培养兴趣,引导创新——《信息光学》理论教学改革实践

重点研究了针对《信息光学》理论性强的课程和学生在学习过程中兴趣下降以及一知半解等问题,着重从提高学生理论学习兴趣,引导学生创新为出发点,通过改进PPT课件,吸引学生注意,采用深入浅出、举一反三、师生互动、启发式教学方法、理论与实际相结合、教学科研相结合等多种方法和手段,帮助学生建立正确的物理概念,促进学生对数学公式所代表的物理意义的理解,达到改善理论教学效果的目的。同时结合创新性实验建设,培养创新型和复合型人才。     

Revelation of ESIPT mechanism for the novel fluorescent system HNIBT in toluene and methanol solvents: A TDDFT study

In this work, we devote to explore excited‐state intramolecular proton transfer (ESIPT) behavior for a novel fluorescent molecule naphthalimide‐based 2‐(2‐hydroxyphenyl)‐benzothiazole (HNIBT) [New J. Chem. 2019, 43, 9152.] in toluene and methanol (MeOH) solvents. Exploring weak interactions, stable HNIBT‐enol, and HNIBT‐MeOH‐enol complex can be found in S₀ state via TDDFT/B3LYP/6‐311+G(d,p) level. Given photoexcitation, intramolecular hydrogen bond O1? H2···N3 of HNIBT‐enol and HNIBT‐MeOH‐enol is dramatically enhanced, which offers impetus for facilitates ESIPT reaction. After repeated comparisons, we verify the unavailability of intermolecular hydrogen bonding effects between HNIBT‐enol and MeOH molecules. In view of excitation, HOMO (π) → LUMO (π*) transition and the changes of electronical densities indeed impulse ESIPT tendency. Via constructing potential energy curves (PECs), for both HNIBT‐enol and HNIBT‐MeOH‐enol complex, the ESIPT could only occur along with intramolecular hydrogen bond O1? H2···N3. Through comparison, the potential barrier falls from 4.124 kcal/mol (HNIBT‐enol) to 2.132 kcal/mol (HNIBT‐MeOH‐enol). Therefore, we confirm that the ESIPT of the HNIBT system happens more easily in the MeOH solvent compared with the toluene solvent.     

Fitting elephants in the density functionals zoo: Statistical criteria for the evaluation of density functional theory methods as a suitable replacement for counting parameters

Counting parameters has become customary in the density functional theory community as a way to infer the transferability of popular approximations to the exchange‐correlation functionals. Recent work in data science, however, has demonstrated that the number of parameters of a fitted model is not related to the complexity of the model itself, nor to its eventual overfitting. Using similar arguments, here, we show that it is possible to represent every modern exchange‐correlation functional approximations using just one single parameter. This procedure proves the futility of the number of parameters as a measure of transferability. To counteract this shortcoming, we introduce and analyze the performance of three statistical criteria for the evaluation of the transferability of exchange‐correlation functionals. The three criteria are called Akaike information criterion, Vapnik‐Chervonenkis criterion, and cross‐validation criterion and are used in a preliminary assessment to rank 60 exchange‐correlation functional approximations using the ASCDB database of chemical data.     

Recent Progress in the Simulation of Chiral Systems with Real Time Propagation Methods

In this brief review, an overview about recent efforts to simulate the spectroscopic signatures of chiral molecules is given with focus on real time propagation approaches to solve the time-dependent Schrödinger equation. In particular the simulation of electric circular dichroism spectra and vibrational Raman optical activity is discussed. In comparison to linear absorption spectra, where only the response of the electric dipole moment is necessary, the response of the magnetic dipole moment and electric quadrupole moment is more intricate. Issues such as gauge origin dependence, basis set dependence, non-local potentials and the dipole approximation are addressed.     

Theoretical and experimental study of IR spectra of large phenol-acetylene clusters,Ph(Ac)n for 8 ≤ n ≤ 12

This work reports a combined theoretical and experimental study on large phenol-acetylene clusters, Ph(Ac)_n, 8 ​≤ ​n ​≤ ​12, extending our earlier work on the smaller clusters [Singh, G.; Nandi, A.; Gadre, S. R.; Chiba, T.; Fujii, A. J. Chem. Phys. 2017, 146, 154303]. Several trial cluster geometries are generated using the molecular electrostatic potential (MESP) for placing additional acetylene moieties, followed by geometry optimization at B97D/aug-cc-pVDZ level theory. The infrared spectra of energetically low-lying (within 0.5 ​mH window) isomers of the clusters are calculated and averaged. The O–H stretching band shows two peaks due to the presence of energetically close isomers differing in the arrangement of acetylenes around the O–H group. The acetylenic C–H stretching band appears around 3260 ​cm⁻¹. The C–H band shows a red shift of about 3 ​cm⁻¹ on going from n ​= ​8 to 12. Moderately size-selected IR spectra of Ph(Ac)_n (n ​= ​~10 and ~13) prepared by a supersonic jet expansion are measured for the acetylenic C–H region by infrared-ultraviolet double resonance spectroscopy combined with time-of-flight mass spectrometry. The observed spectral features are in agreement with the trends of the frequency shift and asymmetric line shape of the C–H stretch band predicted by the theoretical calculations.     

