2025-05-30
Solutions to Principles of Quantum Mechanics
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目录

Chapter 13 The Hydrogen Atom
13.1 The Eigenvalue Problem
13.2 The Degeneracy of the Hydrogen Spectrum
13.3 Numerical Estimates and Comparison with Experiment
13.4 Multielectron Atoms and the Periodic Table

Chapter 13 The Hydrogen Atom

13.1 The Eigenvalue Problem

Exercise 13.1.1 Derive Eqs. (13.1.11) and (13.1.14) starting from Eqs. (13.1.8)-(13.1.10).

Exercise 13.1.2 Derive the degeneracy formula, Eq. (13.1.18).

Exercise 13.1.3 Starting from the recursion relation, obtain ψ210\psi_{210} (normalized).

Exercise 13.1.4 Recall from the last chapter [Eq. (12.6.19)] that as rr \rightarrow \infty, UE(r)me2/κ2eκrU_E \sim(r)^{m e^2 / \kappa \hbar^2} \mathrm{e}^{-\kappa r} in a Coulomb potential V=e2/rV=-\mathrm{e}^2 / r [κ=(2mW/2)1/2]\left[\kappa=\left(2 m W / \hbar^2\right)^{1 / 2}\right]. Show that this agrees with Eq. (13.1.26).

Exercise 13.1.5 (Virial Theorem) Since n,l,m|n, l, m\rangle is a stationary state, Ω˙=0\langle\dot{\mathbf{\Omega}}\rangle=0 for any Ω\mathbf{\Omega}.\ Consider Ω=RP\mathbf{\Omega}=\mathbf{R} \cdot \mathbf{P} and use Ehrenfest's theorem to show that T=(1/2)V\langle T\rangle=(-1 / 2)\langle V\rangle in the state n,l,m|n, l, m\rangle.

13.2 The Degeneracy of the Hydrogen Spectrum

Exercise 13.2.1 Let us see why the conservation of the Runge-Lenz vector n\mathbf{n} implies closed orbits.

(1) Express n\mathbf{n} in terms of r\mathbf{r} and p\mathbf{p} alone (get rid of 1\mathbf{1}).

(2) Since the particle is bound, it cannot escape to infinity. So, as we follow it from some arbitrary time onward, it must reach a point rmax\mathbf{r}_{\max} where its distance from the origin stops growing. Show that

n=rmax(2E+e2rmax)\mathbf{n}=\mathbf{r}_{\max}\left(2 E+\frac{\mathrm{e}^2}{r_{\max}}\right)

13.3 Numerical Estimates and Comparison with Experiment

Exercise 13.3.1 The pion has a range of 1 Fermi=105A˚1~\mathrm{Fermi}=10^{-5} \text{\AA} as a mediator of nuclear force. Estimate its rest energy.

Exercise 13.3.2 Estimate the de Broglie wavelength of an electron of kinetic energy 200 eV200~\mathrm{eV}. (Recall λ=2π/p\lambda=2 \pi \hbar / p.)

13.4 Multielectron Atoms and the Periodic Table

Exercise 13.4.1 Show that if we ignore interelectron interactions, the energy levels of a multielectron atom go as Z2Z^2. Since the Coulomb potential is Ze/rZ e / r, why is the energy Z2\propto Z^2?

Exercise 13.4.2 Compare (roughly) the sizes of the uranium atom and the hydrogen atom. Assume levels fill in the order of increasing nn, and that the nonrelativistic description holds. Ignore interelectron effects.

Exercise 13.4.3 Visible light has a wavelength of approximately 5000A˚5000 \text{\AA}. Which of the series-Lyman, Balmer, Paschen-do you think was discovered first?

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