Chapter 1: Problem 4
Show that (a) \([A, B]=-[B, A],\) (b) \(\left[A^{m}, A^{n}\right]=0\) for all \(m, n,\) (c) \(\left[A^{2}, B\right]=A[A, B]+[A, B] A\) (d) \([A,[B, C]]+[B,[C, A]]+[C,[A, B]]=0\)
Chapter 1: Problem 4
Show that (a) \([A, B]=-[B, A],\) (b) \(\left[A^{m}, A^{n}\right]=0\) for all \(m, n,\) (c) \(\left[A^{2}, B\right]=A[A, B]+[A, B] A\) (d) \([A,[B, C]]+[B,[C, A]]+[C,[A, B]]=0\)
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Get started for freeEvaluate the commutators (a) \(\left[(1 / x), p_{x}\right]\) (b) \(\left[(1 / x), p_{x}^{2}\right]\) (c) \(\left[x p_{y}-y p_{x}, y p_{z}-z p_{y}\right]\) (d) \(\left[x^{2}\left(\partial^{2} / \partial y^{2}\right), y(\partial / \partial x)\right]\)
A particle in an infinite one-dimensional system was described by the wavefunction \(\psi(x)=\mathrm{Ne}^{-x^{2} / 2 r^{2}}\). Normalize this function. Calculate the probability of finding the particle in the range \(-\Gamma \leq x \leq \Gamma\). Hint. The integral encountered in the second part is the error function. It is available in mathematical software.
Confirm that the operators (a) \(T=-\left(\hbar^{2} / 2 m\right)\left(d^{2} / d x^{2}\right)\) and (b) \(l_{z}=(\hbar / \mathrm{i})(\mathrm{d} / \mathrm{d} \varphi)\) are Hermitian. Hint. Consider the integrals \(\int_{0}^{L} \psi_{a}^{*} T \psi_{b} \mathrm{d} x\) and \(\int_{0}^{2 \pi} \psi_{a}^{*} l_{z} \psi_{b} \mathrm{d} \varphi\) and integrate by parts.
Evaluate the commutator \(\left[l_{y}\left[l_{y}, l_{z}\right]\right]\) given that \(\left[l_{x}, l_{y}\right]=i \hbar l,\left[l_{y}, l_{z}\right]=i \hbar l_{x},\) and \(\left[l_{z}, l_{x}\right]=i \hbar l_{y}\)
Use the momentum representation and a general function \(f\left(p_{x}\right)\) of the linear momentum to confirm that the position and momentum operators in this representation do not commute, and find the value of their commutator.
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