高热膨胀Na2O-MgO-Al2O3-SiO2微晶玻璃的制备及性能研究

采用传统熔体冷却法制备了Na2O-MgO-Al2 O3-SiO2玻璃并采用整体析晶工艺制备了微晶玻璃.利用DSC、XRD、SEM等测试手段研究了微晶玻璃的析晶行为和显微结构,探讨了热处理制度对该体系微晶玻璃热膨胀系数、密度、抗弯强度、显微硬度等性能的影响.研究结果表明,当晶化温度为800℃时该体系微晶玻璃主晶相为颗粒状霞石晶体(NaAlSiO4);当晶化温度达到900℃时玻璃中开始析出镁橄榄石(Mg2SiO4)晶体;延长保温时间可显著促进析晶但对晶体种类没有影响.析晶后微晶玻璃的密度、热膨胀系数、抗弯强度和显微硬度值显著增加,其最高热膨胀系数可达14.1×10-6℃-1.所制备的微晶玻璃具有很好的机械性能,当热处理温度为1000℃时,其抗弯强度和显微硬度分别达160 MPa和7.8 GPa.     

Na2 O-B2O3-SiO2-CaO-P2O5-F生物微晶玻璃制备与性能研究

采用烧结法,选用Na2O-B2O3-SiO2为基础玻璃(NBS),按照氟磷灰石组成配比添加CaO,P2O5,CaF2三种组分,制备Na2O-B2O3-SiO2-CaO-P2O5-CaF2生物微晶玻璃.利用差热分析、X射线衍射分析及扫描电镜等测试手段对微晶玻璃物相、微观结构进行了测试和分析,并采用模拟体液对样品的生物活性进行了验证.结果表明:随着热处理温度升高,样品的晶化程度逐步提高,当热处理温度在750℃时,可以获得主晶相为氟磷灰石,晶粒尺寸在100 nm左右、其晶化率≥80;的微晶玻璃样品,通过模拟体液浸泡实验证明了样品具有一定的生物活性.     

烧结法制备高炉渣CMAS系统微晶玻璃的研究

利用高炉渣及其它辅助原料制备基础玻璃,采用一步烧结法制备主晶相为辉石的CaO-MgO-Al2O3-SiO2(CMAS)微晶玻璃.综合运用DSC,XRD以及场发射扫描电子显微镜等测试手段,分析热处理制度对高炉渣CMAS微晶玻璃的析晶行为及性能的影响.结果表明:随着热处理温度上升,微晶玻璃的主晶相均为辉石,次晶相均为长石,晶相析出量增加,微晶玻璃的体积密度及抗折强度均呈现先增后减趋势.随着热处理时间增加,微晶玻璃的体积密度及抗折强度均呈现下降趋势.当热处理温度为1020 ℃,晶化时间30 min时,样品的机械性能最好,体积密度为2.690 g·cm-3,抗折强度为67.00 MPa.     

Li2O-ZnO-Al2O3-SiO2系微晶玻璃的烧结特性

采用收缩率、X射线衍射、扫描电镜对Li2O-ZnO-Al2O3-SiO2 (LZAS)系微晶玻璃的烧结特性、析晶特性及烧结后微晶玻璃试样的结构进行了研究.结果表明:LZAS微晶玻璃在530～560℃烧结时,析出的主晶相为γⅡ-LZS,γ0-LZS和方石英为次晶相.在590℃烧结时开始析出β-石英固溶体.620℃以上温度烧结时,析出的主晶相为γ0-LZS和β-石英固溶体,方石英为次晶相.LZAS系微晶玻璃的烧结属于粘滞性流动烧结,试样在470～590℃的温度区间完成烧结,但烧结温度高于530℃时由于试样析晶导致烧结收缩出现"滞缓"现象,590℃以上温度烧结时试样出现了流散.     

热处理制度对透辉石微晶玻璃析晶与导热性能的影响

以SiO2、CaO和MgO为主要原料,采用传统高温熔融工艺制备了基础玻璃,并通过一步析晶热处理工艺制备了透辉石微晶玻璃.利用X射线衍射仪、电子扫描显微镜和激光导热仪分别研究了热处理温度和时间对透辉石微晶玻璃析晶和导热性能的影响.结果表明:随着热处理温度的升高,微晶玻璃的结晶度增加,晶粒尺寸增大,导热系数先增大后减小;随着热处理时间的延长,微晶玻璃的晶粒尺寸增大,导热系数先增大后减小.当热处理温度890℃,热处理时间120 min,升温速率为10℃/min,微晶玻璃晶粒尺寸为0.3～0.4μm,结晶度为79;,导热系数达到最大值2.59 W/(m·K).     

