HAc溶解碳酸盐岩测定87Sr/86Sr值实验方法研究

传统的碳酸盐岩的sr同位素比值测定因为采用HCl溶样,往往导致非碳酸盐组分的溶解,引起测定值偏高,采用HAc溶样可以防止样品中非碳酸盐组分的溶解,同时也避免过多的杂质离子进入溶解液,从而使^87Sr／^86Sr测定值趋于准确和可靠;通过2.5mol/L HAc溶解碳酸盐矿样和4.0mol/L HCl溶解残渣样的最后质谱测定的^87Sr／^86Sr值比较,证实碳酸盐岩中非碳酸盐组分的^87Sr／^86Sr值较碳酸盐组分高。     

Sr/Ca比变化对红色荧光粉Cal-xSrxS:Eu2+的影响

在CO气氛下采用固相反应法合成了发红光的Ca1-xSrxS:Eu2 荧光粉,研究了基质阳离子Sr/Ca比变化对其晶体性质及发光性能的影响.结果表明,随着Sr/Ca比的减少,荧光粉的晶胞参数逐渐降低;同时,由于受电子云膨胀效应和晶体场影响,发射主峰向长波方向移动,红色比逐渐增大,色纯度提高.     

巡游磁体Sr1-xCaxRuO3系列的磁性

固相反应法制备了Sr1-xCaxRuO3系列. PPMS测量了样品的零场冷却和加场冷却磁化强度和交流磁化率. 居里-外斯定律确定了样品的顺磁居里温度TP. 结果表明, 随x的增加, TP减小. 当x≤0.6时TP大于零; 当x>0.6时TP小于零. 利用交流磁化率随温度变化的关系确定样品的铁磁居里温度TC, 随x的增加TC减小. 当x=0.8时TC降至4 K; 而当x=1.0时, 即使温度降到1.7 K, 也未出现磁有序.     

可见光下高催化活性不同结构Sr/TiO2催化剂的制备和表征

采用分步沉积法制备不同Sr/Ti 摩尔比例的Sr/TiO₂催化剂, 以X射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)、傅里叶变换红外(FT-IR) 光谱、紫外-可见漫反射光谱(UV-Vis RDS)等手段对样品进行了表征, 以可见光催化降解亚甲基蓝为模型反应考察样品光催化活性. 结果表明, 催化剂的活性和结构随Sr/Ti 摩尔比(n(Sr)/n(Ti))的变化而变化, 当n(Sr)/n(Ti)≤3/2 时, 催化剂呈由TiO₂和SrTiO₃组成的球状结构; 而当n(Sr)/n(Ti)在3/2 与4/1 之间时, 催化剂呈片状结构, 且随着n(Sr)/n(Ti)增大, 催化剂组成由SrTiO₃ 和Sr₂₄ 变为Sr₂₄和Sr(OH)₂·H₂O; 当n(Sr)/n(Ti)=9/1 时, 催化剂呈以Sr(OH)₂·H₂O为主的针状结构. 其中, n(Sr)/n(Ti)=4/1的样品表现出最高的光催化活性, 一级反应速率为SrTiO₃钙钛矿催化剂的5.0倍, 商用P25的86.7倍.     

Sr／Ca比变化对红色荧光粉Ca1-xSrxS：Eu^2＋的影响

在CO气氛下采用固相反应法合成了发红光的Ca1-xSrxS:Eu^2 荧光粉，研究了基质阳离子Sr／Ca比变化对其晶体性质及发光性能的影响。结果表明，随着Sr／Ca比的减少，荧光粉的晶胞参数逐渐降低；同时，由于受电子云膨胀效应和晶体场影响，发射主峰向长波方向移动，红色比逐渐增大，色纯度提高。     

Sr3SiO5降温过程分解及对制备Sr3SiO5:Eu2+的影响

采用高温固相反应法制备Sr3SiO5:Eu2+时,往往有Sr2SiO4:Eu2+共存,从而影响Sr3SiO5:Eu2+的发光性能.本文采用DSC/TG、淬冷法结合XRD,研究了Sr3SiO5:Eu2+在降温过程中的分解反应.结果表明,Sr3SiO5是在1 250℃以上稳定存在的化合物,在降温过程中Sr3SiO5在1 250℃分解为Sr2SiO4和SrO.采用快速降温的方法可以抑制Sr3SiO5的分解.当降温速率小于10℃·min-1时,Sr3SiO5全部分解为Sr2SiO4和SrO;当降温速率为15℃·min-1时,样品主要物相为Sr3SiO5,但有少部分Sr3SiO5发生分解,当降温速率增大到20℃·min-1时,Sr3SiO5分解的量更少,即随着降温速率增大,Sr3SiO5分解的量减小,从而获得几近纯相的Sr3SiO:Eu2+荧光粉.     