Kinetic study on solute permeation at the interface of molecular aggregates by partial filling capillary electrophoresis

Moment analysis method using partial filling CE was developed for the kinetic study on solute permeation at the interface of spherical molecular aggregates. Moment equations for partial filling CE were developed by classifying CE systems into five categories according to the migration velocities of solute and molecular aggregate. The method was applied to the study on the dissolution of electrically neutral solutes into SDS micelles. Elution peaks were measured by partial filling CE while changing the concentration of SDS and the filling ratio of SDS micellar zone to the capillary (ϕ_M). Partition equilibrium constants (K_p) and rate constants of interfacial solute permeation of SDS micelles (k_in and k_out) were determined from the first absolute and second central moments of the elution peaks by using the moment equations. Their values were comparable irrespective of ϕ_M and were almost the same as those previously measured by complete filling CE. The positive correlation of K_p with the hydrophobicity of the solutes was explained in terms of the change in k_in and k_out. It was demonstrated that the moment analysis method using partial filling CE is effective for studying solute permeation kinetics at the interface of spherical molecular aggregates.     

NH3在硼纳米管表面吸附的密度泛函理论研究

利用密度泛函理论研究了NH₃在完整和含有缺陷的硼纳米管上的吸附行为以及相关电子性质. 计算结果表明, 对于α硼纳米管, 在不同的直径和手性条件下, NH₃均倾向于吸附在配位数为6的顶位上. 电子结构计算结果表明, NH₃能够吸附在纳米管表面主要是由于N和B原子产生了较强的相互作用. 表明硼纳米管是一种潜在的NH₃气气敏材料.     

Sc,Ti,V修饰B/N掺杂单缺陷石墨烯的储氢研究

3d过渡金属修饰是改善石墨烯储氢性能的最有效途径, 但仍存在金属团聚和H₂解离导致难以脱附的问题. 提出了B/N掺杂单缺陷石墨烯(BMG/NMG)的策略来避免以上两个问题. 密度泛函理论计算结果表明, N掺杂可以使Sc, Ti, V与石墨烯的结合能提高3~4倍, B掺杂可以将Sc与石墨烯的结合能提高3倍. Sc/BMG和Sc/NMG吸附的第一个H₂不会解离. Sc/BMG中Sc吸附5个H₂, 平均氢分子结合能为-0.18～-0.43 eV, 并且可以通过在同侧锚定多个Sc原子形成Sc/C₃B₂五元环增加H₂吸附位点. Sc/NMG中每个Sc吸附6个H₂, 平均氢分子结合能为-0.17～-0.29 eV, 还可以通过在异侧修饰形成Sc/N₃/Sc单元进一步提高储氢能力. 研究结果将为设计基于3d过渡金属修饰碳材料的储氢材料提供理论基础.     

金刚石纳米线氮空位色心的表面与尺寸效应

使用大规模自旋极化密度泛函理论计算研究了表面修饰和尺寸对金刚石纳米线(DNs)中氮空位(NV)色心的几何结构、 电子结构、 磁性和稳定性的影响. 理论上设计了几种不同的DNs, 这些DNs具有不同的表面修饰(干净、 氢化和氟化), 并且直径达数百个原子. 实验结果证明, 中性(NV⁰)和带1个负电荷(NV^-)的NV色心的电子结构不受半导体表面修饰和DNs直径大小的影响, 但NV色心的稳定性对这两个因素具有不同的响应. 此外, 研究中还发现, 由于DNs中存在圆柱形表面电偶极子层, 对DNs中掺杂的NV^-色心的稳定性, 表面改性诱导了不依赖尺寸的长程效应. 特别地, 对于n型氟化金刚石表面, 掺杂在DN中的NV^-色心可以稳定存在, 而对于p型氢化表面, NV⁰则相对更稳定. 因此, 表面修饰为控制金刚石纳米线中的NV色心的电子结构和稳定性提供了一种精确有效的调控方法.     

