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1.
A fully-coupled model for a piezoelectric hetero-junction subjected to a pair of stresses is proposed by discarding the depletion layer approximation. The effect of mechanical loadings on PN junction performance is discussed in detail. Numerical examples are carried out for a p-Si/ZnO-n hetero-junction under a pair of stresses acting on the ntype ZnO portion near the PN interface, where ZnO has the piezoelectric property while Si is not. It is found that the bottom of conduction band is lowered/raised near the two loading points due to the decrease/increase in the electron potential energy there induced by a tensile-stress mode via sucking in majority-carriers from two outside regions, which implies appearance of a potential barrier and a potential well near two loading points. Furthermore, the barrier height and well depth gradually become large with increasing tensile stress such that more and more electrons/holes are inhaled in loading region from the n-/p-zone, respectively. Conversely, rising/dropping of conduction band bottom is brought out near the two loading points by a compressive-stress mode due to the increase/decrease in the potential energy of electrons by pumping out the majority-carriers from the loading region to the two outside regions. Therefore, a potential well and a potential barrier are induced near the two loading points, such that more and more electrons/holes are driven away from the loading region to the n-zone/p-zone, respectively, with the increasing compressive stress. These effects are important to tune the carrier recombination rate near the PN interface. Thus, the present study possesses great referential significance to piezotronic devices.  相似文献   
2.
In the present work, we systematically study the α-decay half-lives of uranium (Z=92) isotopes based on the Gamow model with a screened electrostatic barrier. There are only two adjustable parameters in our model i.e. the parameter g and the screening parameter t in the Hulthen potential for considering the screened electrostatic effect of the Coulomb potential. The calculated results are in good agreement with experimental data, and the corresponding root-mean-square (rms) deviations of uranium isotopes with α transition orbital angular momentum l=0 and l=2 are 0.141 and 0.340, respectively. Moreover, we extend this model to predict α-decay half-lives of uranium isotopes whose α decay is energetically allowed or observed but not yet quantified in NUBASE2020. For comparison, the modified Hatsukawa formula (XLZ), the unified Royer formula (DZR), the universal decay law (UDL) and the Viola–Seaborg–Sobiczewski formula (VSS) are also used. The predictions are basically consistent with each other. Meanwhile, the results also indicate that N=126 shell closure is still robust at Z=92 and the spectroscopic factor \begin{document}$ S_{\alpha} $\end{document} is almost the same for uranium isotopes with the same l.  相似文献   
3.
对未燃烧的可燃混合气体进行DBD放电,放电后会产生大量的活性粒子,这些活性粒子可以辅助气体燃烧,达到提高燃料燃烧利用率等目的。以DBD激励氩气、甲烷、空气产生的自由基(CH基和OH基)等强化燃烧的关键活性粒子为探索对象,研究DBD放电激励甲烷对滑动弧火焰的影响。为此,采用自主设计的DBD-滑动弧双模式等离子体激励器,利用同轴介质阻挡放电结构对氩气、甲烷、空气混合气进行放电激励,将激励后的氩气、甲烷、空气混合气通入滑动弧端进行点火。固定氩气流量不变,调整空气流量为4.76 L·min-1,并加入甲烷0.5 L·min-1,保证进气通道内氩气与空气-甲烷的气体体积流量比达到Ar∶(CH4+Air)=1∶30,其中空气、甲烷这两种气体达到了化学燃烧当量比φ=1,氩气、甲烷、甲烷混合气体能实现均匀而稳定的放电并燃烧。DBD段放电电压在15~20 kV范围变化,放电频率在6~10 kHz范围变化,滑动弧段的电压和频率分别保持4 kV与10 kHz恒定,通过改变DBD段放电电压和放电频率,用高速光纤光谱仪检测滑动弧火焰中自由基种类及其光谱强度,分析放电参数激励甲烷对火焰中自由基(CH基和OH基)的影响。结果表明,DBD段放电电压及放电频率的增加可以促进火焰内部的偶联反应发生,可有效提升甲烷滑动弧火焰内部的活性粒子含量,其中OH基团、CH基团在燃烧链式化学反应进程中发挥着较为重要的作用。甲烷经过DBD激励后,随放电电压和频率的增加,火焰中OH基、CH基等主要活性粒子都随之增加。DBD放电后,活性粒子的光谱强度增大,特征谱线比单模式更加明显;甲烷经过DBD激励后,火焰组成发生了变化,滑动弧段出口处甲烷燃烧反应更加充分,火焰温度越高越容易产生OH基。与单模式滑动弧相比,双模式放电可有效促进火焰内部的链式化学反应进程,促进燃料燃烧。  相似文献   
4.
