多分形的动态描述和相变研究

本文给出了多分形的动态描述,讨论了多分形的一级、二级相变以及广义熵Kq在多分形中的应用。     

可逆热色性化合物的研究进展

本文就可逆热色性化合物的研究现状和发展趋势进行了评述, 着重介绍了可逆热色性化合物的类别、变色原理及应用等。     

具有双稳态的化学反应中的涨落现象

化学反应中的非线性动力学行为一直受到人们的普遍的关注[1-3]Schlogl等人[4,5]曾用两个自催化反应模式说明连续的二级相变和不连续的一级相变特征．而在文献[6，7]中，我们提出在具有双稳态的化学反应中，存在类一级与类二级相变之间的转变点，而此转变点也具有类似Landau二级     

光敏异构化智能生物开关的进展

引出光敏异构化智能生物开关的概念。介绍了可逆光敏异构化生物物质的机制和特点, 并结合这个领域的研究和发展对其进行了较全面的讨论。探讨了可逆异构化开关物质在光记忆、电化学控制、生物传感器等方面的应用, 并对它的未来前景作出展望。     

D-、L-和DL-缬氨酸晶体低温旋光性研究

由于电弱力宇称不守恒,氨基酸对映体分子间存在宇称破缺能差，通过Z0粒子的介导，在某临界温度下，氨基酸分子会发生类似于BCS(Bardeen-Cooper-Schrieffer)超导的玻色凝聚,引起二级相变,理论推测相变温度约在250 K.本文通过原位测量在240～290 K下， D型、L型和DL型缬氨酸晶体的旋光角随温度的变化，发现D型和DL型缬氨酸晶体在270 K有旋光角跃变， L型缬氨酸晶体的旋光角基本不变，为Salam预言的二级相变提供了直接证据.     

关于Clapeyron方程适用条件的讨论

本文比较了近年来国内外出版的物理化学教材关于Clapeyron方程适用条件的不同表述,分析了不同表述的特点,提出了Clapeyron方程适用条件应统一严格表述并增加二级相变教学内容的建议,以消除教学中的误解和困惑。     

LaFe13-xSix (1.2≤x≤2.2)化合物的磁场诱导熵变与磁场的关系

通过真空电弧熔炼、长时间真空热处理的方法获得了单相NaZn13-型LaFe13-xSix(1.2≤x≤2.2)化合物,并测量了它们的磁化强度与磁场和温度的关系,用Maxwell关系式计算出在不同磁场下化合物的熵变ΔS。用Landau的二级相变理论及平均场近似下的标度律,分析拟合了LaFe13-xSix化合物ΔS与H之间的关系,对于具有一级和二级相变的材料,发现均存在ΔS∝H2/3的关系,只是拟合得到的参数不同。采用熵变峰值拟合得到的参数能够反映材料中一级磁性相变的程度,研究磁场诱导的熵变与磁场的关系可以为磁制冷研制提供指导。     

钴卟啉络合物的氧结合性能及其在功能材料中的应用

钴卟啉可与氧发生迅速、可逆的结合反应,是有效的氧载体,已被用于氧气吸收、光学传感器和氧气选择性分离膜。综述了钴卟啉的立体结构、配住体、环境等对其与氧可逆结合性能的影响,以及钴卟啉在功能材料中的应用。     

氧化还原可逆荧光探针的研究及其在细胞成像中的应用进展

细胞氧化还原可逆状态的动态变化可以提供丰富的生理、病理信息,因此可以瞬时、动态检测细胞氧化还原状态变化的分析方法越来越受到人们的关注.基于荧光探针的荧光分析法因其直观、简便、可原位操作、信息丰富等特点,近年来在氧化还原分析等研究方面得到了较为广泛的应用.本文对近年来氧化还原可逆荧光探针研究及其在细胞成像中的应用进展进行了评述,并对其发展前景进行了展望.引用文献54篇.     

聚合物可逆互锁网络的设计、制备和应用初探

聚合物复合体系是聚合物材料重要的应用形式,发展能够充分抑制相分离的多组分聚合物复合体系制备新技术有着重要意义.利用动态交联聚合物网络拓扑结构的可逆变换,可以使不同交联聚合物网络间的分子链扩散与混合成为可能,待混合完全后再通过动态可逆共价键闭合来重筑交联网络,最终得到由不同子网络穿插互锁形成的均匀复合交联网络,即聚合物可逆互锁网络,其中的子网络之间没有共价键连接,具有相对的独立性.本文由聚合物可逆互锁网络的设计制备出发,阐述了相关方法的概念、原理和所得材料的结构特点,介绍了基于聚合物可逆互锁网络策略的聚合物材料高性能化与功能化应用实例,内容包括提升和调控力学性能、宽pH水环境中的自修复、增进本征导热率、固态聚合物电解质的优化、多组分聚合物复合体系的可控分离与可控降解以及闭环循环利用等,同时分析了与聚合物互穿网络(IPNs)的区别,最后对这类材料未来可能的发展进行了分析和展望.     

Disorder and ionic polarons in solid electrolytes

The role of ion-ion repulsion and ion-phonon coupling in superionic conduction is explored. It is argued that the order-disorder phase transition is not associated with the conductivity discontinuity, but with a higher temperature second order phase transition which has been seen in some superionic conductors and which we predict for others. The specific heat, ion distribution, and conductivity are calculated.     

