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Volumn 57, Issue 8, 1998, Pages 4782-4797

Unified view of step-edge kinetics and fluctuations

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EID: 0001232154     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.57.4782     Document Type: Article
Times cited : (101)

References (61)
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    • Rubenstein, L.1
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    • O. Pierre-Louis, Ph.D. thesis, Université J. Fourier-Grenoble 1, 1997 (unpublished);O. Pierre-Louis and C. Misbah (unpublished).
    • Pierre-Louis, O.1    Misbah, C.2
  • 42
    • 0000967138 scopus 로고    scopus 로고
    • See also Appendix D for comments on the notation used in this paper
    • S. V. Khare and T. L. Einstein, Phys. Rev. B 54, 11 752 (1996). See also Appendix D for comments on the notation used in this paper.
    • (1996) Phys. Rev. B , vol.54 , pp. 11752
    • Khare, S.1    Einstein, T.2
  • 48
    • 4243985566 scopus 로고    scopus 로고
    • private communication. Specifically, from his Eq. (6-i) it follows that our kinetic coefficient (Formula presented), where (Formula presented) is the attachment/detachment factor from the step edge and (Formula presented) is the extra barrier (above the normal diffusion barrier on the terrace) associated with the appropriate side of the step edge. (The prefactor of (Formula presented) is assumed to be the same as that of (Formula presented).) Then it quickly follows that (Formula presented). For (Formula presented), (Formula presented), where (Formula presented) but in general there is no simple connection between (Formula presented) and (Formula presented). In fact, in the limit of high temperature, (Formula presented) In Fig. 5 of Ref. 23(Formula presented) and (Formula presented) are labeled (Formula presented) and (Formula presented) respectively
    • D. Kandel, Phys. Rev. Lett. 78, 499 (1997) and private communication. Specifically, from his Eq. (6-i) it follows that our kinetic coefficient (Formula presented), where (Formula presented) is the attachment/detachment factor from the step edge and (Formula presented) is the extra barrier (above the normal diffusion barrier on the terrace) associated with the appropriate side of the step edge. (The prefactor of (Formula presented) is assumed to be the same as that of (Formula presented).) Then it quickly follows that (Formula presented). For (Formula presented), (Formula presented), where (Formula presented) but in general there is no simple connection between (Formula presented) and (Formula presented). In fact, in the limit of high temperature, (Formula presented) In Fig. 5 of Ref. 23, (Formula presented) and (Formula presented) are labeled (Formula presented) and (Formula presented) respectively.
    • (1997) Phys. Rev. Lett. , vol.78 , pp. 499
    • Kandel, D.1
  • 50
    • 0001718659 scopus 로고    scopus 로고
    • W. W. Pai, A. K. Swan, Z. Zhang, and J. F. Wendelken, Phys. Rev. Lett. 79, 3210 (1997). In these systems there is evidence that the dominant transport mechanism is step-edge diffusion. In our perspective, the experiment would seem to lie in the crossover region at the bottom of Fig. 3 of Ref. 33 between EC and PD behavior.
    • (1997) Phys. Rev. Lett. , vol.79 , pp. 3210
    • Pai, W.1    Swan, A.2    Zhang, Z.3    Wendelken, J.4
  • 53
    • 85037887500 scopus 로고    scopus 로고
    • B. Blagojević and P. M. Duxbury (unpublished)
    • P. M. Duxbury (private communication);B. Blagojević and P. M. Duxbury (unpublished).
    • Duxbury, P.1
  • 54
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    • Handbook of Mathematical Functions, edited by M. Abramowitz and I. A. Stegun (Dover Publications Inc., New York, 1972).
    • (1972) Handbook of Mathematical Functions


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