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Problem set 4 from physics 471, fall 2004. The problems involve normalization and expression of wave functions in terms of energy eigenstates for particles in infinite potential wells. The potential wells have different shapes and boundary conditions. Students are asked to find the wave functions, expectation values, and allowed bound state energies.
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Physics 471 Problem Set 4 Fall 2004
Ψ(x, 0) = A sin^3 (πx/a).
(a) Normalize Ψ(x, 0). (b) Express Ψ(x, 0) in terms of the energy eigenstates
ψn(x) =
√ 2 a
sin(nπx/a) , n = 1, 2 , 3 , · · · ,
as Ψ(x, 0) =
∑ n
Cnψn(x).
Hint: There are only two terms in the expansion and they can be found by expressing sin^3 (x) as a combination of sin(x) and sin(3x) using
e 3 ix^ = (cos(x) + i sin(x))^3.
(c) Obtain Ψ(x, t) and find 〈x〉 as a function of time.
∞ for x = 0 0 for 0 < x ≤ a V 0 for x ≥ a
is ψ(x) =
{ A sin(kx) for 0 < x ≤ a Ce−κx^ for x ≥ a with k =
√ 2 mE ¯h^2
κ =
√ 2 m(V 0 − E) ¯h^2
(a) Apply the boundary conditions at x = a and obtain the transcendental equation which determines the bound state energies E. (b) If (^) √ 2 mV 0 a^2 ¯h^2
= 3π ,
determine the allowed bound state energies.