structure of low-z glass at high pressure.     

A 125Te and 23Na NMR investigation of the structure and crystallisation of sodium tellurite glasses

125Te static nuclear magnetic resonance (NMR) and 23Na and 125Te magic angle spinning (MAS) NMR have been used, in conjunction with X-ray diffraction, to examine the structure and crystallisation behaviour of glasses of composition xNa2O.(1-x)TeO2 (0.075 x 0.4). The MAS NMR 23Na spectra from the glasses are broad and featureless but shift by approximately +5 ppm with increased x, i.e. as the system becomes more ionic. The static 125Te NMR spectra show an increase in axial symmetry with increasing x, indicating a shift from predominantly [TeO4] to [TeO3] structural units. The 23Na and 125Te spectra from the crystallised samples have been fitted to obtain information on the sites in the metastable crystal phases, which are the first to form on heating and which are therefore more closely related to the glass structure than thermodynamically stable crystal phases. New sodium tellurite phases are reported, including a sodium stabilised, face centred cubic phase related to delta-TeO2; a metastable form of Na2Te4O9 containing 3 sodium and 4 tellurium sites; and a metastable form of Na2Te2O5 containing 2 sodium sites. There is evidence of oxidation of TeIV to TeVI occurring in glasses with high values of x and, at x=0.40 and 0.50 (outside the glass forming range), some sodium metatellurate (Na2TeO4) is formed at the same time as sodium metatellurite (Na2TeO3). The 125Te shift is very sensitive to environment within the sodium tellurite system, covering more than 320 ppm, with anisotropies varying from 640 to 1540 ppm. The lack of features in the 125Te spectra of the glass phases, combined with the large shift range and high but variable anisotropy, means than it is not possible to obtain a unique fit to any presumed species present. Furthermore, the chemical shift anisotropy parameters for three of the four Te sites in the Na2Te4O9 phase are found to lie outside the range used for previous simulations of glass spectra.     

Preparation and optical spectroscopy of phosphate glasses containing divalent europium ions

P2O5.BaO.Na2O.K2O glasses doped with various content of Eu2O3 were prepared using high temperature melting method, and the Eu2+ ions in the phosphate glasses were obtained with the aid of the reductive action of silicon powder. The fabricating conditions, fluorescence, excitation spectra of the glasses were then studied. The glasses containing europium show a broad emission band at 450 nm and sharp bands from 580 to 650 nm, and the co-existence of Eu2+ and Eu3+ is identified. Also, a good glass with a dominant proportion and large quantity of Eu2+ ions can be obtained by the reductive action of silicon powder and proper processing.     

XANES and EXAFS in Cu-Ti and Ni-Zr glasses

X-ray absorption near edge structure (XANES) and extended X-ray absorption fine structure (EXAFS) measurements have been done at the K-edge of Cu in Cu-Ti glasses and on the K-edges of Ni and Zr in Ni-Zr glasses using a synchrotron radiation source. The results are discussed in terms of the shape shift and intensity of the absorption edge as well as the principal absorption maximum. The values of bondlength calculated by the one-electron multiple scattering XANES theory as well as the graphical analysis EXAFS technique show good agreement.     

Magnesium K‐edge XANES spectroscopy of geological standards

Magnesium K‐edge X‐ray absorption near‐edge structure (XANES) spectra have been investigated to develop a systematic understanding of a suite of Mg‐bearing geological materials such as silicate and carbonate minerals, sediments, rocks and chemical reagents. For the model compounds the Mg XANES was found to vary widely between compounds and to provide a fingerprint for the form of Mg involved in geologic materials. The energy positions and resonance features obtained from these spectra can be used to specify the dominant molecular host site of Mg, thus shedding light on Mg partitioning and isotope fractionation in geologic materials and providing a valuable complement to existing knowledge of Mg geochemistry.     

X-ray absorption spectroscopic study of a hot pressed MgB2

X-ray near edge absorption spectra (XANES) of boron and oxygen K edge of a hot-pressed MgB₂ (HP2) sample were measured by using synchrotron radiation. The HP2 was produced by annealing a commercial powder of MgB₂ in ambient air under a hydrostatic pressure of 2.0 GPa at 900 °C. No substantial change of the electronic structure in HP2 was observed as indicated in the B K-edge XANES. This sample maintains high superconductivity and enhances the critical current density. The XANES and the XRD combined indicate that both MgO and B₂O₃ in HP2 increase and more B₂O₃ than MgO was produced during the hot-press process. The better connection of the grain in HP2 can be the major cause to increase its critical current density. However, the impurity may also increase the flux pinning and therefore increases the current density.