Chiral molecular motors driven by a nonhelical laser pulse.
Chiral molecular motors driven by a nonhelical laser pulse.
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由非螺旋激光脉冲驱动的手性分子马达。
DOI:
10.1002/anie.200250872
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发表时间:
2003
影响因子:
--
通讯作者:
Y. Fujimura
中科院分区:
文献类型:
--
作者:
K. Hoki;M. Yamaki;Y. Fujimura
The field of molecular motors and machines is one of the most rapidly advancing research areas in applied chemistry.[1–4] It is expected that this area will play an important role in the advent of nanoscience and nanotechnology. Most of the molecular motors reported to date have been made from chiral molecules that have asymmetric potentials. Furthermore, these motors are driven by concentration gradients that are created by thermal and chemical forces, or by the timecorrelated forces of electromagnetic radiation.[5–9] Lightdriven molecular motors are particularly interesting because their rotational directions, as well as their torque, can be controlled by utilizing the properties of light, such as photon polarization, frequency, and pulse shape.[10, 11] For example, a grid-mounted molecular dipolar rotor, driven by a circularly polarized electric field, has been theoretically studied on the basis of classical molecular dynamics.[6] It should be noted that if helical light fields, such as circularly polarized lasers are used, the chirality of the molecular motors is unnecessary.[12] Interesting experiments regarding nonhelical-light-driven chiral molecular motors have recently been reported;[8, 9] such motors consist of an alkene with two chiral centers. cis–trans Isomerization that is induced by linearly polarized visible or UV light generates repetitive unidirectional rotation around a central carbon–carbon double bond, which is followed by thermally induced cis–trans isomerization; the latter blocks reverse rotation. In those experiments, the ratedetermining step of the motor action is the thermally controlled isomerization, which is an incoherent process.[8, 9] To the best of our knowledge, there are only a few reports on molecular motors driven by using the coherent properties of radiation fields. Investigation of molecular motors driven by the coherent properties of electromagnetic fields is therefore required.In this communication, on the basis of both quantum and classical mechanical calculations, we explain how a chiral molecular motor is unidirectionally driven by a nonhelical coherent light pulse. For this purpose, 2-chloro-5-methylcyclopenta-2, 4-dienecarbaldehyde was chosen (Figure1), which is a simple, chiral molecular motor. In this communication, chiral molecules with an R formation are called (R)-