976 resultados para ER-2O-3
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Series of tellurite glasses were prepared by traditional melting method, the glass composition were changed and the different effects of glass modifier oxides(alkali metals and alkaline earth metal oxides) and glass intermediate (Y
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2.0 μm spectroscopic properties of Er3+/Tm3+/Ho3+ triply-doped fluorophosphate glasses pumped by 808 nm and the energy transfer mechanisms between the three rare earth ions were investigated. J-O theory was used to calculate the parameters of Ho3+ in fluorophosphate glasses. Absorption and emission cross-sections and the gain coefficients were calculated. The obtained lifetime r and spontaneous transition probability Ar of Ho3+:5I
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To study the effects of upconversion in Erbium, a set of rate equations that simulates the performance of the passively Q-switched Er:Yb:glass laser with a Co2+:MgAl
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研究了退火和二次离子交换对Er^3+/Yb^3+共掺的磷酸盐玻璃平面光波导传输特性的影响。在退火过程中,由于热效应和波导层Ag^+离子的浓度差使得Ag^+离子重新分布;随着退火时间的延长和温度的升高,光波导模式数目逐渐增加,波导层深度加深,且波导表面折射率与玻璃基质折射率差减小,退火扩散深度与退火时间的平方根成正比。电子探针结果显示在二次离子交换后形成了掩埋式的光波导,Ag^+离子浓度接近二次方分布,而掩埋式的光波导有助于降低光波导的传输损耗。
Substrate-assisted nucleation of ultra-thin dielectric layers on graphene by atomic layer deposition
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We report on a large improvement in the wetting of Al 2O 3 thin films grown by un-seeded atomic layer deposition on monolayer graphene, without creating point defects. This enhanced wetting is achieved by greatly increasing the nucleation density through the use of polar traps induced on the graphene surface by an underlying metallic substrate. The resulting Al 2O 3/graphene stack is then transferred to SiO 2 by standard methods. © 2012 American Institute of Physics.
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A lattice Boltzmann method is used to model gas-solid reactions where the composition of both the gas and solid phase changes with time, while the boundary between phases remains fixed. The flow of the bulk gas phase is treated using a multiple relaxation time MRT D3Q19 model; the dilute reactant is treated as a passive scalar using a single relaxation time BGK D3Q7 model with distinct inter- and intraparticle diffusivities. A first-order reaction is incorporated by modifying the method of Sullivan et al. [13] to include the conversion of a solid reactant. The detailed computational model is able to capture the multiscale physics encountered in reactor systems. Specifically, the model reproduced steady state analytical solutions for the reaction of a porous catalyst sphere (pore scale) and empirical solutions for mass transfer to the surface of a sphere at Re=10 (particle scale). Excellent quantitative agreement between the model and experiments for the transient reduction of a single, porous sphere of Fe 2O 3 to Fe 3O 4 in CO at 1023K and 10 5Pa is demonstrated. Model solutions for the reduction of a packed bed of Fe 2O 3 (reactor scale) at identical conditions approached those of experiments after 25 s, but required prohibitively long processor times. The presented lattice Boltzmann model resolved successfully mass transport at the pore, particle and reactor scales and highlights the relevance of LB methods for modelling convection, diffusion and reaction physics. © 2012 Elsevier Inc.
