Plasmonic Bloch oscillations and resonant Zener tunneling in subwavelength metal-dielectric-air waveguide superlattices

In this paper,we study the propagation properties of surface plasmon polaritons in plasmonic single-cavity superlattices and two-cavity superlattices which are composed of two kinds of alternately stacked subwavelength metal-dielectric-air waveguides with large dispersion.Theoretical predictions of plasmonic time-resolved Bloch oscillations existing in single-cavity superlat-tices and resonant Zener tunneling(ZT) occurring in two-cavity superlattices by the transfer matrix method(TMM) are well dem-onstrated by the numerical simulations on the propagation of SPPs pulse in the two kinds of superlattices by the finite-difference time-domain(FDTD) method.The two proposed superlattices can be conveniently fabricated by present nanotechnology,and the study may promote the realization of plasmonic BO and resonant ZT in nanoscale devices experimentally.     

Meyer-Konig and Zeller算子及Bernstein 算子在内插空间中一致逼近的特征性定理

给出了一般内插空间中线性一致有界算子序列逼近的正逆定理,作为应用,用Meyer-Konig and Zeller算子和Bernstein算子给出了一类特殊的内插空间中一致逼近的特征性定理,其结果为已有的经典Zygmund类中相应结论的推广.     

有机共轭聚合物材料中的齐纳隧穿

基于扩展的SSH模型,采用非绝热动力学方法,研究高电场下一维有机共轭聚合物的电性质.发现在足够高的电场下,价带中的电子可以穿过带隙进入导带,即有机聚合物中的齐纳隧穿现象.伴随电子的带间隧穿,带隙消失,发生从绝缘体(半导体)到金属的相变(I-M 相变),晶格结构同时发生重大变化.     

Evolutions of diffusion activation energy and Zener–Hollomon parameter of ultra-high strength Al-Zn-Mg-Cu-Zr alloy during hot compression

The changes of stress level for the ultra-high strength Al-Zn-Mg-Cu-Zr alloy were described by constitutive equation with considering lattice diffusion of aluminum, zinc, magnesium and copper. Zener–Hollomon(Z)parameter expression based on the constitutive equation with considering lattice diffusion was used to reflect the changes of microstructure. The critical stress σcfor the initiation of dynamic recrystallization(DRX) was introduced to calculate the Z parameter. Steady-state dislocation density ρsatand critical dislocation density ρcfor the initiation of DRX decreased with the increase of deformation temperature. The dependence of diffusion activation energy Q on temperature and strain rate was given and the effects of deformation conditions on Q were discussed in detail. Microstructural evolution revealed that low angle boundaries(2–5°) created in the process of dynamic recovery(DRV) could convert into subgrain boundary, thus the original grains were divided into subgrains, and then subgrains transformed into DRX grains by the way of progressive rotation. When the Z value was high(ln Z 30.9), DRV was the main softening mechanism. With the decrease of Z value, both of DRV and DRX played an important roles in softening effect, while with the further decrease of Z value(ln Z 28.6), DRX became the main softening mechanism. Continuous dynamic recrystallization(CDRX) and discontinuous dynamic recrystallization(DDRX) operated together under the condition of lower Z value, but CDRX was confirmed as the dominant DRX mechanism.     

改进的黏弹材料应力松弛模型

为了用较少的参数准确描述粘弹材料的应力松弛实验数据,并且唯象解释松弛速率与应力的幂律关系,用假塑性粘壶与弹簧串联,得到改进的Maxwell模型。改进的Maxwell模型再与弹簧并联,给出改进的Zener模型。取定应变时,可得出松弛速率与应力满足幂律关系。求解本构方程得到它们的应力松弛函数。结果表明,常见的幂律型松弛可视为改进后模型的解,幂律函数的指数与反映材料非线性强弱的参数建立了关系,而Debye型松弛是幂律型松弛的一种极限情况。用给出的松弛函数对聚异丁烯的松弛模量进行了研究,拟合过程简单,准确度较高。     

声波在声子晶体中的Zener共振遂穿效应

应用转移矩阵方法,研究了由两个全同声子晶体构成的可调谐声学谐振腔中声波的共振遂穿效应,其遂穿过程类似于量子力学中的Zener共振遂穿效应.通过改变声波谐振腔的长度,研究了声子晶体的带隙中声波遂穿的动力学过程.结果表明:不同带隙具有不同的遂穿特征,遂穿频率随着谐振腔的增加呈周期性振荡变化的规律.     

服从分数阶Zener模型黏弹性体的力学特性研究

基于黏弹性理论和分数阶导数理论,建立了分数阶Zener模型并给出其本构方程形式,在此基础上推导出服从分数阶Zener模型黏弹性体的松弛函数、蠕变函数及复模量、损耗比等力学性能参数的表达式.通过数值算例,分析了材料的蠕变和松弛行为以及部分力学参数随频率的变化规律.结果表明:服从该模型的黏弹性材料的蠕变和松弛特性,可以通过改变分数阶Zener模型的分数阶数值来控制.在低频时,黏弹性材料的存储模量趋于1,此时材料处于一种橡胶态,其性质接近弹性体.而在高频时,分数微分算子的值越大,耗散率越快趋于稳定;损耗比在低频时加速上升,随着频率增大,在达到最大值后开始有下降趋势.     

TiAl合金高温拉伸流变应力与Zener-Hollomon因子的关系函数

:把温度T和应变速率ε·对Ti-47Al-2Mn-2Nb(TiAlMnNb)和Ti-47Al-2Mn-2Nb-0.8TiB2(TiAlMnNbB)合金在1073～1373K和10-5～10-1s-1条件范围内拉伸应力的影响归结为Zener-Hollomon因子Z=ε·exp(Q/RT)的影响,利用Sellars和Tegart提出的双曲函数,确定两种合金拉伸形变应力峰值σP与Z因子之间的关系函数;得到的σP解析表达式中A、α和n值分别为2.308×108s-1、8.50×10-9Pa-1和2.594(TiAlMnNb),1.423×1010s-1、6.275×10-9Pa-1和2.980(TiAlMnNbB);Z因子中的激活能Q值分别为322.3kJ/mol和351.6kJ/mol,提示两种合金高温拉伸形变受微观原子扩散过程控制     

Fe_(57)Al_(43)合金中的Zener弛豫

考察了Fe57Al43合金的内耗特征。对于空冷和炉冷的样品,在520℃左右观察到一个弛豫型内耗峰,该峰在升降温测量过程中都能出现。根据该内耗峰的激活能,该峰可归因为Zener弛豫,产生于Fe-Al合金中Al原子对的重新取向。     

C194铜合金热压缩变形流变应力

在Gleeble-1500热模拟机上对C194铜合金在应变速率为0.01～10s~(-1)、变形温度为650～850℃条件下的流变应力行为进行了研究.结果表明:在实验范围内,C194铜合金热压缩变形时发生明显的动态再结晶;用Zener-Hollomon参数的指数函数形式能较好的描述C194铜合金高温变形时的流变应力行为;所获得的应变速率ε解析表达式中,参数A和β值分别为6.35×10~9 s~(-1)和0.119 MPa~(-1);其热变形激活能Q为316.11 kJ/mol.