Phonons driven at high frequency

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SUMMARY

The discussion centers on the behavior of phonons in one-dimensional monatomic crystals when subjected to high-frequency driving forces. It is established that when the driving frequency exceeds the maximum phonon frequency (ωmax), phonons cease to propagate and instead decay. The participants explore obtaining a wave number (k) expression using a decaying function, specifically considering solutions of the form e-γsa alongside the original oscillatory solution Aei(ksa-ωt). The challenge lies in integrating this decay into the equation of motion without yielding a solvable form for 'k'.

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  • Understanding of phonon dispersion relations in one-dimensional crystals
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  • Knowledge of decay functions and their mathematical implications
  • Proficiency in solving differential equations related to physical systems
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  • Research the derivation of phonon dispersion relations in one-dimensional monatomic crystals
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  • Explore the implications of high-frequency oscillations on crystal lattice dynamics
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Students and researchers in condensed matter physics, particularly those studying phonon behavior in crystalline structures and the effects of high-frequency oscillations on material properties.

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Homework Statement


For one-dimensional monatomic crystals, the dispersion plot for phonons has a maximum frequency ωmax. If a driving force oscillates the crystal beyond this frequency, the phonon will no longer propagate and will instead decay as it gets further from the external source of oscillation. Obtain an expression for k (the wave number) using a decaying function rather than an oscillating one.

Homework Equations


Original "oscillatory" solution of form Aei(ksa-ωt) where s indexes the atoms of the crystal and a is the spacing between crystals. The equation of motion is given by d2us/dt2 = C (us+1+us-1-2us) where us is the displacement of the sth atom from equillbrium and C is the constant of interaction between atoms.

The Attempt at a Solution


I can tack on an e-γsa to the oscillatory solution but the result of substituting that in the equation of motion above does not look like it can be solved for 'k'. Subsequent questions suggest that a closed-form solution is what is being asked for. I also considered a solution that simply decayed (vs decaying a sinusoidal function) just of the form e-γsa but I am not sure how k would fit into such a solution.
 
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