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1.
Nature ; 406(6796): 608-11, 2000 Aug 10.
Artigo em Inglês | MEDLINE | ID: mdl-10949297

RESUMO

Analogues of mechanical devices that operate on the molecular level, such as shuttles, brakes, ratchets, turnstiles and unidirectional spinning motors, are current targets of both synthetic chemistry and nanotechnology. These structures are designed to restrict the degrees of freedom of submolecular components such that they can only move with respect to each other in a predetermined manner, ideally under the influence of some external stimuli. Alternating-current (a.c.) electric fields are commonly used to probe electronic structure, but can also change the orientation of molecules (a phenomenon exploited in liquid crystal displays), or interact with large-scale molecular motions, such as the backbone fluctuations of semi-rigid polymers. Here we show that modest a.c. fields can be used to monitor and influence the relative motion within certain rotaxanes, molecules comprising a ring that rotates around a linear 'thread' carrying bulky 'stoppers' at each end. We observe strong birefringence at frequencies that correspond to the rate at which the molecular ring pirouettes about the thread, with the frequency of maximum birefringence, and by inference also the rate of ring pirouetting giving rise to it, changing as the electric field strength is varied. Computer simulations and nuclear magnetic resonance spectroscopy show the ring rotation to be the only dynamic process occurring on a timescale corresponding to the frequency of maximum birefringence, thus confirming that mechanical motion within the rotaxanes can be addressed, and to some extent controlled, by oscillating electric fields.

2.
Opt Lett ; 20(20): 2045-7, 1995 Oct 15.
Artigo em Inglês | MEDLINE | ID: mdl-19862245

RESUMO

The complex amplitude function in the waist of a one-dimensional Hermite-Gaussian model beam is measured by a noniterative method based on the Page distribution function in the two-dimensional spatial-angular phase space. The measurement procedure is realized by an extension of the knife-edge method. The model beam is generated by means of a phase plate in conjunction with a He-Ne laser.

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