Chapter 6: Q12P (page 270)
Question: Use the virial theorem (Problem 4.40) to prove Equation 6.55.
Short Answer
It is proved that .
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Chapter 6: Q12P (page 270)
Question: Use the virial theorem (Problem 4.40) to prove Equation 6.55.
It is proved that .
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Suppose we put a delta-function bump in the center of the infinite square well:
whereis a constant.
(a) Find the first-order correction to the allowed energies. Explain why the energies are not perturbed for even.
(b) Find the first three nonzero terms in the expansion (Equation 6.13) of the correction to the ground state,.
Starting with Equation 6.80, and using Equations 6.57, 6.61, 6.64, and 6.81, derive Equation 6.82.
By appropriate modification of the hydrogen formula, determine the hyperfine splitting in the ground state of
(a) muonic hydrogen (in which a muon-same charge and g-factor as the electron, but 207times the mass-substitutes for the electron),
(b) positronium (in which a positron-same mass and g-factor as the electron, but opposite charge-substitutes for the proton), and
(c) muonium (in which an anti-muon-same mass and g-factor as a muon, but opposite charge-substitutes for the proton). Hint: Don't forget to use the reduced mass (Problem 5.1) in calculating the "Bohr radius" of these exotic "atoms." Incidentally, the answer you get for positronium is quite far from the experimental value; the large discrepancy is due to pair annihilation , which contributes an extra localid="1656057412048" and does not occur (of course) in ordinary hydrogen, muonic hydrogen, or muoniun.
If I=0, then j=s,, and the "good" states are the same for weak and strong fields. Determine(from Equation) and the fine structure energies (Equation 6.67), and write down the general result for the I=O Zeeman Effect - regardless of the strength of the field. Show that the strong field formula (Equation 6.82) reproduces this result, provided that we interpret the indeterminate term in square brackets as.
Question: Sometimes it is possible to solve Equation 6.10 directly, without having to expand in terms of the unperturbed wave functions (Equation 6.11). Here are two particularly nice examples.
(a) Stark effect in the ground state of hydrogen.
(i) Find the first-order correction to the ground state of hydrogen in the presence of a uniform external electric field (the Stark effect-see Problem 6.36). Hint: Try a solution of the form
your problem is to find the constants , and C that solve Equation 6.10.
(ii) Use Equation to determine the second-order correction to the ground state energy (the first-order correction is zero, as you found in Problem 6.36(a)). Answer: .
(b) If the proton had an electric dipole moment p the potential energy of the electron in hydrogen would be perturbed in the amount
(i) Solve Equation 6.10 for the first-order correction to the ground state wave function.
(ii) Show that the total electric dipole moment of the atom is (surprisingly) zero, to this order.
(iii) Use Equation 6.14 to determine the second-order correction to the ground state energy. What is the first-order correction?
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