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Diapositiva 1

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Nonlinear lattice dynamics: Phonons vs Intrinsic Localized Modes (Discrete Breathers) ... The appearance of dark lines of mica muscovite ... – PowerPoint PPT presentation

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Title: Diapositiva 1


1
Intrinsic Localized modes A mechanism for the
migration of defects
Jesús Cuevas Maraver Nonlinear Physics
Group Universidad de Sevilla
2
Outline
  • Nonlinear lattice dynamics Phonons vs Intrinsic
    Localized Modes (Discrete Breathers)
  • A classical nonlinear model Frenkel-Kontorova
  • Stationary and moving breathers
  • Point defects Impurities, vacancies and
    interstitials
  • Interaction between discrete breathers and
    vacancies
  • Double vacancies and interstitials
  • Conclusions
  • References
  • J. Phys. A 35 (2002) 10519
  • Phys. Lett. A 315 (2003) 364

3
Nonlinear lattices
  • A great number of systems can be described by
    oscillator networks (crystals, biomolecules,
    Josephson-junctions arrays)
  • The interactions between the oscillators is
    nonlinear, although most of the times they are
    approximated by linear functions
  • An oscillator network is described by the
    following Hamiltonian

Interaction potential
On-site potential
Kinetic Energy
4
Linear lattices
Linear vibrational modes phonons
5
Nonlinear lattices
Phonons Intrinsic localized modes (breathers)
6
Discrete breathers
  • Exact periodic and localized solutions of the
    dynamical equations that exist due to
    nonlinearity and discreteness.
  • They exist as long as two conditions are
    fulfilled (MacKay-Aubry theorem, 1994)
  • The on-site potential is nonlinear
  • The breather frequency does not resonate with
    phonons
  • They have been generated in Josephson-junction
    arrays and observed in molecular crystals (PtCl).
  • They are speculated to play an important role in
  • DNA transcription and denaturation bubbles
  • The appearance of dark lines of mica muscovite
  • Reconstructive transformations in layered
    silicates

7
The Frenkel-Kontorova model
  • Introduced in 1938 to study the dynamics of
    dislocations.
  • It consists of a on-site periodic potential
    (sine-Gordon)
  • The particles are located at the bottom of the
    potential

8
Breathers in Frenkel-Kontorova
  • The Frenkel-Kontorova model supports discrete
    breathers due to the nonlinearity of the on-site
    potential

9
Mobile breathers
  • In some conditions, a static breather can be
    perturbed leading to a mobile state.
  • These solutions are not exact can only be
    observed through numerical simulations.
  • Contrary to static breather, they are not
    supported in every nonlinear lattices.
  • One of the systems supporting moving breathers is
    the Frenkel-Kontorova model.

10
Mobile breathers in Frenkel-Kontorova
11
Point defects
  • The Frenkel-Kontorova is the simplest way of
    modelling vacancies (an empty well) and
    interstitials (two particles in the same well).

12
Moving breathers and vacancies
  • We consider a modified Frenkel-Kontorova model
    with a nonlinear interaction potential
  • W(x) is the Morse potential. b is the inverse
    width of the potential

13
Moving breathers and vacancies
  • We have studied the effect of varying the
    potential width in the interaction.
  • For each value of the potential width, the
    interaction is studied in function of the kinetic
    energy of the moving breather.
  • When the moving breather reaches the vacancy, the
    latter can move forwards, backwards or remain at
    rest. However, there is no correlation between
    the kinetic energy and the number of vacancy
    jumps

14
Critical values
  • Statistical analysis
  • For bgtbf the vacancy does not move forwards.
  • For bb1ltbltbb2 there exist a critical value of the
    kinetic energy for vacancy movement

15
Vacancy moving backwards
16
Vacancy moving backwards
17
Vacancy moving forwards
18
Vacancy moving forwards
19
Double vacancy
  • This configuration needs an narrow interaction
    potential.
  • The double vacancy does not move forwards.
    Instead, it can be broken.
  • The observed regimes are now rest, breaking and
    forwards movement (with breaking). The latter
    needs b to be small enough.
  • The threshold kinetic energy is also observed.

20
Double vacancy breaking
21
Interstitials
  • Preliminary results.
  • A threshold kinetic energy is always observed.
  • For bgtbc, the interstitial always moves forwards.
  • For bltbc, the interstitial can move backwards,
    forwards or remain at rest.

22
Interstitial moving forwards
23
Conclusions
  • We have described the interaction between moving
    breathers and vacancies when the interaction
    potential width is varied.
  • Two critical values of the width exist
  • Vacancy forwards movement
  • Threshold kinetic energy
  • These critical values can be determined through
    the existence and stability analysis of static
    breathers in the neighborhood of the vacancy.
  • More information
  • http//www.grupo.us.es/gfnl
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