Nonlinear effects of number density of solvent molecules on solvation dynamics

1996 ◽  
Vol 105 (14) ◽  
pp. 5971-5978 ◽  
Author(s):  
Akira Yoshimori
2004 ◽  
Vol 03 (01) ◽  
pp. 117-144 ◽  
Author(s):  
AKIRA YOSHIMORI

This article reviews microscopic development of time dependent functional method and its application to chemical physics. It begins with the formulation of density functional theory. The time dependent extension is discussed after the equilibrium formulation. Its application is explained by solvation dynamics. In addition, it reviews studies of nonlinear effects on polar liquids and simple mixtures.


1990 ◽  
Vol 10 (5-6) ◽  
pp. 413-429 ◽  
Author(s):  
A. Declémy ◽  
C. Rulliére ◽  
Ph. Kottis

The dynamics of the Time-Dependent Fluorescence Shift (TDFS) of a rigid polar excited probe dissolved in alcohol solvents at different temperatures have been studied by picosecond time-resolved spectroscopy. The results are compared to previously published results on well characterized polar systems. These results show that solvation dynamics in such systems are strongly scaled by the microscopic (singleparticle) reorientation time τM of the solvent molecules and/or by the (macroscopic) longitudinal relaxation time τL of the solvent. The key point governing this scaling is the relative interaction between the solvent molecules and the probe compared to the interaction between the solvent molecules. It is also shown that specific interactions, such as hydrogen bonded-complex formation, may play an important role.


2016 ◽  
Vol 18 (23) ◽  
pp. 15534-15544 ◽  
Author(s):  
Ken-ichi Amano ◽  
Yunfeng Liang ◽  
Keisuke Miyazawa ◽  
Kazuya Kobayashi ◽  
Kota Hashimoto ◽  
...  

A theory that transforms the force curve into a hydration structure is derived, and the transformation is demonstrated.


1995 ◽  
Vol 78 (1-2) ◽  
pp. 239-266 ◽  
Author(s):  
Harold L. Friedman ◽  
Fernando O. Raineri ◽  
Fumio Hirata ◽  
Baw-Ching Perng

2006 ◽  
Vol 125 (24) ◽  
pp. 244501 ◽  
Author(s):  
Shuhei Murata ◽  
Akira Yoshimori

2016 ◽  
Vol 18 (29) ◽  
pp. 19973-19974
Author(s):  
Ken-ichi Amano ◽  
Yunfeng Liang ◽  
Keisuke Miyazawa ◽  
Kazuya Kobayashi ◽  
Kota Hashimoto ◽  
...  

Correction for ‘Number density distribution of solvent molecules on a substrate: a transform theory for atomic force microscopy’ by Ken-ichi Amano et al., Phys. Chem. Chem. Phys., 2016, 18, 15534–15544.


Author(s):  
Abraham Nitzan

Solvent dynamical effects on relaxation and reaction process were considered in Chapters 13 and 14. These effects are usually associated with small amplitude solvent motions that do not appreciably change its configuration. However, the most important solvent effect is often equilibrium in nature—modifying the free energies of the reactants, products, and transition states, thereby affecting the free energy of activation and sometime even the course of the chemical process. Solvation energies relevant to these modifications can be studied experimentally by calorimetric and spectroscopic methods, and theoretically by methods of equilibrium statistical mechanics. With advances of experimental techniques that made it possible to observe timescales down to the femtosecond regime, the dynamics of solvation itself became accessible and therefore an interesting subject of study. Moreover, we are now able to probe molecular processes that occur on the same timescale as solvation, making it necessary to address solvation as dynamic in addition to energetic phenomenon. This chapter focuses on the important and most studied subclass of these phenomena—solvation dynamics involving charged and polar solutes in dielectric environments. In addition to their intrinsic importance, these phenomena play a central role in all processes involving molecular charge rearrangement, most profoundly in electron transfer processes that are discussed in the next chapter. Consider, as a particular example, a neutral (q = 0) atomic solute embedded in a dielectric solvent, that undergoes a sudden change of its charge to q = e, where e is the magnitude of the electron charge. This can be achieved, for example, by photoionization. The dipolar solvent molecules respond to this change in the local charge distribution by rotating in order to make their negative end point, on the average, to the just formed positive ion. Thus, the solvent configuration changes in response to the sudden change in a local charge distribution. The driving force for this change is the lowering of overall free energy that accompanies the buildup of solvent polarization.


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