超声动载荷下三维随机骨料混凝土的损伤

混凝土是一种由粗骨料与水泥砂浆组成的非均质复合材料。本研究利用APDL语言程序编写三维水泥混凝土骨料随机投放程序并导入ABAQUS中,同时赋予各相材料塑性损伤本构关系来研究混凝土动态加载下的破坏规律,运用超声波在混凝土破碎中的作用机理对混凝土动态损伤破坏过程进行模拟研究。结果表明:随着超声动态载荷的增大,粗骨料体积分数为40%的混凝土始终能够承受最大应力载荷;随着超声应力波幅值增大,混凝土在动载荷下的损伤值逐渐增大,且粗骨料体积分数为40%时,其抗损伤能力最优;当粗骨料最大粒径逐渐增大,或者当粗骨料最小粒径增大,混凝土级配不合理导致性能不稳定,更易损伤破坏。     

基于6-羟基-2-吡啶基膦酸配体的铜配合物的合成、结构及磁性

在水热条件下, 以6-羟基-2-吡啶基膦酸为主配体, 4, 4'-联吡啶(bpy)及1, 2-二(4-吡啶基)乙烯(bpe)为桥联配体, 合成了2个铜膦酸配位聚合物[Cu₃(L)₂(bpy)₂(H₂O)₂]·2H₂O (1), [Cu₃(L)₂(bpy)₂(H₂O)₃]·2H₂O (2)。配合物1中, Cu²⁺离子由膦酸配体连接成一条链, 该链由bpy桥联成二维层, 层与层之间通过氢键作用构成三维结构。配合物2与配合物1是同构的, 桥联配体是bpe。磁性研究表明, 配合物1与2中铜离子之间存在反铁磁性耦合。     

NiS助催化剂的硫调控光沉积合成及其增强g-C3N4的光催化产氢性能

作为一种非金属聚合半导体,石墨相氮化碳(g-C3N4)具有特殊的能带结构、可见光响应能力以及优良的物理化学性质以及生产成本低等特点,因而已成为目前光催化领域的研究热点.然而,由于g-C3N4被光激发的电子与空穴极易复合,导致g-C3N4材料的光催化性能并不理想.而助剂修饰是实现光生载流子有效分离以提高光催化活性的有效途径.众所周知,贵金属Pt可以作为光催化产氢的反应位点,但高昂的成本限制了它的实际应用.所以,开发高效的非贵金属助剂很有必要.近年来,NiS作为优良的电子助剂在光催化领域受到广泛关注.大量研究表明,NiS可以作为g-C3N4的产氢活性位点用于提高其光催化产氢性能.NiS助剂主要是通过水热、煅烧和液相沉淀的方法修饰在g-C3N4的表面上.相较而言,助剂的光沉积方法具有一些独特的优势,例如节能、环保、简易并且能够实现其原位牢固地沉积在光催化剂的表面.然而g-C3N4光生电子和空穴强还原和氧化能力容易导致像Ni^2+的还原和S^2-的氧化等副反应发生,因此NiS助剂很难光沉积在g-C3N4材料表面.本文采用硫调控的光沉积法成功合成了NiS/g-C3N4光催化材料,该法利用g-C3N4在光照条件下产生的光生电子结合S以及Ni^2+生成NiS,然后原位沉积在g-C3N4表面.由于E0(S/NiS)(0.096 V)比E0(Ni^2+/Ni)(-0.23 V)更正,所以NiS优先原位沉积在g-C3N4表面.因此,硫调控的光沉积法促进了NiS的生成,并抑制了金属Ni等副反应的形成.通过X射线光电子能谱分析NiS/g-C3N4的表面化学态,表明该方法能成功地将NiS修饰在g-C3N4的表面,这也得到透射电镜和高分辨透射电镜结果的证实.光催化产氢的结果表明,NiS/g-C3N4光催化剂实现了良好的光催化性能,其最优产氢速率(244μmol h^?1 g^?1)接近于1 wt%Pt/g-C3N4(316μmol h^?1 g^?1).这是因为硫调控的光沉积法实现NiS助剂在g-C3N4表面的修饰,从而促进光生电子与空穴的有效分离,进而提高光催化制氢效率.此外,在该方法中,NiS的形成通常在g-C3N4光生电子的表面传输位点上,因此也能够使NiS提供更多的活性位点以提高界面产氢催化反应速率.电化学表征结果也进一步证明NiS/g-C3N4光催化剂加快了电子与空穴的分离和转移.更重要的是,这种简易且通用的方法还可以实现CoSx,CuSx,AgSx对g-C3N4的助剂修饰,并且都提高了g-C3N4的光催化产氢性能,表明该方法具有一定的普适性,为高效光催化材料的合成提供了新的思路.     

