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Physics LibreTexts

7.P: Exercises

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  1. Calculate the energy-shift in the ground state of the one-dimensional harmonic oscillator when the perturbation $ V = \lambda\,x^4
$ is added to $ H = \frac{p_x^{\,2}}{2\,m} + \frac{1}{2}\,m\,\omega^2\,x^2.
$ The properly normalized ground-state wavefunction is $ \psi(x) = \left(\frac{m\,\omega}{\pi\,\hbar}\right)^{1/4}\,\exp\left(-\frac{m\,\omega^2\,x^2}{2\,\hbar}\right).
$
  2. Calculate the energy-shifts due to the first-order Stark effect in the n=3 state of a hydrogen atom. You do not need to perform all of the integrals, but you should construct the correct linear combinations of states.
  3. The Hamiltonian of the valence electron in a hydrogen-like atom can be written $ H = \frac{p^2}{2\,m_e} + V(r) - \frac{p^4}{8\,m_e^{\,3}\,c^2}.
$ Here, the final term on the right-hand side is the first-order correction due to the electron's relativistic mass increase. Treating this term as a small perturbation, deduce that it causes an energy-shift in the energy eigenstate characterized by the standard quantum numbers n , l , m of $ {\mit\Delta}E_{nlm} = -\frac{1}{2\,m_e\,c^2}\left(E_n^{\,2} - 2\,E_n\,\langle V\rangle + \langle V^{\,2}\rangle\right),
$ where En is the unperturbed energy, and α the fine structure constant.
  4. Consider an energy eigenstate of the hydrogen atom characterized by the standard quantum numbers n , l , and m . Show that if the energy-shift due to spin-orbit coupling (see Section 7.7) is added to that due to the electron's relativistic mass increase (see previous exercise) then the net fine structure energy-shift can be written $ {\mit\Delta} E_{nlm} = \frac{\alpha^2\,E_n}{n^2}\left(\frac{n}{j+1/2}-\frac{3}{4}\right).
$ Here, En is the unperturbed energy, α the fine structure constant, and j=l±1/2 the quantum number associated with the magnitude of the sum of the electron's orbital and spin angular momenta. You will need to use the following standard results for a hydrogen atom:
  5. a0r =1n2, a20r2 =1(l+1/2)n3, a30r3 =1l(l+1/2)(l+1)n3. Here, a0 is the Bohr radius. Assuming that the above formula for the energy shift is valid for l=0 (which it is), show that fine structure causes the energy of the (2p)3/2 states of a hydrogen atom to exceed those of the (2p)1/2 and (2s)1/2 states by 4.5×105eV .

Contributors

  • Richard Fitzpatrick (Professor of Physics, The University of Texas at Austin)


This page titled 7.P: Exercises is shared under a not declared license and was authored, remixed, and/or curated by Richard Fitzpatrick.

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