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.
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Get started for freeQuestion: Consider a quantum system with just three linearly independent states. Suppose the Hamiltonian, in matrix form, is
Whereis a constant, andis some small number.
(a) Write down the eigenvectors and eigenvalues of the unperturbed Hamiltonian.
(b) Solve for the exact eigen values of H. Expand each of them as a power series in, up to second order.
(c) Use first- and second-order non degenerate perturbation theory to find the approximate eigen value for the state that grows out of the non-degenerate eigenvector of. Compare the exact result, from (a).
(d) Use degenerate perturbation theory to find the first-order correction to the two initially degenerate eigen values. Compare the exact results.
Van der Waals interaction. Consider two atoms a distanceapart. Because they are electrically neutral you might suppose there would be no force between them, but if they are polarizable there is in fact a weak attraction. To model this system, picture each atom as an electron (mass m , charge -e ) attached by a spring (spring constant k ) to the nucleus (charge +e ), as in Figure. We'll assume the nuclei are heavy, and essentially motionless. The Hamiltonian for the unperturbed system is
The Coulomb interaction between the atoms is
[6.97]
(a) Explain Equation6.97. Assuming that localid="1658203563220" and are both much less than, show that
localid="1658203513972" [6.98]
(b) Show that the total Hamiltonian (Equationplus Equation) separates into two harmonic oscillator Hamiltonians:
[6.99]
under the change of variables
Which entails [6.100]
(c) The ground state energy for this Hamiltonian is evidently
Where [6.101]
Without the Coulomb interaction it would have been , where . Assuming that, show that
[6.102]
Conclusion: There is an attractive potential between the atoms, proportional to the inverse sixth power of their separation. This is the van der Waals interaction between two neutral atoms.
(d) Now do the same calculation using second-order perturbation theory. Hint: The unperturbed states are of the form , where is a one-particle oscillator wave function with mass mand spring constant is the second-order correction to the ground state energy, for the perturbation in Equation 6.98 (notice that the first-order correction is zero).
Show thatis Hermitian, butis not, for hydrogen states with. Hint: For such statesis independent ofand, so
localid="1656070791118"
(Equation 4.13). Using integration by parts, show that
localid="1656069411605"
Check that the boundary term vanishes for, which goes like
near the origin. Now do the same for, and show that the boundary terms do not vanish. In fact:
Question: Evaluate the following commutators :
a)
b)
c)role="math" localid="1658226147021"
d)
e)
f)
Hint: L and S satisfy the fundamental commutation relations for angular momentum (Equations 4.99 and 4.134 ), but they commute with each other.
Question: The most prominent feature of the hydrogen spectrum in the visible region is the red Balmer line, coming from the transition n = 3to n = 2. First of all, determine the wavelength and frequency of this line according to the Bohr Theory. Fine structure splits this line into several closely spaced lines; the question is: How many, and what is their spacing? Hint: First determine how many sublevels the n = 2level splits into, and find for each of these, in eV. Then do the same for n = 3. Draw an energy level diagram showing all possible transitions from n = 3to n = 2. The energy released (in the form of a photon) is role="math" localid="1658311193797" , the first part being common to all of them, and the (due to fine structure) varying from one transition to the next. Find (in eV) for each transition. Finally, convert to photon frequency, and determine the spacing between adjacent spectral lines (in Hz- -not the frequency interval between each line and the unperturbed line (which is, of course, unobservable), but the frequency interval between each line and the next one. Your final answer should take the form: "The red Balmer line splits into (???)lines. In order of increasing frequency, they come from the transitionsto (1) j =(???),toj =(???) ,(2) j =(???) to j =(???)……. The frequency spacing between line (1)and line (2)is (???) Hz, the spacing between line (2)and (3) line (???) Hzis……..”
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