Question 1:
Explain why the lifetime for the decay of positronium (bound state
of e+ e-) into photons is much
larger for the spin-triplet state than for the spin-singlet state,
τ(3S1) >> τ(1S0).
[Hint: recall that the eigenvalues of C for a
fermion-antifermion system are (-1)L+S, and consider
the possible spin and orbital angular momenta
of the initial e+ e-
and final multi-photon states.]
Question 2:
(a)
Show that for two identical particles with isospin
I(1)=1/2 and I(2)=1/2,
the eigenvalues of the
product
I(1) . I(2)
are -3/4 for the iso-singlet combination,
and +1/4 for the iso-triplet combination.
(b)
If I = (I1, I2, I3)
is the nucleon isospin operator, we can define isospin raising
and lowering
operators by
I+ = I1 + i I2 and
I- = I1 - i I2,
respectively, where Ii satisfy
[Ii, Ij]
= i εijkIk.
An explicit realization of these is by the Pauli matrices,
Ii = τi/2.
If | p > and | n > are states of
the nucleon with 3rd component of isospin
I3 = +1/2 and -1/2, respectively, show that
I+ | n > = | p > and
I- | p > = | n >, but
I+ | p > = 0 and
I- | n > = 0.
Question 3:
The G-parity of a state is given by
G = (-1)I C,
where I is the total isospin of the multiplet,
and C is the charge-conjugation
number of the neutral member of the multiplet.
(a)
Derive the G-parity of the following states:
π, ρ, ω, η, p .
(b)
Discuss why the ρ meson decays to π π,
while the ω meson decays to π π π.