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研究了H_2和CO在CuO-ZnO_Al_2O_3催化床中转化成H_2O和CO_2的实验装置和实验结果,论证了不同床层工作温度、系统压力、杂质浓度、流量及露点温度等因素对氧化铜床工作性能的影响;测得了H_2和CO在CuO-ZnO-Al_2O_3床上的转化特性曲线等变化规律,获得了转化容量、工作周期和转化效率等实验数据,确定了最佳运行参数。结果表明,使用CuO_ZnO-Al_2O_3床可使净化后的H_2和CO的体积分数都小于2×l0 ̄(-6),满足高温气冷堆的净化要求。为高温气冷堆中氧化铜床装置提供了可靠的设计数据。
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本论文由两大部分组成。第一部分是新型稀土永磁材料Nd-Fe-B氧化过程及抗氧化新体系的研究。Nd-Fe-B永磁体是1983年问世的新型稀土永磁材料。和原有的铁氧体及Sm-Co体系相比,具有磁能积高(50MGOe)。价廉源广,制备简单等三大优点;也有居里温度低(310℃),温度系数大(-0.126%/K),易氧化等三大缺点,我们对Nd-Fe-B合金的氧化过程进行研究,发现该材料热稳定性差,容易发生氧化反应,氧化使材料的结构受到破坏,并给材料的磁性造成不可恢复的损失,整个氧化过程是分阶段的。在室温和干燥的空气中材料基本是稳定的。150℃以下材料磁性受到破坏的主要原因是体系中Nd的氧化。230℃以上材料主体成分Fe也开始氧化,温度升高使反应进程大大加快。到800℃左右反应基本结束,最终产物主要为Fe_2O_3, Nd_2O_3·FeNdO_3和NdBO_3。增加体系中B的相对含量和添加某些新的元素均能提高材料的抗氧化能力,新研制的Nd-Fe-B-Si四元体系和原来的Nd-Fe-B体系相比具有下列显著优点:新体系的抗氧化能力大大提高,经过150℃的长期恒温试验,材料的结构,磁性均未受到破坏,某些体系甚至能在更高的温度下使用,另外,新体系的居里温度Tc也大为提高。比原有Nd-Fe-B磁体高40℃左右。因此该体系是一种大有发展前途的新材料。此外,我们用动态热重法研究了Nd-Fe-B合金的氧化动力学过程,但由于我们新合成的体系构相较为复杂,未能达到预期效果。第二部分是CuO,Y_2Cu_2O_5,BaCuO_2和RBa_2Cu_3O_(7-δ)超导体(R稀土元素)磁化率及铜价态研究,铜的氧化物具有复杂的化学计量关系和磁学性质。在对CuO的磁化率研究中,我们发现在低温区(77K-110K)和一定磁场下,CuO由顺磁突变为抗磁。这种转变与磁场强度有很大关系。这一结果与前人的工作有较大的出入。而与超导体的形为极为相似。所不同的是,转变温度与样品的重量也有关系。实验结果重复。由于铜氧性质在R-Ba-Cu-O超导体中起决定作用,因此有必要对CuO的低温磁性作进一步研究。此外,我们对文献尚未报道的Y_2Cu_2O_5的磁化率在77-300K温度区间进行了测量,发现它是顺磁性物质,室温有效磁矩μ_(eff) = 2.13μB。高于Cu~(2+)的理论有效磁矩(1.73μB)。经过碘量法价态分析,发现Y_2Cu_2O_5中有部分Cu~(3+),这与磁化率的测定相符合。Tc在90K左右的Y-Ba-Cu-O体系是近期才发现的具有超高温超导材料。该体系有着独特的结构和性质。在对R-Ba-Cu-O及R-Ba-Cu-O-Ag超导体的研究中,我们发现此类超导体属II类超导体,在临界温附近该超导体由顺磁转变为抗磁,此种变化与磁场强度有很大关系,当场强大于一定值后,则观察不到这种转变。在对RBa_2Cu_3O_(7-δ) (R = Y, Sm, Eu, Gd, Dy, Ho, Er, Tm)超导体和具有相同配比但由于合成工艺条件不同而不超导的R'Ba_2Cu_3O_(7-δ) (R' = Y, Sm, Eu, Gd)非超导体的铜价态分析中,我们发现此两类化合物中均含有一定量的Cu~(3+)。且超导体中Cu~(3+)的含量高于非超导体中Cu~(3+)的含量(同样比例)。我们还发现Cu~(3+)对水极为敏感,将RBa_2Cu_3O_(7-δ) (除R = Gd, Dy, Er)超导体在未干燥容器中测出的Cu~(3+)量远远低于干燥容器中所测得的值。我们认为这可能是引起超导体不稳定的重要原因。由于尚缺乏用其它手段检测到超导体中Cu~(3+)存在的例证。故对此问题还有待于今后继续作进一步的研究。
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异质外延法是目前制备新型SOI材料的技术途径之一。采用低压化学气相沉积技术(LPCVD)在硅衬底上先外延r-A1-2O-3绝缘单晶薄膜,制备出硅衬底上外延氧化物外延结构r-Al-2O-3/Si(EOS),然后采用类似SOS薄膜生长的常压CVD(APCVD)方法在EOS上外延硅单晶薄膜,形成新型硅基双异质SOl材料Si/r-Al-2O-3/Si。利用反射高能电子衍射(RHEED)、X射线衍射(XRD)、俄歇电子能谱(AES)及MOS电学测量等技术表征分析了Si(100)/r-Al-2O-3(100)/Si(100)SOI异质结构的晶体结构、组分和电学性能。测试结果表明,已成功实现了高质量的新型双异质外延SOI结构材料Si(100)/ r-Al-2O-3(100)/Si(100),r-Al-2O-3与Si外延薄膜均为单晶,r-Al-2O-3薄膜具有良好绝缘性能,SOI结构界面清晰陡峭,该SOI材料可应用于CMOS电路的研制。
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The crystal structure of Er(PM)(3)(TP)(2) [PM = 1-Phenyl-3-methyl-4-isobutyryl-5-pyrazoloiie, TP = triphenyl phosphine oxide] was reported and its photoluminescence properties were studied by UV-vis absorption, excited, and emission spectra. The Judd-ofelt theory was introduced to calculate the radiative transition rate and the radiative decay time of 3.65 ms for the I-4(13/2) -> I-4(15/2) transition of Er3+ ion in this complex.
