Problem 2.5 A particle in the infinite square well has as its initial wave function an even mixture of the first two stationary states: ¥ (x, 0) = A [Y1(x)+ y2(x)]. (a) Normalize ¥ (x,0). (That is, find A. This is very easy, if you exploit the orthonor- mality of v1 and 2. Recall that, having normalized Y at t = 0, you can rest assured that it stays normalized–if you doubt this, check it explicitly after doing part (b).) (b) Find ¥(x, 1) and |4 (x, t)|². Express the latter as a sinusoidal function of time, as in Example 2.1. To simplify the result, let w = 7²h/2ma². (c) Compute (x). Notice that it oscillates in time. What is the angular frequency of the oscillation? What is the amplitude of the oscillation? (If your amplitude is greater than a/2, go directly to jail.) (d) Compute (p). (As Peter Lorre would say, “Do it ze kveek vay, Johnny!") (e) If you measured the energy of this particle, what values might you get, and what is the probability of getting each of them? Find the expectation value of H. How does it compare with Ej and E2?

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Problem 2.5 A particle in the infinite square well has as its initial wave function an even
mixture of the first two stationary states:
Y (x, 0) = A [Y1(x)+ ¥2(x)].
(a) Normalize ¥ (x, 0). (That is, find A. This is very easy, if you exploit the orthonor-
mality of y1 and ý2. Recall that, having normalized ¥ at t = 0, you can rest
assured that it stays normalized–if you doubt this, check it explicitly after doing
part (b).)
(b) Find ¥ (x, t) and |4 (x, t)|². Express the latter as a sinusoidal function of time, as
in Example 2.1. To simplify the result, let w = 7²h/2ma².
(c) Compute (x). Notice that it oscillates in time. What is the angular frequency of the
oscillation? What is the amplitude of the oscillation? (If your amplitude is greater
than a/2, go directly to jail.)
(d) Compute (p). (As Peter Lorre would say, “Do it ze kveek vay, Johnny!")
(e) If you measured the energy of this particle, what values might you get, and what is
the probability of getting each of them? Find the expectation value of H. How does
it compare with Ej and E2?
Transcribed Image Text:Problem 2.5 A particle in the infinite square well has as its initial wave function an even mixture of the first two stationary states: Y (x, 0) = A [Y1(x)+ ¥2(x)]. (a) Normalize ¥ (x, 0). (That is, find A. This is very easy, if you exploit the orthonor- mality of y1 and ý2. Recall that, having normalized ¥ at t = 0, you can rest assured that it stays normalized–if you doubt this, check it explicitly after doing part (b).) (b) Find ¥ (x, t) and |4 (x, t)|². Express the latter as a sinusoidal function of time, as in Example 2.1. To simplify the result, let w = 7²h/2ma². (c) Compute (x). Notice that it oscillates in time. What is the angular frequency of the oscillation? What is the amplitude of the oscillation? (If your amplitude is greater than a/2, go directly to jail.) (d) Compute (p). (As Peter Lorre would say, “Do it ze kveek vay, Johnny!") (e) If you measured the energy of this particle, what values might you get, and what is the probability of getting each of them? Find the expectation value of H. How does it compare with Ej and E2?
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