Sr2+-TiO2薄膜的制备及超亲水性

以钛酸丁酯作为前驱物,采用溶胶-凝胶法及浸渍-提拉法在载玻片上制备SrO-TiO2薄膜。通过X射线衍射和红外光谱等测试技术表征了SrO-TiO2粉末的结构,用紫外可见分光光度计测定薄膜的透光率,用接触角测试仪测定水与薄膜的接触角。结果表明,掺杂适量Sr2+后,SrO-TiO2粉末中TiO2晶粒的尺寸变小,SrO-TiO2薄膜表面吸附的羟基含量增多且稳定,可提高TiO2薄膜的超亲水性。经紫外光照１ｈ或自然光照５ｈ后,掺杂Sr2+（摩尔分数））为1.0％的SrO-TiO2薄膜与水的接触角接近于0°,表现出良好的亲水性。     

Structure and Luminescence Characteristics of Europium Activated Strontium Silicates Sr（Eu ,Bi）SiO3 and Sr（Eu ,Bi）2SiO4

Sr2SiO4 ： Eu^3 , Bi^3 and SrSiO3 ：Eu^3 , Bi^3 samples were synthesized at high temperature and high pressure. The effect of high pressure on the structure and luminescence properties of the samples were stud-ied. As a comparison, the samples were also prepared by the method of sol-gel at high temperature and atmo-spheric pressure. The SrSiO3 ： Eu^3 , Bi^3 prepared at atmosphere has a hexagonal phase structure; in the pressure range of 2. 34—4. 10 GPa, it is transformed into a pseudo-orthorhombic structure (monoclinic), and in the pressure range of 4. 10—4. 15 GPa, the structure change of Sr2SiO4 ： Eu^3 , Bi^3 has not been ob-served, it maintains the monoclinic structure of the samples synthesized at an atmospheric pressure. High pressure makes the luminescence properties of the samples changed obviously. The intensity and the relative quantum luminescent efficiency decrease, the half-width increases obviously and the red shift occurs. The changes of the luminescence properties result from the pressure-induced changes of the crystal structures.     

Ba2CdMoO6及新化合物—Sr2CdMoO6晶体结构的研究

自从对Sr_2CaWO_6的相变和晶体结构研究以后,引起了我们对该类型化合物A_2~ⅡB~ⅡB~ⅥO_6的兴趣(A~Ⅱ=Ba~( 2),Sr~( 2);B~Ⅱ=Ca~( 2),Cd~( 2),Fe~( 2),Co~( 2),…;B~Ⅵ=W~( 6),Mo~( 6)),它们属于复杂的钙钛矿型结构,且具有一定的规律性。据文献[2]报导Ba_2CaWO_6属立方晶系,而文献[1]报导Sr_2CaWO_6低温相属正交晶系。在元素周期表中Mo和W同属于ⅥB族,它们的化学性质相似,二元素的离子半径也非常相近,Cd和Ca虽不同族,但离子半径很相近,化合价相同。为此,本文用Mo~( 6)代替W~( 6),Cd~( 2)代替Ca~( 2)来研究Ba_2CdMoO_6和Sr_2CdMoO_6的晶体结构。文献[3]对Ba_2CdMoO_6做了简单的报导,但Sr_2CdMoO_6则未见报导。     

Bi2Sr2CuO6的电子结构和铜氧对间电荷涨落

自发现含铋铜氧化物的高温超导性以来,采用各种复杂程度方法对电子结构的计算已经在文献中报道.它们集中讨论了能带结构,态密度和Fermi面的性质,但很少报道铜氧对间的电荷涨落。而价态变动对超导电性起着至关重要的作用,因此本文对Bi_2Sr_2CuO_6进行了紧束缚带计算,探讨了电子缺陷和氧呼吸式振动对铜和氧电荷分布的影响。     

Sm0.5Sr0.5CoO3阴极氧还原动力学

利用极化、交流阻抗技术考察了担载于La0.9Sr0.1Ga0.8Mg0.2O3(LSGM)电解质上的Sm0.5Sr0.5CoO3- La0.8Sr0.2Ga0.8Mg0.15Co0.05O3(SSC-LSGMC5)复合阴极的氧还原反应动力学.在SSC-LSGMC5阴极氧还原反应的阻抗谱中可以观察到明显的两个半圆.高频环的电导与氧分压无关,低频环的电导正比于氧分压的0.5次方.并且低频环的氧分压级数随着反应温度的降低而减小,可能对应于吸附氧原子的扩散过程. SSC-LSGMC5极化曲线与经典的Butler-Volmer方程吻合.阴、阳极的电荷转移系数均为1左右,交换电流密度的氧分压级数为1/4,对应于电荷转移过程. 实验结果显示SSC-LSGMC5上的氧还原反应机制随反应条件的不同而发生变化.     

