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A linear diatomic lattice of lattice constant a with masses M and m (M > m) are coupled by a force constant C. The dispersion relation is given by $${\omega ^2} = C\left( {\frac{{M + m}}{{Mm}}} \right) \pm {\left[ {{C^2}{{\left( {\frac{{m + m}}{{Mm}}} \right)}^2} - \frac{{4{C^2}}}{{Mm}}{{\sin }^2}\frac{{ka}}{2}} \right]^{\frac{1}{2}}}$$
Which one of the following statements is incorrect?

A. The atoms vibrating in transverse mode correspond to the optical branch

B. The maximum frequency of the acoustic branch depends on the mass of the Iighter atom m

C. The dispersion of frequency in the optical branch is smaller than that in the acoustic branch

D. No normal modes exist in the acoustic branch for any frequency greater than the maximum frequency at $$k = \frac{\pi }{a}$$

Answer: Option C


This Question Belongs to Engineering Physics >> Solid State Physics

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Related Questions on Solid State Physics

In a cubic crystal, atoms of mass M1 lie on one set of planes and atoms of mass M2 lie on planes interleaved between those of the first set. If C is the forte constant between nearest neighbour planes, the frequency of lattice vibrations for the optical phonon branch with wave vector k = 0 is

A. $$\sqrt {2C\left( {\frac{1}{{{M_1}}} + \frac{1}{{{M_2}}}} \right)} $$

B. $$\sqrt {C\left( {\frac{1}{{2{M_1}}} + \frac{1}{{{M_2}}}} \right)} $$

C. $$\sqrt {C\left( {\frac{1}{{{M_1}}} + \frac{1}{{2{M_2}}}} \right)} $$

D. zero