Elasticity and melting of skyrmion flux lattices in p-wave superconductors

We analytically calculate the energy, magnetization curves [B(H)], and elasticity of Skyrmions flux lattices in p-wave superconductors near the lower critical field H(c1), and we use these results with the Lindemann criterion to predict their melting curve. In striking contrast to vortex flux lattices, which always melt at an external field H>H(c1), Skyrmion flux lattices never melt near H(c1). This provides a simple and unambiguous test for the presence of Skyrmions.     

Observation of B-->eta'K* and evidence for B+-->eta'rho+

We present an observation of B-->eta'K*. The data sample corresponds to 232x10(6) BB[over ] pairs collected with the BABAR detector at the PEP-II asymmetric-energy B factory at the Stanford Linear Accelerator Center. We measure the branching fractions (in units of 10(-6)) B(B(0)-->eta'K*0)=3.8+/-1.1+/-0.5 and B(B+-->eta'K*+)=4.9(1.7)(+1.9)+/-0.8, where the first error is statistical and the second systematic. A simultaneous fit results in the observation of B-->eta'K* with B(B-->eta'K*)=4.1(-0.9)(+1.0)+/-0.5. We also search for B-->eta'rho and eta'f(0)(980)(f(0)-->pi+pi-) with results and 90% confidence level upper limits B(B+-->eta'rho+)=8.7(-2.8-1.3)(+3.1+2.3) (<14), B(B(0)-->eta'rho0)<3.7, and B(B(0)-->eta'f(0)(980)(f(0)-->pi+pi-))<1.5. Charge asymmetries in the channels with significant yields are consistent with zero.     

High-power and high-temperature THz quantum-cascade lasers based on lens-coupled metal-metal waveguides

A metal-metal waveguide quantum cascade laser with an abutted silicon hyperhemispherical lens is demonstrated at ~4.1 THz. The device produced 145 mW of peak pulsed power at 5 K with a wall-plug power efficiency of 0.7%, lasing up to a maximum operating temperature of 160 K. The far-field beam pattern has a full width at half-maximum value of ~4.8 degrees in the H plane. The same device produced ~26 mW of peak power using a Winston cone instead of a lens, lasing up to 165 K. The large increase in output power is mainly attributed to an increase in collection efficiency.     

Exact solutions for KdV system equations hierarchy

Exact solutions for KdV system equations hierarchy are obtained by using the inverse scattering transform. Exact solutions of isospectral KdV hierarchy, nonisospectral KdV hierarchies and τ$\tau$-equations related to the KdV spectral problem are obtained by reduction. The interaction of two solitons is investigated.     

ZnII and CdII Metal Organic Frameworks Based on 2-Methyl-6-oxygen-1,6-dihydro-3,4'bipyridine-5-carbonitrile

To investigate the coordination chemistry of modbc (2-methyl-6-oxygen-1,6-dihydro-3,4'-bipyridine-5-carbonitrile) with Zn^II and Cd^II salts under the solvothermal conditions, six new MOFs with the formulas [Zn(modbc)₂(mpa)]_n ( 1 ), [Zn(modbc)(mpa)(H₂O)]_n ( 2 ), [Zn(modbc)(pa)_0.5(H₂O)]_n ( 3 ), [Cd(modbc)(pa)_0.5(H₂O)]_n ( 4 ), [Zn(modbc)₂(tpa)]_n ( 5 ), and [Cd(modbc)₂(pda)(H₂O)]_n ( 6 ) (mpa = m-phthalic acid; pa = pyromellitic acid; tpa = terephthalic acid; pda = pentane diacid) were successfully synthesized by solvothermal reaction and fully characterized by elemental analysis, IR spectroscopy, single crystal, powder X-ray diffraction, thermal and photoluminescence properties. Though MOFs 3 and 4 have the same structure, we have obtained three different kinds of coordination configurations by the X-ray diffration analysis. Compared with 1 and 2 , coordination water has no effect on the solid fluorescence emission of MOFs. It is worth noting that the fluorescence intensity of 3 containing central Zn^II atoms is very strong, whereas that of isomorphism 4 containing central Cd^II atoms has almost no fluorescence emission, showing that metal ions have very important influence on the fluorescence emission. Further, we found that solvents had an important effect on the fluorescence emission in liquid fluorescence of MOFs 1 – 6 .     