多跨锯齿屋面因其具有跨度大、结构轻盈的特点成为典型的风灾易损结构。目前国内规范对锯齿屋盖的风荷载规定较为粗略,简单给定了统一的风压系数参考值,在实际工程应用中具有一定的局限性。本文以某4跨锯齿房屋为研究对象,通过风洞试验测试了15°、21°、26°、30°和40°等5种不同屋面坡度对锯齿屋盖风压特性的影响。试验结果表明,我国建筑结构荷载规范GB 50009-2012关于锯齿屋面的负风压系数绝对值明显偏小,锯齿屋面最不利均面积负风压系数随着坡度的增加逐渐从高屋角(HC)区转移到屋面边区(SE),且与HC区相反,SE区内的最不利负风压系数绝对值随角度增加而增大;锯齿中间B、C跨最不利均面积负风压系数始终出现在HE区,其绝对值随角度增加而增大,而尾跨D则出现在SE区,且随角度增加而减小;屋面最不利极值负风压系数为-9.6,随着屋面坡度的增大,屋面的最大极值负风压系数绝对值逐渐减小。此外,以各坡度屋面负风压系数的分布为依据,给出了不同屋面坡度范围和不同跨屋面风压系数分区划分建议。  相似文献   
5.
We propose a novel device structure with a WO3/NiOx bilayer to improve the hole injection ability in QLEDs fabricated mainly by a solution-based process. First, we employed a spin-coated NiOx thin film as a hole injection layer (HIL) to replace Poly(3,4-ethylenedioxythiophene) poly(styrenesulfonate) PEDOT:PSS which corrodes indium tin oxide (ITO) used as an anode in QLEDs. We showed a simply optimized annealing process, instead of a rather complicated process like doping, can improve the electrical conductivity of the NiOx thin film. The reason for the dependency of conductivity on the post-metallization annealing is because of the change of the total amount of Ni vacancy in the NiOx thin film as a function of annealing temperature: The electrical conductivity of the NiOx thin film annealed at 275 °C was the best in this work. Second, we inserted the WO3 thin film in between ITO electrode and NiOx HIL to form an ITO/WO3/NiOx structure which reduces the hole injection barrier to 0.35 eV, resulting in the excellent characteristic in view of charge balance. Finally, we measured the properties of QLEDs with the WO3/NiOx bilayer to check the effects of the proposed device structure and showed the substantial improvement of the electrical conductivity of NiOx, the luminance, and the current efficiency of the QLEDs.  相似文献   
6.
The dielectric barrier discharge of helium in a 6 mm gap at atmospheric pressure was studied. In this paper, the influence of electric field distribution on the uniformity of DBD is analyzed theoretically and verified by experiments. The experimental results show that the mesh electrode produces a local enhancement effect by affecting the electric field and then produces corona discharge, which provides seed electrons for the subsequent discharge process. The effects of mesh diameter and size on discharge uniformity and stability are analyzed, the electrode structure parameters are optimized, the method of a segmented electrode is proposed, and the discharge process and charge distribution are studied. The electrical diagnosis results of plasma technology show that the segmented mesh electrode reduces the breakdown voltage of DBD and increases the charge deposition.  相似文献   
7.
