Lecture 7 Flashcards
How do the modes of a crystal change when the basis has more than one atom type?
There are additional vibrational modes
Describe the model of a diatomic chain of atoms where the masses m1 and m2 (where m1 > m2) alternate
a = lattice parameter
u_n = displacement of n-th atom
Atom n is at a distance na from the origin. Atom n+1/2 is at a distance (n+1/2)a from the origin.
Give the two equations of motion for a diatomic chain of atoms
Give the travelling wave solution for the displacement of the n-th atom in a diatomic chain of atoms
u_n = displacement of the n-th atom
A = amplitude
Give the travelling wave solution for the displacement of the (n+1/2)-th atom in a diatomic chain of atoms
u_n+1/2 = displacement of the (n+1/2)-th atom
B = amplitude
Give the equation for the dispersion relationship for vibrations of a diatomic chain of atoms
ω = angular frequency
C = force constant
m1, m2 = mass
k = wavevector
a = lattice constant
Describe the shape of the dispersion relationship for vibrations of a diatomic chain of atoms with nearest neighbour harmonic forces
What is the optical mode of the dispersion relationship for vibrations of a diatomic chain of atoms?
The branch that occurs when the square root term is positive. m1 and m2 oscillate in anti-phase.
Give the equation for the optical mode of the dispersion relationship for vibrations of a diatomic chain of atoms
Describe the limiting case of the optical mode
m1»_space; m2
The heavy atoms are almost stationary and only the light atoms vibrate.
How can optical modes be driven?
By oscillating the electric fields of photons.
What is the acoustic mode of the dispersion relationship for vibrations of a diatomic chain of atoms?
The branch that occurs when the square root term is negative. m1 and m2 oscillate in phase.
Give the equation for the optical mode of the dispersion relationship for vibrations of a diatomic chain of atoms
What is a longitudinal wave?
Atoms that oscillate along the direction of propagation
What is a transverse wave?
Atoms that oscillate perpendicular to the propagation direction. There are two distinct polarisations.