聚多联苯2,6-二甲酰对苯二胺的力学性能模拟

设计了一类线型聚多联苯2,6-二甲酰对苯二胺聚合物, 并对聚合物分子模型进行了计算机模拟, 通过分子力学和力学性质模块的计算得到了聚多联苯2,6-二甲酰对苯二胺的一些力学参数. 模拟结果表明, 聚多联苯2,6-二甲酰对苯二胺类型芳酰胺聚合物通过自组装可以呈现类倒插蜂窝结构排列, 除聚二联苯2,6-二甲酰对苯二胺和聚三联苯2,6-二甲酰对苯二胺以外, 该系列聚合物在xy平面内均具有负泊松比.     

与蛋白质调控DNA空穴迁移相关的具有负离解能特征的亚稳态氢键

利用密度泛函理论方法研究了作为空穴迁移载体的蛋白质复合的DNA三聚体(Protonated arginine…guanine…cytosine, ArgH⁺-GC)的氢键性质. 结果表明, 空穴迁移通过该载体单元时此类氢键表现为亚稳态, 且具有明显的负离解能. 正常情况下ArgH⁺基团在大小沟均能与GC碱对形成氢键, 且具有正的离解能. 然而, 当空穴转移至此将削弱氢键至亚稳态, 使之具有一定的离解势垒和负的离解能. 这种势垒抑制的负离解能现象意味着由于空穴俘获导致此三聚体结构单元在它的ArgH⁺…N7/O6键区储存了一定的能量(约108.78 kJ/mol). 该氢键离解通道受控于此键区两个相关组分之间的静电排斥和氢键吸引之间的平衡以及这两个相反作用随氢键距离不同的衰减速率. 基于电子密度分布的拓扑性质以及键临界点的Laplacian数值分析澄清了此类特殊的能量现象主要源自通过高能氢键(ArgH⁺…N7/O6)连接的授受体间的静电排斥. 进一步空穴俘获诱导的G→C质子转移可扩展负离解能区至ArgH⁺…N7/O6和Watson-Crick(WC) 氢键区. 另外, ArgH⁺ 结合到GC的大小沟增加其电离势, 因此削弱其空穴传导能力, 削弱程度取决于ArgH⁺与GC的距离. 推而广之, 在protonated lysine-GC和protonated histidine-GC体系也可观察到类似的现象. 显然, 此类性质可调的亚稳态氢键可调控DNA空穴迁移机理. 此工作为理解蛋白质调控的DNA空穴迁移机理提供了重要的能量学信息.     

稠密k-子图问题的双非负松弛

稠密k-子图问题是组合优化里面一类经典的优化问题,其在通常情况下是非凸且NP-难的。本文给出了求解该问题的一个新凸松弛方法-双非负松弛方法,并建立了问题的相应双非负松弛模型,而且证明了其在一定的条件下等价于一个新的半定松弛模型。最后,我们使用一些随机例子对这些模型进行了数值测试,测试的结果表明双非负松弛的计算效果要优于等价的半定松弛。     

二维铁电材料ABP2X6内在极高的负泊松比

Recently, ferroelectric materials have attracted considerable research attention. In particular, two dimensional (2D) ferroelectric materials have been considered as most crucial for next-generation circuit designs because of their application as novel electric memory devices. However, a 2D ferroelectric material is very rare. The ferroelectric materials with the form ABP₂X₆ (A = Ag, Cu; B = Bi, In; X = S, Se) are of interest because of their ferroelectric property maintained in their ultrathin structures. Within the ABP₂X₆ monolayer, the P―P bonds form the pillars that hold the top and bottom X planes, while the off-center A―B atoms between the X layers induce a spontaneous ferroelectric polarization. If the two off-center A―B sites are equally aligned, this would lead to the appearance of the paraelectric state. Such intriguing structures must impart novel mechanical properties to the materials. Until now, there has been no report on the mechanical properties of monolayer ABP₂X₆. Based on first-principles calculations, we studied the structural, electronic, mechanical as well as the electromechanical coupling properties of monolayer ABP₂X₆ (A = Ag, Cu; B = Bi, In; X = S, Se). We found that they are all semiconductors with wide bandgaps of 2.73, 2.17, 3.00, and 2.31 eV for CuInP₂Se₆, CuBiP₂Se₆, AgBiP₂S₆, and AgBiP₂Se₆, respectively, which are calculated based on the Heyd-Scuseria-Ernzerhof (HSE) exchange correlation functional model. The conduction band minimum is mainly from p orbitals of X and B atoms, whereas the valence band maximum is due to the hybridization of the p orbital of X atoms and the d orbital of A atoms. Moreover, there are three short and three long A/B―X bonds due to the A―B off-center displacement. Together with the d-p orbital hybridization, the main reason for the distorted ferroelectric structure in ABP₂X₆ monolayers is the Jahn-Teller effect. ABP₂X₆ monolayers are predicted to be a new class of auxetic materials with an out-of-plane negative Poisson's ratio, i.e., the values of the negative Poisson's ratio are in the order AgBiP₂S₆ (−0.805) < AgBiP₂Se₆ (−0.778) < CuBiP₂Se₆ (−0.670) < CuInP₂S₆ (−0.060). This is mainly due to the tensile strain applied in the x/y direction enlarging the angle between P―P bonds and top layer X atoms, thereby enhancing the bucking height of monolayer ABP₂X₆. Moreover, external strain has a significant impact on the A―B off-center displacement, rendering an out-of-plane piezoelectric polarization. The values of e₁₃ for CuInP₂S₆, CuBiP₂Se₆, AgBiP₂S₆, AgBiP₂Se₆ monolayers are calculated to be −3.95 × 10⁻¹², −5.68 × 10⁻¹², −3.94 × 10⁻¹², −2.71 × 10⁻¹² C∙m⁻¹, respectively, which are comparable to the only experimentally confirmed 2D out-of-plane piezoelectric Janus system (piezoelectric coefficient = −3.8 × 10⁻¹² C∙m⁻¹). This unusual auxetic behavior, ferroelectric polarization, and the electromechanical coupling in monolayer ABP₂X₆ could potentially lead to enormous technologically important applications in nanoelectronics, nanomechanics, and piezoelectrics.     