Efficient domino strategy for synthesis of 3-substituted 1,5-dihydro-4H-pyrrolo[3,2-c]pyridin-4-one derivatives

A series of 1,5-dihydro-4H-pyrrolo[3,2-c]pyridin-4-one derivatives with 3-(4-hydroxy-2-oxo-2H-pyran-3-yl) groups were synthesized via a one-pot three-component reaction of 4-aminopyridin-2(1H)-ones, 2,2-dihydroxy-1-arylethan-1-ones, and 4-hydroxy-2H-pyran-2-ones in water. This strategy not only provides a valuable tool in the design and synthesis of new hydrogenated pyrrolo[3,2-c]pyridines but also has the advantages of inexpensive starting materials, atom and step economy, environmental friendliness, good to excellent yields, and operational simplicity. A total of 14 examples were examined to show a broad substrate scope and high yields.     

固体核磁共振Multiple-CP定量技术的参数优化与应用研究

固体核磁共振Multiple-CP定量技术可实现对不同体系、 不同定量信息的检测. 然而, Multiple-CP对样品属性的宽容度较低, 其中有关样品属性的核磁共振参数包括氢的自旋晶格弛豫时间(T_1,H)、 交叉弛豫时 间(T_CH)和自旋锁定场下氢的自旋晶格弛豫时间(T_{\mathrm{1}\rho }^{\text{?}\mathrm{H}})等. 因而需要系统地掌握Multiple-CP各种实验参数与样品上述特性参数之间的关系, 从而确定Multiple-CP技术可适用的体系范围以及最优的实验参数范围. 基于此, 首先以L-丙氨酸为模型样品, 探讨在Multiple-CP实验中弛豫恢复时间(t_d)、 交叉极化接触时间(t_p)和交叉极化次数(n) 3种实验参数对分子中基团比例测量结果的影响规律. 并以L-缬氨酸、 L-丙氨酸/L-缬氨酸的混合物为模型样品, 探讨样品特性参数的差异性对Multiple-CP实验参数范围的影响. 实验结果表明, t_p受T_CH和\text{?}{T}_{\mathrm{1}\rho }^{\text{?}\mathrm{H}}的影响较大. 对于纯净物或均相体系, T_CH是影响t_p参数设置的关键. 依据实验数据发现, 当样品中各基团T_CH差异度小于8%时, 实验对t_p的宽容度较高; 对于混合物体系, 需同时考虑混合物中组分\text{?}{T}_{\mathrm{1}\rho }^{\text{?}\mathrm{H}\text{?}}差异度的影响. 当组分\text{?}{T}_{\mathrm{1}\rho }^{\text{?}\mathrm{H}\text{?}}差异度为32%、 各基团T_CH差异度为21%时, Multiple-CP对t_p的宽容度高, 可在较宽的参数范围内实现定量检测. 而当T_CH差异度较大时, 获取定量结果时t_p的参数范围较小, 实验条件较苛刻. Multiple-CP定量方法更适用于T_CH和\text{?}{T}_{\mathrm{1}\rho }^{\text{?}\mathrm{H}\text{?}}差异度较小的样品体系的定量研究. 通过研究样品T_CH和\text{?}{T}_{\mathrm{1}\rho }^{\text{?}\mathrm{H}\text{?}}对实验参数的影响, 总结了Multiple-CP方法所适用的样品体系特征, 为使用Multiple-CP进行定量检测提供可参考的参数设置方案.     

具有光控氧空缺的钼掺杂Bi5O7Br纳米片用于光催化氮气合成氨

氨(NH3)作为合成燃料、化肥和潜在能源载体的重要前体,是现代化学工业中最重要的化学品之一.工业中主要通过高能耗的Haber-Bosch工艺在高温高压下将氮气和氢气转化为NH3,而原料氢气由天然气蒸汽获得,因而不仅消耗大量能源,而且导致温室气体二氧化碳的大量排放,对环境造成危害.光催化固氮以光能为驱动力,以水为质子源,为合成NH3提供了一种温和、绿色和可持续的方法.然而,传统固氮催化剂具有与N2结合弱、成键难以及电子转移效率低的缺点.为了克服上述问题,在催化剂中引入氧空缺和过渡金属作为给电子中心和活性位点的策略被广泛研究.本文以半导体Bi5O7Br纳米片作为研究对象,通过在水热合成过程中添加Na2MoO4前驱盐在Bi5O7Br中掺杂钼元素,合成了不同摩尔含量的钼掺杂Bi5O7Br(Mo-Bi5O7Br)纳米片,并将其应用于光催化N2还原反应,发现Mo-Bi5O7Br的光催化固氮性能显著优于空白Bi5O7Br的催化性能.扫描电镜、透射电镜、能量色散X射线元素映射以及X射线光电子能谱的结果表明,掺杂过程不会影响Bi5O7Br纳米片的晶相和形貌,掺杂后钼元素均匀地分布在Bi5O7Br纳米片晶格中.采用紫外可见漫反射光谱、电子自旋共振光谱、氮气程序升温脱附谱以及光电化学测试等方法研究了Mo-Bi5O7Br相较于空白Bi5O7Br纳米片在光催化N2还原反应中催化性能提升的原因.UV-vis DRS结果表明,钼掺杂对Bi5O7Br可见光吸收能力具有增强作用.以催化NH3产率最高的Mo-Bi5O7Br-1(Mo摩尔百分含量为1％)为研究样本,EPR结果表明,在黑暗条件下,只有Mo-Bi5O7Br-1样品可以检测到明显的表面氧空位(OVs)信号;在光照条件下,Bi5O7Br和Mo-Bi5O7Br-1两种样品都出现OVs的信号峰,但同等光照时间下的Mo-Bi5O7Br-1具有更高的信号强度.此外,OVs信号会随着光照时间的延长逐渐增强;当移除光源后,信号强度逐渐降低.这表明Mo-Bi5O7Br-1在光照下会产生更高浓度的表面光控OVs.N2-TPD结果表明,光控OVs作为活性位点促进催化剂对N2的吸附.关闭光源后,OVs被环境中的水或氧气中的氧原子重新填充,避免了OVs易被氧化而导致反应失活的缺点,有助于保持Mo-Bi5O7Br-1催化N2还原反应的活性和稳定性.光电化学表征结果表明,Mo-Bi5O7Br-1中的光生载流子的分离和迁移效率明显提高.以上结果表明,掺杂过渡金属钼有助于Bi5O7Br纳米片表面光控OVs的生成,光控OVs作为活性位点提升了Bi5O7Br吸附和活化N2的能力,钼掺杂和光控OVs协同提高Bi5O7Br内部光生载流子的分离迁移效率,增强Bi5O7Br光催化固氮合成氨的反应性能.     