CeO2修饰Ni3S2纳米片用于高效电催化析氧

电化学水分解制氢作为重要的生产氢能的新能源技术,包括氢气析出反应(HER)和氧气析出反应(OER).然而,OER进行的是多步电子转移过程,动力学过程缓慢且过电位高,严重制约了电解水制氢的发展.因此开发低成本、高效稳定的非贵金属催化剂替代贵金属催化剂(RuO2,IrO2)来降低过电位,减少能源消耗十分必要.Ni₃S₂由于其高导电性、高活性、低成本等优点,具有作为贵金属催化剂替代品的广阔应用前景,但其OER性能仍需进一步提高.对已有的有效OER催化剂进行表界面调控是提高催化剂性能的一种有效策略.CeO₂中的Ce3+和Ce4+价态之间可以灵活过渡,使其具有良好的电子/离子导电性、可逆的表面氧离子交换和较高的储氧能力.CeO₂的多价性使其有机会与其它基质产生强烈的电子相互作用,良好的电子/离子导电性和较高的储氧能力是提高催化剂析氧活性的有利因素.因此,用CeO₂对Ni₃S₂进行修饰是提高其析氧活性的有效途径.基于此,本文运用水热和电沉积相结合的方法将CeO₂修饰到Ni₃S₂纳米片上,制备得到生长于泡沫镍上的Ni₃S₂-CeO₂纳米片阵列(Ni₃S₂-CeO₂/NF),并运用X射线粉末衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)、X射线光电子能谱(XPS)等手段进行了表征,以三电极系统测试了其电催化析氧性能及稳定性,并通过密度泛函理论计算进行了验证.XRD结果表明,复合材料中确实存在Ni₃S₂和CeO₂.通过SEM发现,泡沫镍基底上均匀分布着Ni₃S₂纳米片阵列;电沉积CeO₂后,Ni₃S₂-CeO₂仍保持其纳米片特性,但表面变得粗糙.Ni₃S₂-CeO₂的TEM结果也证实了纳米片结构的形成,高分辨率TEM图像清晰的显示出Ni₃S₂和CeO₂之间具有明显的界面.XPS结果表明,Ni₃S₂-CeO₂的Ni 2p的结合能与Ni₃S₂相比出现负位移.与纯CeO₂的Ce 3d谱图相比,Ni₃S₂-CeO₂杂化体系中Ce4+的比例明显增加,表明Ce的价态发生了重排,部分电子转移给了Ni元素.这些结果均说明Ni₃S₂与CeO₂之间存在着较强的电子相互作用.相应的电催化测试结果显示,在1.0 M KOH中,当电流密度达到20 mA cm^–2时,Ni₃S₂/NF需提供356 mV的过电位,Ni₃S₂-CeO₂/NF只需264 mV的过电位,仅次于RuO2/NF.而且,Ni₃S₂-CeO₂/NF在中性条件下也显示出了较理想的析氧活性.Ni₃S₂-CeO₂/NF的Tafel斜率明显低于CeO₂/NF和Ni₃S₂/NF,表明其具有良好的OER反应动力学.循环伏安法和计时电位法结果均表明,Ni₃S₂-CeO₂/NF具有良好的电化学稳定性.电化学阻抗谱测试结果表明,与Ni₃S₂/NF和CeO₂/NF相比,Ni₃S₂-CeO₂/NF明显具有更小的半圆直径,说明其电荷转移阻抗更小,进一步表明CeO₂的修饰有助于催化过程中电子的快速转移.在非法拉第区域的循环伏安扫描曲线以及拟合扫描速度对电容电流曲线结果显示,Ni₃S₂-CeO₂/NF的最大电容值大于CeO₂/NF和Ni₃S₂/NF,表明其暴露了更多的活性位点,具有更大的电化学活性表面积;而且,Ni₃S₂-CeO₂/NF在400和500 mV时的电催化析氧转换频率明显高于Ni₃S₂/NF和CeO₂/NF,进一步说明Ni₃S₂-CeO₂/NF具有更高的本征催化活性.密度泛函理论计算表明,由于^*OH,^*O和^*OOH与Ni₃S₂-CeO₂中的Ni和Ce原子相互作用的存在,使得反应中间产物与Ni₃S₂-CeO₂之间的结合强度较纯Ni₃S₂或CeO₂强,使其显示出了更高的OER性能.在经过24 h连续电解后,SEM和TEM结果均表明,Ni₃S₂-CeO₂/NF材料仍保持了其纳米片形貌.稳定性测试后的XPS结果表明,Ni 2p对应的峰强度降低,而与氧化镍物种对应的峰强度增强;S元素在Ni₃S₂-CeO₂表面的信号强度明显降低.根据文献报道,在强烈的氧化环境下,过渡金属硫化物会部分转化为氧化物或氢氧化物,这通常被认为是OER过程的实际催化物种.