Consider a particle of mass m in the one-dimensional infinite square well potential V(x) = +∞ {x < - L and x > L} V(x) = 0 {−L
Consider a particle of mass m in the one-dimensional infinite square well potential V(x) = +∞ {x < - L and x > L} V(x) = 0 {−L
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![3. Consider a particle of mass m in the one-dimensional infinite square well potential
V(x) = +∞ {x < - L and x > L}
V(x) = 0 {-L<x<L}
(a) Write down all the normalized stationary state wavefunctions y(x) in terms of L and also the
corresponding energies (you may either rewrite those already shown in Griffiths, or derive
them directly by solving the Schrodinger equation).
(b) For the odd wavefunctions, ¥(x) = - 4(-x), calculate the spatial uncertainty Ax = Ox and the
momentum uncertainty Ap = op and then verify that the uncertainty principle is satisfied.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F62a79166-ba2c-43d7-9fa1-94c5c5be2063%2F641ac829-47d8-43dd-b274-a5261e313448%2Fpcxwc7b_processed.png&w=3840&q=75)
Transcribed Image Text:3. Consider a particle of mass m in the one-dimensional infinite square well potential
V(x) = +∞ {x < - L and x > L}
V(x) = 0 {-L<x<L}
(a) Write down all the normalized stationary state wavefunctions y(x) in terms of L and also the
corresponding energies (you may either rewrite those already shown in Griffiths, or derive
them directly by solving the Schrodinger equation).
(b) For the odd wavefunctions, ¥(x) = - 4(-x), calculate the spatial uncertainty Ax = Ox and the
momentum uncertainty Ap = op and then verify that the uncertainty principle is satisfied.
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