Chapter 6: Q22P (page 280)
Starting with Equation 6.80, and using Equations 6.57, 6.61, 6.64, and 6.81, derive Equation 6.82.
Short Answer
The equation is derived, .
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Chapter 6: Q22P (page 280)
Starting with Equation 6.80, and using Equations 6.57, 6.61, 6.64, and 6.81, derive Equation 6.82.
The equation is derived, .
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Consider the isotropic three-dimensional harmonic oscillator (Problem 4.38). Discuss the effect (in first order) of the perturbation
(for some constant ) on
(a) the ground state
(b) the (triply degenerate) first excited state. Hint: Use the answers to Problems 2.12and 3.33
Use Equation 6.59 to estimate the internal field in hydrogen, and characterize quantitatively a "strong" and "weak" Zeeman field.
Suppose we perturb the infinite cubical well (Equation 6.30) by putting a delta function 鈥渂ump鈥 at the point
Find the first-order corrections to the energy of the ground state and the (triply degenerate) first excited states.
Calculate the wavelength, in centimeters, of the photon emitted under a hyperfine transition in the ground state (n=1) of deuterium. Deuterium is "heavy" hydrogen, with an extra neutron in the nucleus; the proton and neutron bind together to form a deuteron, with spin 1 and magnetic moment
he deuteron g-factor is 1.71.
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,.
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