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PHY 521/321: Condensed Matter Physics I
Prof. S. Teitel stte@pas.rochester.edu  Spring 2010
Problem Set 4
Due Thursday, April 1, in lecture
 Problem 1
(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) Basecentered cubic (simple cubic with additional points in the centers of the horizontal faces of the cubic cell).
b) Sidecentered cubic (simple cubic with additional points in the centers of the vertical faces of the cubic cell).
c) Edgecentered cubic (simple cubic with additional points at the midpoints of the lines joining nearest neighbors).
 Problem 2
(Ashcroft & Mermin problem 4.6)
The facecentered cubic is the most dense and the simple cubic is the least dense of the three cubic Bravais lattices. The diamond structure is less dense than any of these One measure of this is that the coordination numbers are: fcc, 12; bcc, 8; sc, 6; diamond, 4. Another is the following: Suppose identical solid spheres are distributed through space in such a way that their centers lie on the points of each of these four structures, and spheres on neighboring points just touch, without overlapping. (Such an arrangement of spheres is called a closepacking arrangement.) Assuming that the spheres have unit density, show that the density of a set of closepacked spheres on each of the four structures (the "packing fraction") is:
fcc:  sqrt(2)π/6 = 0.74 
bcc:  sqrt(3)π/8 = 0.68 
sc:  π/6 = 0.52 
diamond:  sqrt(3)π/16 = 0.34 
 Problem 3
a) If a_{1}, a_{2}, a_{3} are the primitive vectors of a Bravais Lattice, show that the volume of a primitive cell is:
v = a_{1}·(a_{2}×a_{3})
b) Using the definition of the primitive vectors of the reciprocal lattice:
b_{1} = 2π 
a_{2}×a_{3} a_{1}·(a_{2}×a_{3})  , etc. 
show that:
b_{1}·(b_{2}×b_{3}) = 
(2π)^{3} a_{1}·(a_{2}×a_{3}) 
and hence that the volume of a primitive cell of the reciprocal lattice is (2π)^{3}/v.
c) The nth Brillouin Zone can be defined as that region of kspace which can be reached from the origin by crossing exactly n1 Bragg planes and no more or less. Alternatively, the nth Brillouin Zone can be defined as the set of points in kspace that have the origin as their nth nearest reciprocal lattice point. Use this later definition to show that each Brillouin Zone is a primitive cell of the reciprocal lattice (Hint: consider the proof we gave that the WignerSeitz cell was a primitive cell of the Bravais lattice).