Metabolome Analysis of Selective Inactivation of Human Melanoma and Normal Cells by Cold Atmospheric Plasma

Plasma Chemistry and Plasma Processing - Cold atmospheric plasma (CAP) is a novel technology which is widely used in the biomedical field and has developed quickly over the past few years,...     

MIL-53(Al)衍生的Rh单原子催化剂在间氯硝基苯选择性加氢制间氯苯胺反应中的应用

卤代苯胺是化学工业中重要的中间体,主要用于制造药物、聚合物、染料等含氮化学品,用多相金属催化剂催化卤代硝基芳烃加氢制备卤代苯胺是一种高效,绿色和可持续发展的生产工艺.该过程需要选择性加氢硝基基团,同时避免卤素基团的脱卤副反应发生.然而,化学选择性加氢存在巨大的挑战,难点在于催化剂的精准设计,一方面要求具备对硝基基团合适的加氢能力,另一方面要阻止对卤素基团的脱卤副反应发生.基于此,研制高效多相金属催化剂用于卤代硝基芳烃选择性加氢制备卤代苯胺反应引起了高度关注.近年来,单原子金属催化剂受到越来越多的关注,并在卤代硝基芳烃选择性加氢制备卤代苯胺反应中显现出极大的潜力.本文通过在金属有机骨架材料MIL-53(Al)自组装的过程中将金属Rh原位嫁接其骨架结构中,继而通过限域热解的方法制备了Rh@Al2O3@C单原子催化剂,其在间氯硝基苯(m-CNB)加氢制间氯苯胺(m-CAN)反应中显现了高效催化选择性.球差校正高角度环形暗场模式的透射电镜,CO作为探针分子的红外光谱和X射线光电子能谱等结果发现,Rh是以单原子的形式均匀的分布在Al2O3上并被无定型碳包覆,且Rh化学价态呈正价.而27Al固体核磁共振与密度泛函理论计算的结果则进一步确定Al2O3@C载体中存在的五配位的Al物种(AlV)是锚定Rh单原子的主要位点,AlV的不饱和的配位结构可以有效地稳定Rh单原子,对形成Rh位点的单原子分散至关重要.在间氯硝基苯选择性加氢制间氯苯胺反应中,与等体积浸渍法制备的Rh/C和Rh/γ-Al2O3纳米催化剂相比,Rh@Al2O3@C单原子催化剂表现出优异催化性能:其在313 K,氢气压力为20 bar的温和条件下转换频率(TOF)高达2317 molm-CNB·molRh-1·h-1,优于已报道的多相金属催化剂,是目前的最高值.此外,该催化剂展现出极佳的稳定性能,经过五次循环后,该催化剂对m-CAN的选择性仍旧保持在98％左右.Rh@Al2O3@C单原子催化剂的优异催化性能源自于金属单原子结构的形成对于金属位点电子结构的有效调节,进而调控催化剂加氢性能并实现对加氢脱卤副反应的抑制;与此同时,Rh@Al2O3@C催化剂增进了酸位点的可及性,从而促进了其串联步骤中包含的脱水反应的发生,进而有效提高催化剂的反应活性.