Raman frequency shifts of an internal mode near the tricritical and second order phase transitions in NH4Cl

This study gives our analysis for the frequency shifts of the v2 (1708 cm-1) Raman mode in NH4Cl close to its tricritical (P=1.6 kbar) and second order (P=2.8 kbar) phase transitions. From our analysis, we extract the values of the critical exponent which describes the critical behavior of the Raman frequency shifts for this internal mode for the pressure conditions studied in NH4Cl. Our exponent value of alpha approximately 0.2 for the tricritical phase transition is close to the values of 1/16 (TTc) for the specific heat, predicted from a 3D Ising model. Our exponent values for the second order phase transition (P=2.8 kbar) for TTc are comparable with those reported in earlier studies.     

A+B2表面催化反应相变及自振荡的蒙特卡罗模拟

用MonteCarlo法研究了脱附和E－R机理对不可逆催化氧化反应A＋1／2B2→AB的相交和自振荡的影响、结果表明，（1）催化剂表面A的脱附使ZGB模型中的一级相变点消失，但对二级相交点的影响很小；当有E－R机理参与时，二级相交点消失，且E－R过程的几率对一级相交点的影响较大；当A的脱附和E－R过程同时起作用时，上述反应不存在相交（2）在ZGB模型中的二级相变点附近，反应速率随时间的变化具有明显的振荡现象，在其它位置主要表现为噪音。引入A的脱附后在二级相交点附近明显的自振荡现象依然存在；当E-R过程起作用时，随着二级相交点的消失，明显的振荡现象亦随之消失．（3）A的脱附和E－R过程对上述反应相变的影响与A的表面扩散对相变的影响有着本质的区别，因为后者只能改变相变点的位置而不能改变相变点的存在状况．     

固体样品的光声位相理论及应用研究

在R-G理论的基础上,考虑了无辐射弛豫过程对位相信号的影响,推导出新的位相公式。研究结果表明,位相(ψ)与吸收系数(β)、热扩散长(μ_s)、弛豫时的延迟时间(τ)和快弛豫与慢弛豫时的热量比(R)有关。并用此公式解释了稀土化合物PrF₃和叶绿素b的位相谱。PrF₃的位相由f-f跃迁的吸收系数决定,而叶绿素b两个吸收带之间的位相差是由快弛豫与慢弛豫时放出的热量比不同产生的。     

The Specific Heat of Tetramethylammonium Salts

New measurements of the (N(CH₃ )₄ )₂ MnBr₄ specific heat by adiabatic calorimetry around the ferro- paraelastic phase transition shown by the crystal around 276 K are compared with previous calorimetric studies on similar tetramethylammonium bromide compounds. The thermodynamic behaviour of the tribromides and tetrabromides derivatives together with the influence on the phase transition parameters of the cation and halogen molecular substitutions are examined. The thermal relaxation experiments permit to study the behaviour of the crystals thermal conduction as a function of the temperature. Finally, the Landau theory for second order phase transitions is used to describe the thermodynamic behaviour of some of these crystals. This revised version was published online in July 2006 with corrections to the Cover Date.     

A simple molecular theory of a nematic–nematic phase transition in highly polar compounds

Abstract

We have extended an earlier molecular model which was developed to explain the double reentrant sequence in highly polar compounds to predict the possibility of a nematic (N₁)–nematic (N₂) phase transition in such compounds. At moderate densities the dipolar interactions would give rise to an antiparallel near neighbour arrangement of the polar molecules while at higher densities, the dipole–induced dipole and chain–chain dispersion interactions give rise to a parallel configuration. The N₁–N₂ transition corresponds to a jump in the relative concentration of the two species. Using the mean field approximation we have calculated the phase diagram. The weak first order transition disappears above a critical point as a function of an appropriate parameter. We have also calculated the specific heat anomaly around the transition region.     

Theory of the orientational ordering for dimers with conformational flexibility

In the self-consistent field approximation a theory of the orientational ordering is developed for the melt of dimers containing two mesogenic fragments capable of conformational reorganization. Discrete conformations of the dimers (rotational isomers) are characterized by the values of valence angles. Both three-dimensional and two-dimensional melts are considered. It is shown that the presence of bent isomers in the melt reduces the temperature of the phase transition to the anisotropic phase. For a three-dimensional system with first-order phase transition to the ordered state, the jump of the order parameter at the transition point for dimers with conformational flexibility appears to be greater than for rigid dimers. For dimers with two isomers (a linear and a bent one) the order parameter and the statistical weight of the linear isomer at the transition point depend nonmonotonously on the statistical weight of this isomer in the isotropic phase. The effect of “supercooling” of the isotropic phase for linear conformations of flexible dimers is discussed.     

Surface anchoring energy and the first order Fréedericksz transition of a NLC cell

Many authors have suggested new forms to describe the surface anchoring energy of the liquid crystal-wall interface, replacing the Rapini-Papoular (RP) formula g s = (1/2) A sin2 theta. If the RP function is considered as the primary approximation, and a lowest order modification is included, then the surface anchoring energy can be represented by g s = (1/2) A sin2 theta(1 + zeta sin2 theta). zeta characterizes the modification to the RP formula and varies for the different energy forms. It is well known that the RP formula predicts a second order Freedericksz transition. This paper points out that the transition can be first order if the modification is taken into account, in which case at the threshold point the tilt angle of the director at the middle layer of the cell, thetam, is finite. The conditions for the existence of the first order transition are obtained; zeta < 0 is required for a first order transition. The approximate expression of the threshold field is also given.     

Phenomenological theory of the nematic to lamellar phase transition in lyotropic liquid crystals

A phenomenological theory is presented to describe the nematic to lamellar phase transition in lyotropic liquid crystals. The problem of the first or second order transition is explored by means of the variation of the surfactant concentration. The possibility of the tricritical point at the nematic to lamellar phase transition is discussed in a phenomenological way. The influence of the electrolyte on this transition is also discussed by varying the coupling between the electrolyte concentration variables and the order parameters. The theoretical prediction is found to be in good qualitative agreement with experimental results.