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in this communication, a novel Er3+ complex Er(PT)(3)TPPO [PT = 1-phenyl-3-methyl-4-tert-butylbenzoyl-5-pyrazolone, TPPO = triphenyl phosphine oxide] is successfully synthesized and characterized by elemental analysis and single-crystal X-ray diffraction. Its optical properties and the energy transfer process from the ligand PT to the Er3+ ion are investigated, the typical near-infrared (NIR) luminescence (centered at around 1530 nm) is attributed to the I-4(13/2) -> I-4(15/2) transition of Er3+ ion which results from the efficient energy transfer from PT to Er3+ ion (an antenna effect). The wider full width at half maximum (78 nm) peaked at 1530 nm in the emission spectrum and the Judd-Ofelt theory calculation on the radiative properties suggest that Er(PT)(3)TPPO should be a promising candidate for tunable lasers and planar optical amplifiers.
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Infrared emission at 1.54 mu m excited optically and electrically from an erbium organic compound tris(acetylacetonato)(1,10-phenanthroline) erbium [Er(acac)(3)(phen)] is observed. The rare-earth complex is dispersed into a polymer matrix of poly(N-vinylcarbazole) (PVK) to fabricate an electroluminescent (EL) device with an ITO/PVK:Er(acac)(3)(phen)/Al:Li/Ag structure, where ITO represents indium-tin-oxide-coated glass. The device shows infrared EL emission at 1.54 mu m, which suggests a simple and cheap method to obtain a light source for 1.54-mu m-wavelength devices in optical communications. (C) 2000 American Institute of Physics. [S0021-8979(00)00301-7].
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以H_2S和CS_2作硫化剂,用TPS和TPDS方法研究了水媒气变换催化剂CoMoK/γ-Al_2O_3的硫化及反硫化过程。用H_2S/H_2硫化时,只发现H_2S的消耗和H_2O的生成,用CS_2/H_2硫化时,首先生成CO_2,然后是CH_4,H_2O和H_2S,TPG实验表明催化剂表面上有积炭,造成催化剂的活性降低。但积炭在水煤气变换反应进行中逐渐除去。TPDS实验表明N_2不起反硫化作用,H_2和CO也没有明显反硫化作用,H_2O对CoMoK/γ-Al_2O_3催化剂有根强的反硫化作用。O_2能使催化剂部分永久性失活。XPS测试表明反硫化的催化剂中低价的Mo ̄(4+)转变成高价的Mo ̄(5+)和Mo ̄(6+),导致其活性下降。
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Fundação de Amparo à Pesquisa do Estado de São Paulo (FAPESP)
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In the present study, the effects of electrolytic lesions of the anteroventral third ventricle (AV3V) region and of the medial forebrain bundle (MFB) on the pressor response induced by bilateral carotid occlusion (BCO) in conscious intact and aortic baroreceptor-denervated (AD) rats were investigated. In intact control rats, BCO during 60 s produced a pressor response that could be divided into an early response (ER = 50 +/- 3 mmHg) that reachs a peak during the first 20 s and a sustained late response (LR), smaller than ER (32 +/- 2 mmHg), observed during the last 30 s. In intact-innervated rats, AV3V lesion (2 days) reduced ER (22 +/- 3 mmHg) and LR (16 +/- 2 mmHg), whereas the bilateral MFB lesions (6 days) mainly reduced LR (9 +/- 1 mmHg). Rats with simultaneous lesion of both the AV3V region and the MFB showed additional reduction of the ER (15 +/- 3 mmHg), but not LR (11 +/- 1 mmHg) when compared to the effect of MFB lesions alone. Compared to the AV3V lesion alone, LR but not ER was reduced in rats with a double lesion. In sham-lesioned rats, AD induced a significant increase in the pressor response to BCO (ER = 75 +/- 4 mmHg and LR = 65 +/- 3 mmHg) when compared to intact controls. A similar reduction in ER and LR was observed in AD rats after AV3V (ER = 35 +/- 3 mmHg and LR = 40 +/- 2 mmHg) and MFB (ER = 49 +/- 6 mmHg and LR = 41 +/- 5 mmHg) lesions alone or combined (ER = 40 +/- 6 mmHg and LR = 35 +/- 7 mmHg). The results showed that simultaneous lesions of both the AV3V region and the MFB practically abolished the pressor response to BCO. They also suggested that aortic baroreceptor activity plays a significant role in the effects of AV3V and MFB lesions on the pressor response to BCO.