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PHY 521: Condensed Matter Physics I
Prof. S. Teitel stte@pas.rochester.edu ---- Spring 2014

Problem Set 3

Due Wednesday, March 5, in lecture

  • Problem 1

    In this problem you will derive the dispersion relation and other properties of the surface plasmon!

    Consider a metal with a surface in the xy plane, i.e. z > 0 is metal and z < 0 is the vacuum. The surface plasmon is a solution to Maxwell's equations of the form,

    Ex = Aeiqx eKzeiωt,     Ey =0,     Ez = BeiqxeKzeiωt         for z > 0

    Ex = Ceiqx eK'zeiωt,     Ey =0,     Ez = DeiqxeK'zeiωt         for z < 0

    with q, K, K' real and K, K' positive (so that the amplidue of the wave decays as z moves away from z=0).

    Assume that there is no charge density induced in the bulk of the metal, i.e. E=0, (but there may be induced surface charge). By requiring the above expression to satisfy Maxwell's equation, and to satisfy the usual electromagnetic boundary conditions, tangential component of E continuous and normal component of εE continuous, find equations relating the unknown amplitudes A, B, C, D to each other, and relating q, K, K' to each other and to the frequency ω.

    Use for the metal the dielectric function ε(ω) = 1+4πiσ(ω)/ω, with σ(ω) the ac Drude conductivity. You may make the assumption that ωτ >> 1 so that ε(ω) ≈ 1 − (ωP/ω)2, where ωP=4πne2/m is the plasma frequency.

    Use your results above to solve for q as a function of ω. Plot q2c2 vs ω2, and indicate for what range of ω there is indeed a solution with the desired properties.

    Compute the surface charge density induced on the surface of the metal? (Hint: remember your electrostatics!)

    What is the dispersion relation ω(q) in the limit of small q? Show that as q gets very large (i.e. qc >> ω) there is a solution at frequency ω = ωP/√2. What is the polarization of this wave when ω = ωP/√2?

  • Problem 2

    (Ashcroft & Mermin problem 4.1)
    In each of the following cases indicate whether the structure is a Bravais lattice. If it is, give three primitive vectors; if it is not, describe it as a Bravais lattice with a small as possible a basis.

    a) Base-centered cubic (simple cubic with additional points in the centers of the horizontal faces of the cubic cell).

    b) Side-centered cubic (simple cubic with additional points in the centers of the vertical faces of the cubic cell).

    c) Edge-centered cubic (simple cubic with additional points at the midpoints of the lines joining nearest neighbors).