1) SrTiO-3(STO)
SrTiO3(STO)
2) SrTiO 3
SrTiO3
1.
The rheological properties of SrTiO 3 suspersions and the effect of dispersant concentration on suspension stability are studied by meansof colloidal electrosteric stabilization mechanism.
本文采用胶体“电空间稳定机制”,以PMAA-NH4为分散剂,以沉降高度作为衡量浆料稳定性的参数,研究了SrTiO3粉末的悬浮流变特性及分散剂PMAA-NH4加入量对SrTiO3浆料稳定性的影响。
2.
The Electron Energy Loss Spectrum(EELS)of grain boundary composition of SrTiO 3 doped with Fe 3+ ,Nb 5+ was studied by using a high spatial resolution Scanning Transmission Electron Microscope(STEM).
采用高空间分辨率扫描透射电镜(STEM)对掺杂(Fe3+、Nb5+)SrTiO3晶界进行了观察,并利用采集的电子能量损失谱(EELS)对晶界组成进行了分析。
3.
Homoepitaxial SrTiO 3 thin film was grown by laser molecular beam epitaxy(LMBE) on SrTiO 3(100) single crystal substrates in ultrahigh vacuum(UHV).
在超高真空下利用激光分子束外延 (LMBE)方法基于SrTiO3 (10 0 )单晶基片同质外延SrTiO3 薄膜。
3) SrTiO_3
SrTiO3
1.
In this paper,the molecular dynamics method is adopted to simulate the melting process of SrTiO_3 with the interaction model of PIM.
采用分子动力学方法,势函数为PIM势,模拟了SrTiO3的熔化过程,将熔化的SrTiO3快速冷却到室温以获得非晶态。
2.
A SrTiO_3 single crystal (30mm×60mm) was successfully grown by the flame fusion method using SrTiO_3 powder hydrolyzed controllably from strontium chloride and titanium chloride.
本文以氯化锶和氯化钛为原料,采用控制水解法制备SrTiO3 原料粉末,使用焰熔法生长了SrTiO3 单晶体。
3.
In this paper, the making technology, ceramic composition and structure of a varistor-capacitor double properties chip component based on SrTiO_3 are described.
阐述了SrTiO3片式化压敏-电容双功能元件的制作工艺、陶瓷成分及结构,并讨论了陶瓷成分、结构及烧结工艺对元件压敏、电容性能的影响。
4) CaTiO-3-SrTiO-3
CaTiO3-SrTiO3
5) MgO/SrTiO 3
MgO/SrTiO3
6) SrTiO3-based
SrTiO3基
1.
The SrTiO3-based double function (capacitor-varistor) ceramics materials were prepared by conventional electronic ceramic equipments and productive technology.
鉴于气氛炉设备昂贵,笔者提出用非气氛炉烧结SrTiO3基环形压敏电阻器。
补充资料：STO
分子式：
CAS号：
性质：斯莱特建议的用于量子化学计算的轨道。轨道形式是：φζ,nσ,l,m(rA,θ,φ)=[(2nσ)!]-1/2(2ζ)(nσ+1)/2rAnσ-1e-ζ·rAYlm(θ,φ),nσ是有效量子数，rA，θ，φ是以函数φ的中心A为原点的球极坐标，ζ称为斯莱特轨道指数，它可由经验式ζ=(Z-σ)/nσ。确定，Z为原子序数，σ为屏蔽常数。ζ亦可由从头计算确定。斯莱特型轨道既不是正交的，也没有节点。
CAS号：
性质：斯莱特建议的用于量子化学计算的轨道。轨道形式是：φζ,nσ,l,m(rA,θ,φ)=[(2nσ)!]-1/2(2ζ)(nσ+1)/2rAnσ-1e-ζ·rAYlm(θ,φ),nσ是有效量子数，rA，θ，φ是以函数φ的中心A为原点的球极坐标，ζ称为斯莱特轨道指数，它可由经验式ζ=(Z-σ)/nσ。确定，Z为原子序数，σ为屏蔽常数。ζ亦可由从头计算确定。斯莱特型轨道既不是正交的，也没有节点。
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参考词条