浅海负跃层条件下的warping变换宽带无源测距方法

夏季浅海波导中常常存在强烈的负跃层,研究warping变换无源测距在这种水文条件下的使用方法具有重要的应用价值。对于上发上收、上发下收和跃层强度较小时下发下收的情况,海面海底反射类简正波对声场起主要作用,可以对接收信号的自相关函数进行时域warping变换,利用特征频率匹配的方法进行无源测距。而对于跃层强度较大时下发下收的情况,水体折射-海底反射类简正波对声场起主要贡献,可以对接收信号的自相关函数进行频域β-warping变换进行无源测距。并且能在事先获得粗略的水体声速剖面参数的情况下,通过设置一个已知距离的引导声源,那么即使估计得到的波导不变量存在一定误差,实际测距结果也可以与真实距离符合得较好。利用warping变换对一次夏季浅海实验接收到的目标发出的宽带信号进行无源测距,估计距离与真实距离符合较好,相对误差在20%以内。      

双光子J-C模型实现非定域双原子系统量子特性的远程控制

考虑一对纠缠的二能级原子之一与单模腔场发生双光子共振相互作用,经腔QED演化后,对腔场进行光子探测,通过操纵相互作用的时间和光场参数以及初态两纠缠原子的纠缠度,可远程调控腔外原子表现出更强的非经典效应,如原子的偶极压缩;同时使用相同的方法对远程控制的信道-原子间的纠缠演化也进行了控制,从而更有效地实现对原子量子特性的控制.并且发现原子的压缩和原子间的纠缠存在一定的对应关系.     

电场极性对池沸腾换热影响的实验研究

利用EHD技术对工质R123进行了非均匀高压电场下电场极性对池沸腾换热影响的实验研究.结果表明,无论加正、负电压,强化系数均随热流密度的增加而下降,最终达到稳定值;高热流密度下,正电压有较弱的强化效果,负电压对沸腾换热具有削弱作用;正电压下的强化换热效果优于负电压下的强化换热效果.     

15—20mA负氢离子源的设计与加工

离子源是强流质子回旋加速器的核心设备之一, 它的性能指标对最终束流大小和质量都有重大影响. 文章介绍了一种运用于强流质子回旋加速器上的多峰场负氢离子源的设计与加工情况, 该离子源主要是通过深入研究高密度等离子体产生技术、长寿命大直流灯丝电子发射技术、磁约束技术、虚拟过虑技术、残留气体与电子剥离的控制技术, 以及离子引出技术等, 在中国原子能科学研究院原有10mA离子源基础上建立负氢离子源, 实验研究低能、强流束的实验匹配与调试技术, 将平均引出束流提高到15—20mA.     

固相萃取净化-气相色谱-负化学源质谱法测定近岸海洋环境中的甲氧基多溴联苯醚

甲氧基多溴联苯醚（methoxypolybrominated diphenyl ethers, MeO-PBDEs）广泛存在于生物体和海洋环境。以象山海域的生物体和沉积物为样本,采用固相萃取净化-气相色谱-负化学源质谱法,检测了6种MeO-PBDEs,结果显示,当目标分析物浓度为0.1~20.0 μg?L^-1时,线性关系良好（R²>0.999）,检出限为0.13~0.22 μg?kg^-1,定量限为0.42~0.72 μg?kg^-1,实际样品的平均回收率为71.2%~116.2%。MeO-PBDEs的分布状况调查结果显示,藻类样品中仅检出6-MeO-BDE-47,且浓度较低,其他生物体中检出3种MeO-PBDEs,检出率为31.3%,浓度为0.21~2.72 μg?kg^-1。沉积物中无MeO-PBDEs被检出。