Nonadiabatic dynamics simulation of keto isocytosine: a comparison of dynamical performance of different electronic-structure methods

2017 ◽  
Vol 19 (29) ◽  
pp. 19168-19177 ◽  
Author(s):  
Deping Hu ◽  
Yan Fang Liu ◽  
Andrzej L. Sobolewski ◽  
Zhenggang Lan

Different reaction channels are obtained in the nonadiabatic dynamics simulations of isocytosine at CASSCF and ADC(2) levels.

2019 ◽  
Vol 21 (31) ◽  
pp. 17109-17117 ◽  
Author(s):  
Diandong Tang ◽  
Wei-Hai Fang ◽  
Lin Shen ◽  
Ganglong Cui

The MM/SQC method combined with electronic structure calculations at the level of OM2/MRCI and on-the-fly nonadiabatic dynamics simulations.


2016 ◽  
Vol 18 (1) ◽  
pp. 403-413 ◽  
Author(s):  
Bin-Bin Xie ◽  
Shu-Hua Xia ◽  
Xue-Ping Chang ◽  
Ganglong Cui

Sequential vs. concerted S1 relaxation pathways.


2018 ◽  
Vol 20 (9) ◽  
pp. 6524-6532 ◽  
Author(s):  
Meng Che ◽  
Yuan-Jun Gao ◽  
Yan Zhang ◽  
Shu-Hua Xia ◽  
Ganglong Cui

Pigment Yellow 101 (PY101) is widely used as a typical pigment due to its excellent excited-state properties.


2021 ◽  
Author(s):  
Yinan Shu ◽  
Linyao Zhang ◽  
Shaozeng Sun ◽  
Yudong Huang ◽  
Donald Truhlar ◽  
...  

Direct dynamics by mixed quantum–classical nonadiabatic methods is an important tool for understanding processes involving multiple electronic states. Very often, the computational bottleneck of such direct simulation comes from electronic structure theory. For example, at every time step of a trajectory, nonadiabatic dynamics requires potential energy surfaces, their gradients, and the matrix elements coupling the surfaces. The need for the couplings can be alleviated by employing the time derivatives of the wave functions, which can be evaluated from overlaps of electronic wave functions at successive timesteps. However, evaluation of overlap integrals is still expensive for large systems. In addition, for electronic structure methods for which the wave functions or the coupling matrix elements are not available, nonadiabatic dynamics algorithms become inapplicable. In this work, building on recent work by Baeck and An, we propose new nonadiabatic dynamics algorithms that only require adiabatic potential energies and their gradients. The new methods are named curvature- driven coherent switching with decay of mixing (κCSDM) and curvature-driven trajectory surface hopping (κTSH). We show how powerful these new methods are in terms of computer time and good agreement with methods employing nonadiabatic coupling vectors computed in conventional ways. The lowering of the computational cost will allow longer nonadiabatic trajectories and greater ensemble averaging to be affordable, and the ability to calculate the dynamics without electronic structure coupling matrix elements extends the dynamics capability to new classes of electronic structure methods.


2014 ◽  
Vol 16 (21) ◽  
pp. 9760-9775 ◽  
Author(s):  
R. B. Gerber ◽  
D. Shemesh ◽  
M. E. Varner ◽  
J. Kalinowski ◽  
B. Hirshberg

Recent progress in “on-the-fly” trajectory simulations of molecular reactions, using different electronic structure methods is discussed, with analysis of the insights that such calculations can provide and of the strengths and limitations of the algorithms available.


2015 ◽  
Vol 17 (15) ◽  
pp. 9687-9697 ◽  
Author(s):  
Shu-Hua Xia ◽  
Bin-Bin Xie ◽  
Qiu Fang ◽  
Ganglong Cui ◽  
Walter Thiel

The combined electronic structure computations and nonadiabatic dynamics simulations show that excited-state intramolecular proton transfer to carbon atoms can be ultrafast.


Author(s):  
Sebastian Mai ◽  
Leticia Gonzalez

<div>Nonadiabatic dynamics simulations of molecular systems with a large number of nuclear degrees of freedom become increasingly feasible, but there is still a need to extract from such simulations a small number of most important modes of nuclear motion, for example to obtain general insight or to construct low-dimensional model potentials for further simulations. Standard techniques for this dimensionality reduction employ statistical methods that identify the modes that account for the largest variance in nuclear positions. However, large-amplitude motion is not necessarily a good proxy for the influence of a mode on the excited-state wave function evolution. Hence, here we report a number of analysis techniques aimed at extracting from nonadiabatic dynamics simulations the vibrational modes that are most strongly affected by the electronic excitation process and that most significantly affect the interaction of the electronic states. The first technique identifies coherent nuclear motion after excitation from the ratio between total variance and variance of the average trajectory. The second strategy employs linear regression to find normal modes that have a statistically significant effect on excitation energies, energy gaps, or wave function overlaps. The third approach uses time-frequency analysis to find normal modes where the vibrational frequencies change in the course of the dynamics simulation. All three techniques are applied to the case of surface hopping trajectories of [Re(CO)<sub>3</sub>(Im)(Phen)]<sup>+</sup> (Im=imidazole; Phen=1,10-phenanthroline), showing that in this transition metal complex the nonadiabatic dynamics is dominated by a small number of carbonyl and phenanthroline in-plane stretch modes.</div><div><br></div>


RSC Advances ◽  
2016 ◽  
Vol 6 (46) ◽  
pp. 39542-39552 ◽  
Author(s):  
Wanqing Gao ◽  
Le Yu ◽  
Xiaolei Zheng ◽  
Yibo Lei ◽  
Chaoyuan Zhu ◽  
...  

On-the-fly trajectory surface hopping dynamics simulations on the cis ↔ trans photoisomerization mechanisms of bridged-azobenzene upon S1 excitation at the CASSCF level.


2020 ◽  
Author(s):  
Mohammad R. Momeni ◽  
Zeyu Zhang ◽  
Farnaz A. Shakib

A multi-faceted approach is introduced for investigating the effects of intrinsic and guest(water)-induced structural transformations/deformations and heterogeneity on catalytic activity of the 2D π-stacked layered Co3(HTTP)2, HTTP = hexathiotriphenylene, metal-organic framework. Through comprehensive molecular dynamics simulations coupled with periodic and cluster electronic structure calculations, we uncover a complex array of catalytically active sites in 2D Co3(HTTP)2 MOF which would have been entirely missed if conventional static electronic structure methods were to be employed.


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