溶胶-凝胶法制备La0.8Sr0.2CoO3纳米材料

以La(NO3)3·6H2O, Sr(NO3)2, Co(NO3)2·6H2O为原料, 用EDTA作为胶溶剂, 采用溶胶-凝胶法制备La0.8Sr0.2CoO3纳米粉体. 利用TG-DTA, FT-IR, XRD, TEM等技术手段对凝胶制备过程、热分解机制、粉体形貌进行了研究, 并探讨了最佳的煅烧温度. 研究结果表明, 溶胶-凝胶法可以制得均一钙钛矿结构的La0.8Sr0.2CoO3氧化物, 最佳热处理温度为700 ℃, 粒径约为20 nm.     

低浓度甲烷甲醇深度氧化Ag/La0.6Sr0.4MnO3催化剂

Ag-modified La0.6Sr0.4MnO3 catalysts were prepared and their catalytic performance for deep oxidation of CH4 and CH3OH at low concentrations were investigated. The results showed that the La0.6Sr0.4MnO3 host catalyst with the perovskite-type nano-crystallite structure displayed considerably high catalytic activity for deep oxidation of CH4 and CH3OH at low concentrations. Ag modification to the La0.6Sr0.4MnO3 host catalyst resulted in significant enhancement of the catalyst activity, making the T95 (the reaction temperature needed for conversion of 95%of CH4 or CH3OH) lowered down to 735K (for CH4) and 421K (for CH3OH) from 813 and 465 K over the Ag-free system under the reaction conditions:0.1MPa,CH4/O2/N2=2/12/86(molar ratio),GHSV=45000 h-1 and CH3OH/O2/N2= 0.2/1.0/98.8 (molar ratio),GHSV=58000 h-1,respectively.The carbon containing product was almost CO2 and the contents of HCHO and CO in the reaction exit gas were both under GC detectable limit in both cases.
The results of spectroscopic characterization indicated that modification by proper amount of Ag-dopant did not change the perovskite structure of the La0.6Sr0.4MnO3 host catalyst as a whole. Interaction of Ag-dopant with the surface of the host catalyst,La0.6Sr0.4MnO3,was in favor of high dispersion of the Ag component at the catalyst surface and led to the oxidation of part of the Mn3+species to Mn4+,resulting in an increase of amounts of the reducible Mnn+ species and a decrease of their reduction temperature. On the other hand, this interaction led also to enhancement of adsorption ability of the catalyst toward O2 at relatively low temperature. High activity of the Ag modified La0.6Sr0.4MnO3 catalyst for CH4 and CH3OH complete oxidation was closely related to high redox-activity of the catalyst and its prominent adsorption-activation ability to O2 at relatively low temperatures.     

含Sr纳米晶粒二氧化钛多孔微球的制备与表征

半导体光催化剂引发的光化学反应被广泛地应用到有毒有机污染物的深度处理、 光有机合成、 能量的转化与存储等研究领域[1~5]. 其中, 利用半导体二氧化钛光催化降解有机污染物受到了广泛的关注. 近年来, 通过掺杂和负载重金属-[6]和金属氧化物[7]等方法来改性二氧化钛, 虽然在一定程度上提高了其光催化活性, 但是没有彻底解决催化剂回收和重复使用的问题.本文通过溶液浸渍和高温处理的方法合成了含Sr纳米晶粒二氧化钛多孔微球, 在保证了二氧化钛微球粒径较大、 易于回收和重复使用等优点的同时, 使其降解活性艳蓝的活性提高了2倍, 具有较为广阔的应用前景.     

90Sr、137Cs在水泥固化体中的浸出研究

本文分别采用90Sr、137Cs为指示剂,均匀混入富铝碱矿渣水泥和525#水泥中制成圆柱形废物固化体。于25℃、40℃、70℃三种恒温条件下,以现场水为浸出剂(按照GB7023-86)进行长期浸出实验,考察了温度和时间对浸出率的影响。结果表明:同样条件下锶、铯在碱矿渣水泥中的浸出率比在525#水泥中低1~2个数量级;温度对浸出率的影响较大,70℃时明显高于室温下的浸出率。碱矿渣水泥在阻止90Sr、137Cs浸出性能方面明显高于目前采用的525#水泥,将是一种有广泛应用前景的新型放射性废物固化材料。     

