Elong-14-05-15b

Non-Relativistic Case

Ratios and Definitions

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,p)=1+\left(\frac{3(p\xi)^2}{p^2}-1\right)\frac{u(p)w(p)\sqrt{2}+w^2(p)/2}{u^2(p)+w^2(p)}</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>p\xi=\vec{p}\cdot\xi</math>, this leads to three possible ratios:

<math>r(\pm 1,p)=1+\left(\frac{3p_1^2-3p_2^2}{2\vec{p}\cdot\vec{p}}-1\right)\frac{u(p)w(p)\sqrt{2}+w^2(p)/2}{u^2(p)+w^2(p)}</math>

<math>r(0,p)=1+\left(\frac{3p_3^2}{\vec{p}\cdot\vec{p}}-1\right)\frac{u(p)w(p)\sqrt{2}+w^2(p)/2}{u^2(p)+w^2(p)}</math>.

If I am understanding their kinematic variables correctly, then the virtual-photon points along the <math>\hat{z}</math> axis, so in the case of a nucleon being knocked-out at 180deg, <math>p_1=0, p_2=0, p_3=|\vec{p}|</math>. This leads to, in the case of <math>r(0,p)</math> for their Fig. 3.9a,

<math>r(0,p)=1+2\frac{u(p)w(p)\sqrt{2}+w^2(p)/2}{u^2(p)+w^2(p)}</math>,

which can be recreated using the current wavefunctions.

This would make their Fig. 7.5 from their 1988 report simply <math>A_{zz} = r(\pm 1,p)-r(0,p)</math> for D(e,e'p) with p at 180deg, which can also be reproduced.

Angular Dependence

One of the on-going issues I've been having is defining the kinematic directions the same as F&S. Following the convention with <math>z</math> being along the direction of the virtual photon, in the non-relativistic case,

With the light-cone variables being used, I believe that <math>p_1 = p_{\perp} = \sqrt{p_x^2+p_y^2},~~p_2=0,~~p_3=p_z</math>. This lets me recreate their angular distribution in the 1988 report's Fig. 7.6

Note that my assumption for the section above, with the knocked-out proton going at 180deg, as <math>\sin(\pi)=0 \rightarrow p_1=p_2=0, ~\cos(\pi)=1 \rightarrow p_3=p</math> would hold.

Azz for D(e,e')

In order to find the inclusive D(e,e') Azz, we would simply integrate over all possible angles of the knocked-out nucleon. This gives

Relativistic Case

Light Cone Definitions

Using Frankfurt and Strikman's 1981 report, we can repeat the process above for the relativistic case,

<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>

<math>r(0,k)=1+\left(\frac{3k_3^2}{\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>.

To do this, we define the following light-cone variables:

<math>\alpha_N = \frac{2(E_p-p_3)}{m_D}</math>

<math>k_{\perp} = p_{\perp}</math>

<math> k^2 = \frac{m_N^2+p_{\perp}^2}{\alpha_N (2-\alpha_N)} - m_N^2</math>

<math> k_3 = \sqrt{k^2 - k_{\perp}^2}</math>

Angular Comparison with Non-Relativistic

Now, I can re-run my code and attempt to recreate their angular-dependent ratios in the relativistic and non-relativistic case.