CaO对MgO-Al2O3-SiO2系微晶玻璃结构与性能的影响

以化学纯试剂为原料,采用熔融法制备MgO-Al2O3-SiO2(MAS)系微晶玻璃.利用DSC、XRD、SEM等及理化性能测试手段研究了不同CaO含量对微晶玻璃析晶行为、物相组成、显微结构及理化性能的影响.结果表明:一定含量的CaO可以降低析晶活化能,促进玻璃析晶;随CaO含量的增加,微晶玻璃主晶相由假蓝宝石向α-堇青石转变,晶体形貌由棒状晶转变为枝状晶,晶粒尺寸呈先减后增的趋势;当CaO含量为3wt;时微晶玻璃热膨胀系数和相对介电常数(εr)达到最低,分别为3.89×10-1℃-1和10.09(1 MHz);当不外添CaO时微晶玻璃Vickers硬度达到最大,为10.52 GPa.     

废渣微晶玻璃析晶行为分析及热处理制度的优化

以镍渣及粉煤灰为主要原料,使用熔融法制备了复合渣微晶玻璃,渣的综合利用率达到62;,依据DSC曲线确定基础玻璃的热处理制度,并利用修正的JMA方程,对其进行了析晶动力学分析.借助极差分析、XRD、SEM等测试方法探讨了热处理制度对该系统微晶玻璃的影响.结果表明:复合渣微晶玻璃析晶活化能E=91.4 kJ/mol,动力学参数k(Tp)=0.277,n=3.04,该微晶玻璃以体析晶的方式析晶且析晶能力较强,主晶相为普通辉石和透辉石;热处理制度对玻璃体系的微观组织结构及力学性能均有较大影响,且温度因素大于时间因素;经730℃保温1.5h微晶化热处理后能获得晶粒细小均匀、力学性能良好的复合渣微晶玻璃.     

CaO-MgO-Al2O3-SiO2-P2O5-(F)微晶玻璃的析晶及特征

采用熔融法制备了不同P2O5及F含量的CaO-MgO-Al2O3-SiO2-P2O5-(F)基础玻璃试样,研究了CaO-MgO- Al2O3-SiO2-P2O5-(F)系微晶玻璃的析晶及特征.结果表明:在CaO-MgO-Al2O3-SiO2-8.0wt;P2O5玻璃中,表面析晶和内部析晶同时存在,析出晶体主要为钙长石(CaAl2Si2O8)相、硅灰石(CaSiO3)和α-磷酸钙(Ca3(PO4)2).玻璃中P2O5含量的提高抑制玻璃的表面析晶,同时促进了玻璃的整体析晶和α-磷酸钙晶体析出.同时添加P2O5和F的玻璃试样以整体析晶为主,析出晶体为块状氟磷灰石和粒状钙长石相.     

P2O5对CaO-MgO-Al2O3-SiO2系微晶玻璃析晶的影响

采用熔融法制备了不同P2O5含量的CaO-MgO-Al2O3-SiO2玻璃样品,研究了P2O5对该系微晶玻璃析晶的影响规律.结果表明:在所研究的CaO-MgO-Al2O3-SiO2玻璃中,P2O5的最大溶解量在10.0;质量分数左右,超过其饱和溶解度后将析出α-磷酸钙相.玻璃中添加4.0;质量分数P2O5时以表面析晶为主,析出晶体为钙长石和少量硅灰石.随着P2O5含量的提高, α-磷酸钙逐渐析出,同时钙长石和硅灰石的析出逐渐降低.进一步提高P2O5含量抑制了玻璃的表面析晶,促进了玻璃的分相和整体析晶.当P2O5的含量达到10;时,玻璃以整体析晶为主,在分相区内外区域析出晶体的形态非常相似,均呈现为细小粒状.     

