Issued Wed, Feb 18 Due Wed, Feb 25
Required reading for this week: Gas. Ch. 16.
(You might want to look at Griffith's chapter on perturbation theory, too.)
1) Gas 15-5 (Write your answers in "spectroscopic notation", a la Gas. 15-52)
Hint: I get exactly 6 possible answers, but only 4 of those are possible if the pion has negative parity.
2) The Hamiltonian of a spin system is given by
. (Neglect orbital angular momentum, L=0).
Find the eigenvalues and eigenfunctions of the system if the two particles are identical spin 1 particles. (Don't forget the Pauli principle, which says identical bosons must be in a totally symmetric state)
(This is sort of like Gas 15-7, one of the "optional problems" from last week)
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We may or may not get far enough in lecture to fully derive this, but for the rest of this homework all you need is Gas 16-7 and 16-12: the energies of a system with are , where
= the energy eigenvalues of , (with corresponding e-fn ,)
and the correction term is .
3) Last semester (HW 7) you solved (exactly) for the energies and eigenvectors of a particle in a square well with a delta function in the middle:
Now you will treat this problem as a perturbation: will be the usual square well (from -a to +a), and the perturbation is then just
Find the energies , using first order perturbation theory.
(Why are the energies unperturbed for even n?) (over ->)
4) For a harmonic oscillator, , and we know , with . Now suppose k is slightly increased, i.e. .
(Imagine the spring has been slightly cooled, to make it "stiffer".)
a) Find the exact energies of the new system. (This is a "quicky", just write it down!) Expand your answer as a power series in .
b) Now calculate the energies using first order perturbation theory, and compare with part a. (What exactly is here?)
(Note: no integrals need to be calculated for this problem, if you remember the virial theorem, <K.E.> = <V> for a harmonic oscillator)
5) Gas. 16-2, but just do the n=1, l=0 state (i.e. ground state) only.
Hint: If
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