Effect of load-resisting force on photoisomerization mechanism of a single second generation light-driven molecular rotary motor

被引:0
|
作者
Pang, Xiaojuan [1 ]
Zhao, Kaiyue [1 ]
Hu, Deping [2 ]
Zhong, Quanjie [1 ]
Zhang, Ningbo [3 ]
Jiang, Chenwei [4 ]
机构
[1] China Univ Min & Technol, Sch Mat & Phys, Xuzhou 221116, Jiangsu, Peoples R China
[2] Beijing Normal Univ, Ctr Adv Mat Res, Zhuhai 519087, Peoples R China
[3] China Univ Min & Technol, Sch Mines, Xuzhou 221116, Jiangsu, Peoples R China
[4] Xi An Jiao Tong Univ, Sch Phys,Minist Educ, Shaanxi Prov Key Lab Quantum Informat & Quantum Op, Minist Educ,Key Lab Nonequilibrium Synth & Modulat, Xian 710049, Shaanxi, Peoples R China
来源
JOURNAL OF CHEMICAL PHYSICS | 2024年 / 161卷 / 16期
基金
中国国家自然科学基金;
关键词
NONADIABATIC DECAY DYNAMICS; UNIDIRECTIONAL ROTATION; DARK STATE; MOTION; IMMUNOGLOBULIN; ACCELERATION; DOMAINS; DESIGN; SPEED;
D O I
10.1063/5.0216074
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
A pivotal aspect of molecular motors is their capability to generate load capacity from a single entity. However, few studies have directly characterized the load-resisting force of a single light-driven molecular motor. This research provides a simulation analysis of the load-resisting force for a highly efficient, second-generation molecular motor developed by Feringa et al. We investigate the M-to-P photoinduced nonadiabatic molecular dynamics of 9-(2,3-dihydro-2-methyl-1H-benz[e]inden-1-ylidene)-9H-fluorene utilizing Tully's surface hopping method at the semi-empirical OM2/MRCI level under varying load-resisting forces. The findings indicate that the quantum yield remains relatively stable under forces up to 0.003 a.u., with the photoisomerization mechanism functioning typically. Beyond this threshold, the quantum yield declines, and an alternative photoisomerization mechanism emerges, characterized by an inversion of the central double bond's twisting direction. The photoisomerization process stalls when the force attains a critical value of 0.012 a.u. Moreover, the average lifetime of the excited state oscillates around that of the unperturbed system. The quantum yield and mean lifetime of the S1 excited state in the absence of external force are recorded at 0.54 and 877.9 fs, respectively. In addition, we analyze a time-dependent fluorescence radiation spectrum, confirming the presence of a dark state and significant vibrations, as previously observed experimentally by Conyard et al.
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页数:12
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