Elong-14-05-09

Recreating F&S Azz

Using the Frankfurt and Strikman equation 7.3,

<math>A_{zz} = R(p_s) = \frac{3(k_t^2/2-k_z^2)}{k^2}\frac{u(k)w(k)\sqrt{2}+\frac{1}{2}w^2(k)}{u^2(k)+w^2(k)}</math>

I'm trying to recreated their Figure 7.5. I don't entirely understand what <math>k_t</math>, <math>k_z</math>, and <math>k</math> are, but if the ratio out front comes out to -3, I can recreate the D(e,e'p) at 180 degrees plot:

Repeating this same process for all of the wavefunctions that I received from Donal, making sure that the low-k part of the D-state wavefunction is positive as is their convention in Figure 7.1, we see

1981 Report

In Frankfurt and Strikman's 1981 report, they go into a bit more detail of how to make the cross section ratios. In particular, on page 258 there is an equation (3.19 and 3.20) for the ratio of cross sections with respect to k,

<math>r(\xi,k)=1+\left(\frac{3(k\xi)^2}{k^2}-1\right)\frac{u(k)w(k)\sqrt{2}+w^2(k)/2}{u^2(k)+w^2(k)}</math>

where <math>\xi</math> is the D-polarization in the D-rest frame, with <math>\xi=(1,\pm i, 0)/\sqrt{2}</math> for <math>\lambda_D=\pm 1</math>, and <math>\xi=(0,0, 1)</math> for <math>\lambda_D=0</math>. Assuming that <math>k\xi=\vec{k}\cdot\xi</math>, this leads to three possible ratios:

<math>r(\pm 1,k)=1+\left(\frac{3k_1^2-3k_2^2}{2\vec{k}\cdot\vec{k}}-1\right)\frac{u(k)w(k)\sqrt{2}+w^2(k)/2}{u^2(k)+w^2(k)}</math>