Export citation

Export citation

Choose format for download:

Download Citation
  • Access by Xinjiang University

Driven dynamics: A photodriven Frenkel-Kontorova model

Bambi Hu1,4 and Jian-Yang Zhu1,2,3,*

  • 1Centre for Nonlinear Studies and Department of Physics, Baptist University, Hong Kong
  • 2Department of Physics, Jiangxi Normal University, Nanchang 330027, People’s Republic of China
  • 3Department of Physics, Beijing Normal University, Beijing 100875, People’s Republic of China
  • 4Department of Physics and Texas Center for Superconductivity, University of Houston, Houston, Texas 77204

  • *Author to whom correspondence should be addressed. Email address: zhujy@public.nc.jx.cn

Phys. Rev. E 65, 016202 – Published 11 December, 2001

DOI: https://doi.org/10.1103/PhysRevE.65.016202

Abstract

In this study, we examine the dynamics of a one-dimensional Frenkel-Kontorova chain consisting of nanosize clusters (the “particles”) and photochromic molecules (the “bonds”), also being subjected to a periodic substrate potential. Whether the whole chain should be running or be locked depends on both the frequency and the wavelength of the light (keeping the other parameters fixed), as observed through numerical simulation. In the locked state, the particles are bound at the bottom of the external potential and vibrate backwards and forwards at a constant amplitude. In the running state, the initially fed energy is transformed into directed motion as a whole. It is of interest to note that the driving energy is introduced to the system by the irradiation of light, and the driven mechanism is based on the dynamical competition between the inherent lengths of the moving object (the chain) and the supporting carrier (the isotropic surface). However, the most important feature is that the light-induced conformational changes of the chromophore lead to the time-and-space dependence of the rest lengths of the bonds.

References (13)

  1. Ya. Frenkel and T. Kontorova, Phys. Z. Sowjetunion 13, 1 (1938).
  2. R. A. Guyer and M. D. Miller, Phys. Rev. A 17, 1774 (1978); M. Büttiker and R. Landauer, 23, 1397 (1981).
  3. F. Marchesoni, Phys. Rev. B 34, 6536 (1986); P. Hänggi, F. Marchesoni, and P. Sodano, Phys. Rev. Lett. 60, 2563 (1988); F. Marchesoni, 73, 2394 (1994).
  4. L. M. Floria and J. J. Mazo, Adv. Phys. 45, 505 (1996).
  5. B. N. J. Persson, Phys. Rev. Lett. 71, 1212 (1993); Phys. Rev. B 48, 18 140 (1993).
  6. M. V. Paliy, O. M. Braun, T. Dauxois, and Bambi Hu, Phys. Rev. E 56, 4025 (1997); O. M. Braun, M. V. Paliy, J. Röder, and A. R. Bishop, 63, 036129 (2001); A. Vanossi, J. Röder, A. R. Bishop, and V. Bortolani, 63, 017203 (2001).
  7. H. S. J. van der Zant et al., Phys. Rev. Lett. 74, 174 (1995); M. Weiss and F.-J. Elmer, Phys. Rev. B 53, 7539 (1996); T. Strunz and F.-J. Elmer, Phys. Rev. E 58, 1601 (1998); 58, 1612 (1998).
  8. O. M. Braun et al., Phys. Rev. Lett. 78, 1295 (1997); Phys. Rev. E 55, 3598 (1997); 62, 4235 (2000).
  9. S. Watanabe et al., Physica D 97, 429 (1996).
  10. P. J. Martinez et al., Phys. Rev. B 56, 87 (1997).
  11. M. Porto, M. Urbakh, and J. Klafter, Phys. Rev. Lett. 84, 6058 (2000).
  12. Light-induced reversible isomerizations between two forms having different absorption spectra are referred to photochromism, and the compounds capable of these reactions are called photochromic molecules. Diarylethenes are known as the new class of thermally irreversible and fatigue resistant photochromic molecules.
  13. It is notable that a new family of photochromic molecules are becoming a strong candidate for optical data storage and/or other molecular electronic devices. See, e.g., (a) T. Tsujioka et al., Appl. Phys. Lett. 78, 2282 (2001); (b) M. Irie, in Photochromism: Memories and Switches, special thematic issue of Chem. Rev. 100, 5 (2000).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation