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6.P: Exercises

  • Page ID
    1215
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    1. Calculate the Clebsch-Gordon coefficients for adding spin one-half to spin one.
    2. Calculate the Clebsch-Gordon coefficients for adding spin one to spin one.
    3. An electron in a hydrogen atom occupies the combined spin and position state whose wavefunction is
      \[\psi = R_{2\,1}(r)\,\left[\sqrt{1/3}\,Y_{1\,0}(\theta,\varphi)\,\chi_+ + \sqrt{2/3}\,Y_{1\,1}(\theta,\varphi)\,\chi_-\right].\]
      1. What values would a measurement of \( L^2\) yield, and with what probabilities?
      2. Same for \( S^2\) .
      3. Same for \( J^{\,2}\) .
      4. Same for \( r\) , \( \varphi\) ?
      5. What is the probability density for finding the electron in the spin up state (with respect to the \( r\) ?
    4. In a low energy neutron-proton system (with zero orbital angular momentum) the potential energy is given by
      $ V({\bf x}) = V_1(r) + V_2(r)\left[3\,\frac{(\mbox{\boldmath $\sig...
...\right] + V_3(r)\,\mbox{\boldmath $\sigma$}_n\cdot\mbox{\boldmath $\sigma$}_p,
$
      where \( \sigma\) \( \sigma\) \( V({\bf x})\) with respect to the overall spin state.]
    5. Consider two electrons in a spin singlet (i.e., spin zero) state.
      1. If a measurement of the spin of one of the electrons shows that it is in the state with \( z\) -component of the spin of the other electron yields \( S_y=\hbar/2\) , what is the probability that a measurement of the \( S_x=-\hbar/2\) ?
      2. Finally, if electron 1 is in a spin state described by $ \cos\alpha_1\,\chi_+
+ \sin\alpha_1\,{\rm e}^{\,{\rm i}\,\beta_1}\,\chi_-$ , and electron 2 is in a spin state described by $ \cos\alpha_2\,\chi_+
+ \sin\alpha_2\,{\rm e}^{\,{\rm i}\,\beta_2}\,\chi_-$ , what is the probability that the two-electron spin state is a triplet (i.e., spin one) state?

    Contributors

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

      \( \newcommand {\ltapp} {\stackrel {_{\normalsize<}}{_{\normalsize \sim}}}\) \(\newcommand {\gtapp} {\stackrel {_{\normalsize>}}{_{\normalsize \sim}}}\) \(\newcommand {\btau}{\mbox{\boldmath$\tau$}}\) \(\newcommand {\bmu}{\mbox{\boldmath$\mu$}}\) \(\newcommand {\bsigma}{\mbox{\boldmath$\sigma$}}\) \(\newcommand {\bOmega}{\mbox{\boldmath$\Omega$}}\) \(\newcommand {\bomega}{\mbox{\boldmath$\omega$}}\) \(\newcommand {\bepsilon}{\mbox{\boldmath$\epsilon$}}\)

    This page titled 6.P: Exercises is shared under a not declared license and was authored, remixed, and/or curated by Richard Fitzpatrick.

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