结构调制对Bi2Sr2CuO6电子结构的影响

在铋基超导体中,Bi-O,Sr-O和CuO_2层的结构畸变导致了原子偏离理想位置,形成更有利的成键环境。这种原子几何位置的改变在计算其电性质时必须予以考虑。但至今对其进行的电子结构计算都是基于Bi-O层具有理想NaCl型结构。考虑畸变在内的详细电子结构计算有助于了解调制的起因以及这些材料复杂的物理化学特征。因此本文对Bi_2Sr_2CuO_6进行了紧束缚带计算,探讨了结构调制对电子态和化学键性质的影响。     

La0.8Sr0.2MnO3水基料浆稳定性的研究

通过调节pH值和添加分散剂的量来研究La0.8Sr0.2MnO3水基料浆的悬浮性和稳定性.结果表明, pH在碱性条件下(pH>8),分散剂添加量为0.2% 时,锰酸镧水基料浆具有良好的稳定性.     

锶稳定同位素比质谱在进口大麦原产地溯源中的应用研究

利用热电离质谱检测了进口自加拿大、法国、澳大利亚和美国的大麦样本的⁸⁷Sr/⁸⁶Sr同位素比值。研究了TIMS测定进口大麦⁸⁷Sr/⁸⁶Sr同位素比值的精密度，利用SPSS 25.0对不同进口国大麦样本的⁸⁷Sr/⁸⁶Sr同位素比值进行了正态性验证、置信区间分析、方差分析和事后多重比较。结果表明：TIMS技术测定进口大麦⁸⁷Sr/⁸⁶Sr同位素比值日内精密度和日间精密度分别达到0.003 59%和0.010 20%;不同进口国的大麦样本⁸⁷Sr/⁸⁶Sr同位素比值成正态分布，置信区间分析、方差分析以及事后多重比较都显示不同进口国大麦⁸⁷Sr/⁸⁶Sr同位素比值间具有显著性差异，可以利用TIMS测定大麦中的⁸⁷Sr/⁸⁶Sr同位素比值并进行进口国溯源。     

负载型La0.8Sr0.2MnO3燃烧催化剂的载体效应

Combustion catalysts La0.8Sr0.2MnO3 supported on γ-Al2O3, α-Al2O3, cordierite (2MgO•2Al2O3•5SiO2) and ZrO2 were compared. Further investigation was focused on LSM/ γ-Al2O3 catalyst. It was observed that LSM/γ－Al2O3 catalyst loaded with 20% (mass fraction) LSM (La0.8Sr0.2MnO3 or corresponding oxides), heated at 750℃ or above, perovskite-type oxides were found by XRD examination, whereas, the same catalyst loaded with 10% or less LSM, perovskite oxides were absent, calcination temperature about 750℃ is necessary for the formation of perovskite structure in LSM/γ-Al2O3 catalysts. High activity of complete oxidation of xylen will be obtained when perovskite-type oxides.
Investigation of TPR showed that neat LSM or LSM/γ-Al2O3(20%) was reduced by H2-N2 mixed gas. Two degradation processes took place. In the first, reduced temperature peak was about 350 - 450℃. If reduction ended at 400℃, perovskite structure was retained, which may be due to the reduction of Mn3+to Mn2+ on the surface of LSM only. In the second process, perovskite structure was destroied, and La2O3, Mn2O3, Mn - Sr - O oxides could be obtained, which took place in the temperature range 685 - 750℃ and ended at 800℃. This was proved by TPR experiments (Fig. 3, 5) and XRD patterns (Fig. 4)
Catalysts LSM/γ-Al2O3(10% or 20%) heated at 500℃ have only one TPR peak, i. e. lower temperature peak. This is due to the absence of perovskite-type oxides in the catalysts. However, neat LSM or LSM/γ-Al2O3(20%) heated 750℃ or above, not only the first low temperature TPR peak but also the second peak, which is contributed by the perovskite-type oxides in these catalysts appeared. Therefore, the second TPR peak, i. e. the higher temperatue peak is a characteristic peak for perovskite-type oxides in the reduced process. When LSM/ γ-Al2O3 (10%) catalys is heated at 750℃, no perovskite-type oxides were detected by XRD, and the second reduction peak was absent also in TPR process. \
The order of the second reduction peak temperature(characteristic peak of perovskite - type ox- ides) is: neat LSM(750℃）> LSM/γ-Al2O3 20% (685-698℃) -deposited LSM/γ-Al2O3 (698℃) > LSM/γ-Al2O3 15% (677 - 680℃) >(LSM/γ-AL2O3 10% 620 - 630℃, for Mn - Al - O medium oxides on surface). It is correleted with the increasing of the effect of support sequentially.
When LSM/γ-Al2O3 catalysts were heated at 900℃, more stable phase, spinel MnAl2O4 appeared, which could be proved by TPR of model catalyst MnAl2O4/γ-Al2O3.