Question 1:
Using the explicit form for the leptonic tensor in eN elastic
scattering, verify the charge conservation
condition,
qμ Lμ ν
= qν Lμ ν
= 0.
Question 2:
(a)
Show that the Lorentz-invariant phase space, dLips(p',k'),
for unpolarized scattering can be written
in the laboratory (or target rest) frame as
dΩ d|k'| (|k'|/p'0)
δ (p'0 + |k'| - |k| - M)
/ (4π)2 .
(b)
Show further that this reduces to
dLips(p',k')
= (|k'|2/M |k|) dΩ
/ (4π)2 .
(c)
Finally, changing variables from dΩ to dQ2,
show that
d|Q2|
= 2 |k'|2 dcos(θ) .
[Note that the quantities in bold face, e.g. k or k',
denote 3-momentum vectors.]
Question 3:
In the "pion pole model" the induced pseudoscalar form factor of the
nucleon, GP(Q2), is given by
4M fπ gπNN(Q2)
/ (Q2 + mπ2),
where gπNN(Q2) is the
form factor at the pion-nucleon-nucleon vertex.
Using conservation of the axial vector current in the chiral limit,
derive the Goldberger-Treiman
relation,
M GA(Q2)
= fπ gπNN(Q2).
How well does it hold experimentally?