透辉石微晶玻璃的低温烧结制备及性能表征

以废弃建筑玻璃为主体原料,将废玻璃粉、高岭土和氧化镁进行球磨混和,压制成型后直接烧结,在低温下成功制备出具有单一透辉石晶相结构的微晶玻璃.采用X射线衍射、场发射扫描电子显微镜等测试手段,研究了MgO加入量和烧结温度对微晶玻璃样品的晶相组成、显微结构及性能等的影响.结果表明:随着MgO加入量的增多以及烧结温度的升高,微晶玻璃的体积密度和抗弯强度均呈现先增大后减小的趋势.MgO加入量和烧结温度的提高可以有效促进透辉石晶相的析出.当MgO加入量为4;、975℃烧结2 h时所制备得到的透辉石微晶玻璃性能最好,其体积密度为2.395 g·cm-3,抗折强度102.1 MPa.     

Ultraviolet Absorption of Hg2Cl2-and Hg2Br2 Single Crystals

The optical unpolarized absorption spectra of Hg₂Cl₂ and Hg₂Br₂ single crystals were measured in the spectral range 230–400 nm. A sharp exciton peak and other absorption bands of both halides were observed near the fundamental absorption edge. The absorption peaks due to the splitting of the halogen doublet were also observed. Positions of the exciton peaks are characteristic for the Frenkel (localized) type of excitons. Possible interpretations of the other observed bands are discussed.     

Crystal structure of Rb2[GeO2(OH)2]·2H2O

Single crystals of Rb₂[GeO₂(OH)₂] · 2H₂O are studied by X-ray diffraction. The crystals belong to the orthorhombic system, sp. gr. Pna2₁, a = 13.523(6) Å, b = 8.143(4) Å, c = 13.407(6) Å, Z = 8, R ₁ = 0.0506. In [GeO₂(OH)₂]^2? anions, the Ge-O distances (1.71–1.73(1) Å) are shorter than the Ge-OH distances (1.76–1.80(1) Å). Anions are linked to each other by pairs of hydrogen bonds to form infinite chains. The chains are linked by hydrogen bonds involving water molecules to form a 3D structure. The assignment of the bands in the IR spectrum of the compound under study is performed.     

Optical Properties of MnIn2S2Se2 Single Crystals

Optical transmittance and reflectance spectra of MnIn₂S₂Se₂ single crystals are measured in the wavelength range from 0.5 to 30 μm. The interference method is used to determine the refractive index of the compound for wavelengths between 0.8 and 12 μm. From an analysis of the absorption spectrum it follows that the fundamental edge is due to forbidden indirect transitions between parabolic bands for the polarization E ⊥ c with a gap energy of 1.50 eV at room temperature.     

Identification of a new family of diphosphate compounds, AI2BII3(P2O7)2: Structures of Ag2Co3(P2O7)2, Ag2Mn3(P2O7)2, and Na2Cd3(P2O7)2

Syntheses and single-crystal X-ray structural results are reported for three new mixed diphosphates of the family A^I ₂B^II ₃(P₂O₇)₂; Ag₂Co₃(P₂O₇)₂ (I), Ag₂Mn₃(P₂O₇)₂ (II), and Na₂Cd₃(P₂O₇)₂ (III). All crystallize in the triclinic system, space group P1 bar: (I) a = 5.351(4), b = 6.375(4), c = 16.532(4) Å, = 80.83(6) = 81.45(4), = 72.87(5)°, V = 528.9(6) ų, Z = 2, D _calc = 4.649 mg/m³, R/Rw = 0.0428/0.0548 for 3949 obs. reflns; (II) a = 5.432(7), b = 6.619(6), c = 16.51(3) Å, = 80.78(8) = 82.43(9), = 72.82(7)°, V = 557.7(13) ų, Z = 2, D _calc = 4.338 mg/m³, R/Rw = 0.0679/0.1303 for 2100 obs. reflns and (III) a = 5.67(3), b = 7.08(4), c = 7.90(4) Å, = 77.0(2), = 82.5(2), = 67.8(2)°, V = 286(3) ų, Z = 2, D _calc = 4.249 mg/m³, R/Rw = 0.0307/0.0342 for 1945 obs. reflns. (I) and (II) are isostructural but (III) is of a different type. All three structures are characterized by layers of P₂O₇ groups alternating with layers of mixed metal atoms. Differences are seen in the conglomerate bonding patterns of B atoms and in the irregular geometry of Ag in (I) and (II) compared to the octahedral bonding seen for Na in (III). The differences in structure may be understood in terms of the ratios of the ionic radii of A and B atoms.     

