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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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+ 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 = (8k) Σj-1¹jêj, where nj, j = 1,…‚d are
integers, and calculate the quantity Sk.
(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
Vd-sphere
=
77d/2
T(1+d/2)
Rd,
where I() is Euler's gamma function.
(iii) Apply your result to the case of electromagnetic waves in a 3D cavity of volume V.
Transcribed Image Text: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+ 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 = (8k) Σj-1¹jêj, where nj, j = 1,…‚d are integers, and calculate the quantity Sk. (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 Vd-sphere = 77d/2 T(1+d/2) Rd, where I() is Euler's gamma function. (iii) Apply your result to the case of electromagnetic waves in a 3D cavity of volume V.
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