Plane waves in a box with periodic boundary conditions Consider plane waves &(r) = a exp(ik. r) in a d-dimensional cubic region of linear size L in each direction and “volume” V = Lª. There are p possible_wave polarizations. Assume that the waves satisfy "periodic boundary conditions": (r) = (r+ Lêj), j = 1, …‚d, where ê; is the unit vector along the j-th direction. (i) The boundary conditions restrict the possible values of the wavevector k. Show that those possible values can be written in the form k = (dk) Σ;=1 njêj, where nj, j = 1,...,d are integers, and calculate the quantity ok. (ii) Assume that there are p possible polarizations, and that the angular frequency grows linearly with the wavevector: w = ck. Compute the density of modes g(w) in the general case of d dimension and list g(w) for d = 1,2,3. For this, note that the volume of a sphere of radius R in d-dimension is 774/2 Vd-sphere = D Rd.
Plane waves in a box with periodic boundary conditions Consider plane waves &(r) = a exp(ik. r) in a d-dimensional cubic region of linear size L in each direction and “volume” V = Lª. There are p possible_wave polarizations. Assume that the waves satisfy "periodic boundary conditions": (r) = (r+ Lêj), j = 1, …‚d, where ê; is the unit vector along the j-th direction. (i) The boundary conditions restrict the possible values of the wavevector k. Show that those possible values can be written in the form k = (dk) Σ;=1 njêj, where nj, j = 1,...,d are integers, and calculate the quantity ok. (ii) Assume that there are p possible polarizations, and that the angular frequency grows linearly with the wavevector: w = ck. Compute the density of modes g(w) in the general case of d dimension and list g(w) for d = 1,2,3. For this, note that the volume of a sphere of radius R in d-dimension is 774/2 Vd-sphere = D Rd.
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