Dissociation of LiAlO2 and LiGaO2

The thermodynamic calculations of dissociation of LiAlO₂ and LiGaO₂ as function of temperature and oxygen pressure are presented. It has been found that LiGaO₂ evaporates congruently at the melting point under the oxygen pressure equal to 1 · 10^—5 atm. LiAlO₂ evaporates incongruently, the equilibrium oxygen partial pressure at the melting point is equal to 9.6 · 10^—5 atm and the partial pressure of Li and Al oxides decrease with increasing of oxygen pressure.     

The Improvement of Superconductivity in PbxBi2-xSr2CaCu2Oy

In this paper we present the results of recent studies on the improvement of superconductivity in Pb_xBi_2-xSr₂CaCu₂O_y single crystals by preventing impurities incorporation, employing ZrO₂ crucible for crystal growth and post annealing the as-grown crystals in vacuum or argon. It is realized that the superconductivity of as-grown crystals is improved.     

Synthesis and characterization of (NH4)2CuBr2Cl2·2H2O crystals

Single crystals of a new compound, (NH₄)₂CuBr₂Cl₂.2H₂O, were grown from saturated aqueous solution at room temperature by slow evaporation method. The grown crystals were characterized through elemental, powder XRD, thermal and DSC analyses and FTIR and far IR spectra. The elemental analysis and the decomposition pattern formulated using the TG‐DTG studies confirm the stoichiometry of the compound. The crystallinity of the compound is confirmed from the powder XRD pattern. A preliminary single crystal X‐ray diffraction structural analysis reveals that the title compound belongs to the orthorhombic system with a = 7.7466 Å, b = 7.783 Å and c = 8.1211 Å. The low temperature DSC shows thermal anomalies at –161.1, –156.5, –152.4, –145.2, –134, –18.5, and 1.4°C during the heating run and at –4.3, –54.8, –66.1, –90.6, –109.7 and –147.2 °C during the cooling run. The thermal hysterses indicate first order phase transitions in the title compound at these temperatures. The FTIR spectra were used to assign the characteristic vibrational frequencies due to NH₄⁺, CuX₄^2– ions and other chemical bonds. The effect of substitution of two bromine atoms on the phase transitions of a closely related crystal, diammonium tetrachloro cuprate dihydrate is also discussed. (© 2005 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Ru掺杂MoS2对SO2F2和H2S气体吸附的第一性原理研究

本文基于第一性原理探讨了Ru掺杂的单层MoS₂(Ru-MoS₂)的结构及其对SF₆绝缘设备中的两种主要分解气体SO₂F₂和H₂S的传感和吸附行为。Ru原子进入硫空位从而产生Ru-MoS₂,结果表明,Ru-MoS₂对SO₂F₂和H₂S气体的吸附能(E_ad)分别为-1.52和-2.11 eV,属于化学吸附。通过能带分析(BS)和态密度(DOS)分析进一步证明了两个体系的吸附性能,并阐述了Ru-MoS₂用于电阻式气体传感器时的气体吸附传感机制。除此之外,本文在理论上探索了不同温度下Ru-MoS₂解吸附SO₂F₂和H₂S的恢复时间,在598 K温度下,SO₂F₂吸附体系的恢复时间为6...     

Optical properties of the germanate melilites Sr2MgGe2O7, Sr2ZnGe2O7 and Ba2ZnGe2O7

Refractive indices and their dispersion in the wavelength range from 365 nm to 2325 nm and transmission ranges of the tetragonal melilite‐type germanates Sr₂MgGe₂O₇, Sr₂ZnGe₂O₇ and Ba₂ZnGe₂O₇ were determined. The uniaxial positive crystals Sr₂MgGe₂O₇ and Ba₂ZnGe₂O₇ both offer the possibility for phase matched second harmonic generation, a detailed analysis of phase matching conditions is given. The refractive indices of Sr₂ZnGe₂O₇ show an isoindex (isotropic) point at 467 nm. The investigation was performed on Czochralski grown large single crystals. The crystal structure of all three germanates were determined by means of X ‐ray diffraction. The results corroborate unmodulated melilite‐type structures at room temperature. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)