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Transcript
Quantum Mechanics 2, Autumn 2011 CMI
Problem set 5
Due by beginning of class on Monday September 19, 2011
Addition of angular momenta, rotation of spinors, Identical particles
1. Find the 2 × 2 matrix representing a counter-clockwise rotation (by angle φ about the n̂ direction), of the spin wavefunction of a spin- 12 particle. Express the answer as a linear combination
of the identity and Pauli matrices.
2. Show that the exchange operator acting on the Hilbert space of two identical particles is hermitian.
3. Obtain a matrix representation of the Clebsch-Gordan coefficients for the transformation from
uncoupled to coupled basis of a system of two spin-half particles. Show that the matrix is
unitary. Specify the uncoupled and coupled basis vectors and their orderings.
4. Suppose J~ = ~L + S~ is the sum of orbital and spin angular momentum of an electron (say in a
hydrogenic atom). Does ~L · S~ commute with each of J 2 , Jz , L2 and S 2 ?
5. Find the matrix elements of the spin-orbit interaction between coupled basis states
h j m j l s | f (r)~L · S~ | j0 m j 0 l0 s0 i
where f (r) is a function of the radial coordinate r =
p
(1)
x2 + y2 + z2 alone.
6. Consider three identical particles each of which has a translational degree of freedom ( x) and
a color degree of freedom (α). There are three values that color can take α = 1, 2, 3 while
there are infinitely many values that location x can take. The system of three particles is in a
factorized state constructed from a single one-particle orbital φ(x)
ψ(x1 , α1 ; x2 , α2 ; x3 , α3 ) = Aα1 α2 α3 φ(x1 )φ(x2 )φ(x3 )
(2)
Is this a system of bosons or fermions? Justify your answer.
7. Find the constant A so that the total wave function is normalized to one, assuming that the one
particle wave function has norm ||φ|| = 1.
1