PHZ 6426 (Solid State I) Fall 1997
Homework 4, due October 3
Throughout this problem, all reciprocal lattice directions (hkl) are
expressed in terms of the primitive vectors defined in Ashcroft and Mermin
Eq. (5.12), and all energies are measured in units of
h2/(8ma2).
- Construct the "empty lattice" band structure of an fcc Bravais lattice
along the (111) reciprocal lattice direction. Draw the energy bands along
this direction within the reduced zone scheme. Show all levels up
to an energy six times that of the lowest band at the zone boundary.
Indicate the precise energy of each level at the zone center and at the
zone boundary.
- Suppose that the crystal has a weak periodic potential having the
following nonzero Fourier components:
- V( K in {111}) = 0.3.
- V( K in {200}) = 0.4.
Recall that {hkl} means "(hkl) and all directions
related to it by crystal symmetry".
All other Fourier components are negligibly small.
Consider each of the empty-lattice bands from part 1. Calculate to
first order in the lattice potential the energy of each of these
bands at the zone center and at the zone boundary along the (111)
direction.
Sketch the (111) energy bands across the entire zone.
Kevin Ingersent's home page
Kevin Ingersent /
ingersent@phys.ufl.edu /
Last modified: Sep 30, 1997.