1. A linear lattice with lattice constant a has a basis of two identical atoms of mass m where the equilibrium spacing of the atoms within each unit cell is b (where b <Ə, The displacements of the atoms from their equilibrium positions are given by u,Uz, .--, Uzn-1, Uzn, Uzn+1 .... The harmonic forces between nearest-neighbour atoms are characterised by the alternating interatomic force constants B, and B.. (a) Develop: (0 The equation of motion for the 2nth atom in terms of forces exerted by the (2n – 1)th and (2n + 1)*th atoms. (ii) The equation of motion for the (2n + 1)th atom in terms of forces exerted by the 2nth and (2n + 2)th atoms. (b) Using the equations of motion and assuming travelling wave solutions of the form Uzn = Aeot-kna) and un, = Be(wt-kna-kb) derive two simultaneous equations for A and B. (c) Making use of the fact that a homogeneous system of linear equations C11x + C12y = 0 C21x + C2,y = 0 only has a non-zero solution for x and y when C11 C12 =0, C22 C21 obtain an expression for w. (d) Making use of the approximation 1q x² 2p for small x, determine the dispersion relation for the acoustic branch in the long-wavelength limit and thus find the group velocity of acoustic waves in the lattice. B. a U2n 2 || |

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1. A linear lattice with lattice constant a has a basis of two identical atoms of mass m where the
equilibrium spacing of the atoms within each unit cell is b (where b <5. The displacements of
the atoms from their equilibrium positions are given by u,U2, ---, Uzn-1,Uzn, Uzn+1, -.. The
harmonic forces between nearest-neighbour atoms are characterised by the alternating
interatomic force constants B, and B..
(a) Develop:
(i) The equation of motion for the 2nth atom in terms of forces exerted by the (2n - 1)th
and (2n + 1)*th atoms.
(u) The equation of motion for the (2n + 1)th atom in terms of forces exerted by the 2nth
and (2n + 2)th atoms.
(b) Using the equations of motion and assuming travelling wave solutions of the form
Un = Aet-kna) and Um = Bei(@t-kna-kb)
derive two simultaneous equations for A and B.
(c) Making use of the fact that a homogeneous system of linear equations
C11x + C2y = 0
C2,x + Cy = 0
only has a non-zero solution for x and y when
C12
=0.
C22
obtain an expression for w.
(d) Making use of the approximation
1q
2p
for small x, determine the dispersion relation for the acoustic branch in the long-wavelength
limit and thus find the group velocity of acoustic waves in the lattice.
B.
Transcribed Image Text:Please show all working. 1. A linear lattice with lattice constant a has a basis of two identical atoms of mass m where the equilibrium spacing of the atoms within each unit cell is b (where b <5. The displacements of the atoms from their equilibrium positions are given by u,U2, ---, Uzn-1,Uzn, Uzn+1, -.. The harmonic forces between nearest-neighbour atoms are characterised by the alternating interatomic force constants B, and B.. (a) Develop: (i) The equation of motion for the 2nth atom in terms of forces exerted by the (2n - 1)th and (2n + 1)*th atoms. (u) The equation of motion for the (2n + 1)th atom in terms of forces exerted by the 2nth and (2n + 2)th atoms. (b) Using the equations of motion and assuming travelling wave solutions of the form Un = Aet-kna) and Um = Bei(@t-kna-kb) derive two simultaneous equations for A and B. (c) Making use of the fact that a homogeneous system of linear equations C11x + C2y = 0 C2,x + Cy = 0 only has a non-zero solution for x and y when C12 =0. C22 obtain an expression for w. (d) Making use of the approximation 1q 2p for small x, determine the dispersion relation for the acoustic branch in the long-wavelength limit and thus find the group velocity of acoustic waves in the lattice. B.
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