基于废旧锂电池回收制备LixMO (x=0.79, 0.30, 0.08; M=Ni/Co/Mn)材料作为锂-氧气电池正极催化剂的电化学性能研究

锂-氧气电池因其超高的理论比容量而受到科研界的广泛关注, 但其存在较为严重的充放电极化和较差的循环稳定性等问题, 从而极大地限制其商业化进程. 因此设计出有效的正极催化剂是解决锂-氧气电池面临的这些棘手问题的必要手段. 通过对不同充电状态的废旧锂电池正极进行回收制得三种不同锂含量的多元金属氧化物Li_xMO (x=0.79, 0.30, 0.08; M=Ni/Co/Mn), 并分别用作锂-氧气电池正极催化剂. 系统研究了Li_xMO材料中锂含量及晶体结构对其电化学性能的影响. 电化学测试结果表明, 与Li_0.79MO和Li_0.08MO催化剂相比, 基于Li_0.30MO为正极催化剂的锂-氧气电池在电流密度100 mA•g^–1和限定容量800 mAh•g^–1的条件下具有较高的放电比容量(14655.9 mAh•g^–1)、较低的充电电压(3.83 V)和较高的能量转换效率(72.2%). 而且该电池体系在充放电循环140圈后充电终止电压仍低于4.3 V. 最终认为制得的Li_0.30MO材料具有优异的催化性能归因于其稳定的层状-岩盐相复合结构以及结构中富含的氧化镍相和氧空位之间的协同作用. 这些优点能够促进放电产物的可逆形成与分解, 从而提高锂-氧气电池循环性能.     

Phase Diagram of the Spin-1/2 Heisenberg Alternating Chain in a Magnetic Field *

By using the infinite time-evolving block decimation, we study quantum fidelity and entanglemententropy in the spin-1/2 Heisenberg alternating chain under an external magnetic field .The effects of the magnetic field on the fidelity are investigated, and its relation with the quantum hase transition (QPT) is analyzed. The phase diagram of the model is given accordingly, which supports the Haldane phase, the singlet-dimer phase, the Luttinger liquid phase and the paramagnetic phase. The scaling of entanglement entropy in the gapless Luttinger liquid phase is studied, and the central charge $c=1$ is obtained. We also study the relationship between the quantum coherence, string order parameter and QPTs. Results obtained from these quantum information observations are consistent with the previous reports.     

Heterobimetallic Cluster-Based Coordination Polymers: Assembly,Structures and Third-Order Nonlinear Optical Properties

Reactions of (NH₄)₂WS₄ with CuCN, CuCN/1,2-bis(4-pyridyl)propane (bppa) or [Cu(MeCN)₄]PF₆/bppa under different reaction conditions afforded a set of two- or three-dimensional W/Cu/S cluster-based coordination polymers including {[Et₄N]₂[WS₄Cu₄(μ-CN)₂(μ-I)₂]}_n ( 1 ), [WS₄Cu₄(μ-CN)₂(bppa)₂]_n ( 2 ) and {[WS₄Cu₄(bppa)₄](PF₆)₂}_n ( 3 ), respectively. Compound 2 can be readily formed from reaction of 1 with bppa under solvothermal conditions. Compounds 1 and 2 feature two-dimensional networks with a “sql” topology, while 3 possesses a two-fold interpenetrated three-dimensional net with a rare “reo” topology. Compounds 1 – 3 in DMF exhibited different third-order nonlinear optical responses, and they all showed a reverse saturable absorption while 2 held a strong self-focusing effect.     

Multi-multifractality,dynamic scaling and neighbourhood statistics in weighted planar stochastic lattice

The dynamics of random sequential partitioning of a square into ever smaller mutually exclusive rectangular blocks, which we call weighted planar stochastic lattice (WPSL), is governed by infinitely many conservation laws. Recently, we have shown one of the infinitely many conservation laws can be used as multifractal measure. In this article, we show that except the conservation of total area, each of the infinitely many non-trivial conservation laws is actually a multifractal measure and hence WPSL is a multi-multifractal. We then look at the block size distribution function and find that it exhibits dynamic scaling revealing that the spatial patterns of WPSL of different sizes are statistically self-similar. Besides, we investigate how the mean area ⟨A⟩_k of blocks with k neighbours and the average number of neighbours m_k of a typical cell that neighbours a k-sided block behaves with k. These results suggest that the Lewis law, ⟨A⟩_k∝k, is obeyed for up to k ≈ 8 and the Aboav–Weaire law, km_k∝k, is violated for the entire range of k.     

具有Dzyaloshinskii-Moriya相互作用的XY模型的量子相干性

研究了具有Dzyaloshinskii-Moriya(DM)相互作用的一维横场XY自旋链的量子相变和量子相干性.采用约旦-维格纳变换严格求解了哈密顿量,并描绘了体系的关联函数和相图,相图包含反铁磁相、顺磁相和螺旋相.利用相对熵和Jensen-Shannon熵讨论了XY模型的量子相干性.研究发现,相对熵与Jensen-Shannon熵所表现的行为都可以很好地表征该模型的量子相变.非螺旋相中量子相干性不依赖DM相互作用,而在螺旋相DM相互作用对量子相干性有显著影响.此外,指出了在带有DM相互作用的这一类反射对称破缺体系中关联函数计算的常见问题.     

Piecewise shooting reproducing kernel method for linear singularly perturbed boundary value problems

In this letter, a new numerical method is proposed for solving second order linear singularly perturbed boundary value problems with left layers. Firstly a piecewise reproducing kernel method is proposed for second order linear singularly perturbed initial value problems. By combining the method and the shooting method, an effective numerical method is then proposed for solving second order linear singularly perturbed boundary value problems. Two numerical examples are used to show the effectiveness of the present method.