采用发射光谱、紫外可见吸收光谱、红外吸收光谱和核磁共振技术分析1-丁基-3-甲基咪唑硫酸氢盐([Bmim]HSO4), 1-丁基吡啶硫酸氢盐(HSO4)和1-丁基-3-甲基咪唑四氟化硼([Bmim]BF4)三种离子液体在大气压介质阻挡放电氩等离子体体系中的稳定性,并分别以上述三种离子液体为辅助液采用大气压介质阻挡放电等离子体技术制备TiO2,进一步研究三种离子液体在等离子体中的稳定性对所制备的TiO2晶相结构的影响。结果表明:向大气压介质阻挡放电氩等离子体中分别引入[Bmim]HSO4,HSO4和[Bmim]BF4离子液体后并未改变氩等离子体放电光谱谱峰的位置和数量且没有新的谱峰生成,但谱峰强度都明显降低,说明上述三种离子液体没有在等离子体区蒸发形成激发态物种;[Bmim]HSO4和HSO4放电前后的红外吸收光谱基本一致,表明离子液体在放电后的化学键未发生改变;[Bmim]HSO4和HSO4的紫外可见吸收光谱显示其吸收峰的位置和强度未发生改变,说明两种离子液体在等离子体作用后的结构是稳定的;[Bmim]BF4放电前后的红外吸收光谱各个特征峰并无明显差异,但其紫外可见吸收光谱图谱吸收峰的位置却发生较大的偏移,进一步对放电前后的[Bmim]BF4离子液体进行核磁共振分析,两者的1H NMR峰数相同,但放电后的离子液体化学位移向高位偏移大约0.2单位,说明其化学环境发生了变化,表明有部分[Bmim]BF4结构发生改变。光谱和核磁共振技术分析表明离子液体[Bmim]BF4在等离子体作用后结构发生了改变。采用三种离子液体辅助大气压介质阻挡放电等离子体技术制备TiO2样品的X-射线衍射分析结果表明 [Bmim]HSO4和HSO4辅助制备的HSO4-TiO2和[Bmim]HSO4-TiO2,谱图与锐钛矿相TiO2标准谱图基本一致,表明所制备的TiO2为纯锐钛矿型。而[Bmim]BF4辅助制备的[Bmim]BF4-TiO2在2θ=24.1°处的衍射峰向小角度偏移,2θ=48°处的衍射峰向大角度偏移,说明[Bmim]BF4在辅助制备TiO2过程中,F进入TiO2的晶格,破坏了TiO2原子间的平衡状态,生成了F掺杂TiO2光催化材料。F掺杂TiO2光催化材料的形成也间接证明了离子液体[Bmim]BF4在大气压等离子体中的不稳定性,此结果与核磁共振及紫外可见光的检测结果相一致。同时说明离子液体在等离子体的作用下对于纯锐钛矿晶格的形成和促进高活性掺杂型的光催化材料具有重要作用。为等离子体辅助离子液体制备高性能纳米材料提供重要的实验和理论依据。  相似文献   
8.
Reaction of the Schiff base ligand H2L and dysprosium acetate result in a new planar Dy6 cluster [Dy63‐OH)L6(Ac)6] · MeOH ( 1 ) [H2L = N'‐(2‐hydroxybenzylidene)‐2‐(hydroxyimino)propanohydrazide, HAc = acetic acid], which was successfully structurally and magnetically characterized. Single‐crystal X‐ray diffraction analysis revealed that 1 contained a hexanuclear dysprosium cluster [Dy6], which is composed of four Dy3 triangular units. Magnetic measurements suggest that 1 displays single‐molecule magnet (SMM) behavior which is enhanced by applying a 4000 Oe direct‐current field. The effective anisotropic barrier Ueff/kB = 14.9 K and the pre‐exponential factor τ0 = 1.31 × 10–6 s are also obtained. This work may provide more insights for the design and investigation of lanthanide‐based SMMs.  相似文献   
9.
Fission properties of the actinide nuclei are deduced from theoretical analysis. We investigate potential energy surfaces and fission barriers and predict the fission fragment mass yields of actinide isotopes. The results are compared with experimental data where available. The calculations were performed in the macroscopic-microscopic approximation with the Lublin-Strasbourg Drop (LSD) for the macroscopic part, and the microscopic energy corrections were evaluated in the Yukawa-folded potential. The Fourier nuclear shape parametrization is used to describe the nuclear shape, including the non-axial degree of freedom. The fission fragment mass yields of the nuclei considered are evaluated within a 3D collective model using the Born-Oppenheimer approximation.  相似文献   
10.
K-ion batteries (KIBs) attract considerable attention due to the abundance of K, high-working voltages, and chemical similarity with Li, enabling the utilization of mature Li-ion technology. However, shortage of high-performance anode materials is a critical obstacle for the development of KIBs. Through first-principles swarm-intelligence structural search, we identify a potential anode material, the C6S monolayer, which provides not only a remarkably high specific capacity of 1546 mAh/g but also a low diffusion barrier of 0.11 eV and a low open-circuit voltage of 0.21 V. Inherent metallicity originates from delocalized π electrons.  相似文献   
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