2.1 Consider a linear chain in which alternate ions have masses M₁ and M2, and only neares neighbors interact. (i) K K a/2 a K ww w² (k)= M₁ K Show that the dispersion relation for normal modes is: K wow M₂ 2 1 1 1 1 4 ka = K < (+) ± √(-+)²-, M₂ sin (22) +K += M₁ M₂ M₂ M₁M₂ Where, K is the spring constant, and a, is the size of the unit cell (so the spacing between atoms is a/2). Derive an expression for the group velocity vg as a function of k. (iii) Use the results of part (ii), to evaluate vg for k at the Brillouin Zone boundary.[k = + and briefly discuss the physical significance of this Brillouin Zone boundary group
2.1 Consider a linear chain in which alternate ions have masses M₁ and M2, and only neares neighbors interact. (i) K K a/2 a K ww w² (k)= M₁ K Show that the dispersion relation for normal modes is: K wow M₂ 2 1 1 1 1 4 ka = K < (+) ± √(-+)²-, M₂ sin (22) +K += M₁ M₂ M₂ M₁M₂ Where, K is the spring constant, and a, is the size of the unit cell (so the spacing between atoms is a/2). Derive an expression for the group velocity vg as a function of k. (iii) Use the results of part (ii), to evaluate vg for k at the Brillouin Zone boundary.[k = + and briefly discuss the physical significance of this Brillouin Zone boundary group
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