GRE Physics Companion: Diatomic Oscillator Chains and Acoustic and Optical Branches
The diatomic-chain dispersion relation is
| ω±2 | = κ | (1)
|
| ± κ . | (2) |
Figure 1. A compact diatomic-chain strategy: write two equations per cell, insert Bloch factors,
solve the two-by-two determinant, then examine the k = 0 and zone-edge limits to identify the
acoustic and optical branches.
1 High-value GRE facts
- Two displacement degrees of freedom per primitive cell produce two branches.
- The lower branch is acoustic; the upper branch is optical.
- ωac(0) = 0.
- At acoustic k = 0, U = V .
- At optical k = 0, m1U + m2V = 0.
- ωop2(0) = 2κ(1∕m
1 + 1∕m2).
- For m1 > m2, the zone-edge branch values are 2κ∕m1 and 2κ∕m2 in squared frequency.
- Unequal masses create a frequency gap.
- Equal masses close the gap.
- In the equal-mass limit, the two branches are a zone-folded monatomic dispersion
relation.
Part I: Original GRE-style problems
Problem 1: number of branches
A one-dimensional primitive cell contains two independent scalar displacements. The number of
normal-mode branches is
- one
- two
- three
- four
- dependent on k
Problem 2: acoustic k = 0 frequency
At
the acoustic frequency is
- 0
- infinite
Problem 3: acoustic k = 0 polarization
At
on the acoustic branch,
- U = V
- U = −V
- U = 0
- V = 0
- m1U + m2V = 0
Problem 4: optical k = 0 polarization
At
on the optical branch,
- U = V
- m1U + m2V = 0
- U = 0 always
- V = 0 always
- both masses are stationary
Problem 5: optical k = 0 frequency
The optical squared frequency at
is
- 0
- κ(1∕m1 + 1∕m2)
- 2κ(1∕m1 + 1∕m2)
- 2κ∕(m1 + m2)
- 4κ∕(m1 + m2)
Problem 6: acoustic sound speed
The long-wavelength acoustic speed is
- a
- a
- a
- aκ∕(m1 + m2)
Problem 7: zone-edge acoustic frequency
Assume
At
the acoustic squared frequency is
- 2κ∕m1
- 2κ∕m2
- κ∕(m1 + m2)
- 2κ(1∕m1 + 1∕m2)
- zero
Problem 8: zone-edge polarization
For
the acoustic zone-edge mode has
- only the lighter sublattice moving
- only the heavier sublattice moving
- both moving equally
- both moving oppositely with equal amplitude
- no motion
Problem 9: frequency gap
For unequal masses, the frequency gap occurs between
- the two k = 0 frequencies only
- the acoustic maximum and optical minimum at the zone edge
- k = 0 and k = π∕a
- positive and negative k
- two identical acoustic branches
Problem 10: equal masses
When
the frequency gap
- doubles
- remains unchanged
- vanishes
- becomes infinite
- moves to k = 0
Problem 11: numerical optical frequency
Let
Then
is closest to
- 10.00 rad/s
- 14.14 rad/s
- 17.32 rad/s
- 20.00 rad/s
- 30.00 rad/s
Problem 12: equal-mass interpretation
When the two masses become identical, the two reduced-zone branches are best interpreted
as
- two unrelated oscillator systems
- a monatomic dispersion curve folded into a smaller Brillouin zone
- two optical branches
- two acoustic branches with different sound speeds
- evidence that the normal-mode count has doubled physically
Part II: Complete worked solutions
Solution 1
The number of branches equals the number of independent displacement degrees of freedom in the
primitive cell. Two displacements give two branches. Answer: (B).
Solution 2
The lower branch begins at
This is uniform translation. Answer: (A).
Solution 3
At
the acoustic mode does not stretch the springs. Therefore
Answer: (A).
Solution 4
The optical mode keeps the cell center of mass fixed:
Answer: (B).
Solution 5
At
Answer: (C).
Solution 6
The small-k acoustic branch is
Thus
Answer: (B).
Solution 7
For
the lower zone-edge branch is associated with the heavier mass:
Answer: (A).
Solution 8
At the zone boundary the off-diagonal coupling terms vanish. The lower frequency belongs to the
heavier mass, so only that sublattice moves. Answer: (B).
Solution 9
For unequal masses, the top of the acoustic branch and bottom of the optical branch occur at the
zone edge and are separated in frequency. Answer: (B).
Solution 10
When
the two zone-edge frequencies become equal. The gap closes. Answer: (C).
Solution 11
| ωop(0) | =  | (24)
|
| =  | (25)
|
| ≈ 17.32 rad∕s. | (26) |
Answer: (C).
Solution 12
Equal masses make the two-mass cell nonprimitive. The apparent two branches arise by folding the
monatomic curve into the reduced zone. Answer: (B).
2 GRE checklist
- Count the independent displacements in the primitive cell before counting branches.
- Keep the two Bloch amplitudes separate.
- Use the lower sign for the acoustic branch and upper sign for the optical branch.
- Evaluate k = 0 and k = π∕a before attempting complicated algebra.
- Remember that optical k = 0 motion keeps the cell center of mass fixed.
- For unequal masses at the zone edge, the heavy mass belongs to the lower branch.
- Do not confuse a frequency gap with a forbidden interval of wave number.
- In the equal-mass limit, recognize zone folding rather than a genuinely new second
physical branch.
References
References
[1] PhysicsLibrary, M06-06, Discrete Oscillator Chains and Dispersion.
[2] PhysicsLibrary, M06-05, Small Oscillations and the Normal-Mode Eigenvalue
Problem.
[3] A. P. French, Vibrations and Waves, W. W. Norton, 1971.
[4] C. Kittel, Introduction to Solid State Physics, 8th ed., Wiley, 2005.