Chapter 6: Q25P (page 283)
Work out the matrix elements of construct the W matrix given in the text, for n = 2.
Chapter 6: Q25P (page 283)
Work out the matrix elements of construct the W matrix given in the text, for n = 2.
All the tools & learning materials you need for study success - in one app.
Get started for freeThe Feynman-Hellmann theorem (Problem 6.32) can be used to determine the expectation values ofandfor hydrogen.The effective Hamiltonian for the radial wave functions is (Equation4.53)
And the eigenvalues (expressed in terms ofare (Equation 4.70)
(a) Use in the Feynman-Hellmann theorem to obtain . Check your result against Equation 6.55.
(b) Use to obtain . Check your answer with Equation6.56.
Suppose the Hamiltonian H, for a particular quantum system, is a function of some parameter let and be the eigen values and
Eigen functions of. The Feynman-Hellmann theoremstates that
(Assuming either that is nondegenerate, or-if degenerate-that the 's are the "good" linear combinations of the degenerate Eigen functions).
(a) Prove the Feynman-Hellmann theorem. Hint: Use Equation 6.9.
(b) Apply it to the one-dimensional harmonic oscillator,(i)using (this yields a formula for the expectation value of V), (II)using (this yields (T)),and (iii)using (this yields a relation between (T)and (V)). Compare your answers to Problem 2.12, and the virial theorem predictions (Problem 3.31).
For the harmonic oscillator, the allowed energies arewhererole="math" localid="1656044150836" is the classical frequency. Now suppose the spring constant increases slightly:(Perhaps we cool the spring, so it becomes less flexible.)
(a) Find the exact new energies (trivial, in this case). Expand your formula as a power series in, up to second order.
(b) Now calculate the first-order perturbation in the energy, using Equation 6.9. What ishere? Compare your result with part (a).
Hint: It is not necessary - in fact, it is not permitted - to calculate a single integral in doing this problem.
Suppose we perturb the infinite cubical well (Equation 6.30) by putting a delta function “bump” at the point
Find the first-order corrections to the energy of the ground state and the (triply degenerate) first excited states.
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?
What do you think about this solution?
We value your feedback to improve our textbook solutions.