1 | %\subsection{Angular distributions \editor{Johannes Peter}} |
---|
2 | |
---|
3 | Angular distributions for final states other than |
---|
4 | nucleon elastic scattering are |
---|
5 | calculated analytically, derived from the collision term of the |
---|
6 | in-medium relativistic Boltzmann-Uehling-Uhlenbeck equation, |
---|
7 | absed on the nucleon nucleon elastic scattering cross-sections: |
---|
8 | |
---|
9 | $$ |
---|
10 | \sigma_{NN\rightarrow NN}(s,t) = |
---|
11 | {1\over(2\pi)^2s}\left(D(s,t)+E(s,t) + (inverted t,u)\right) |
---|
12 | $$ |
---|
13 | |
---|
14 | Here $s$, $t$, $u$ are the Mandelstamm variables, |
---|
15 | $D(s,t)$ is the direct term, and $E(s,t)$ is the exchange |
---|
16 | term, with |
---|
17 | \begin{eqnarray} |
---|
18 | D(s,t) = &{(g_{NN}^\sigma)^4(t-4m^{*}2)^2 \over2(t-m_\sigma^2 )^2} + |
---|
19 | {(g_{NN}^\omega)^4(2s^2+2st+t^2-8m^{*2}s+8m^{*4}) \over (t-m_\omega^2)^2} + \nonumber\\ |
---|
20 | & {24(g_{NN}^\pi)^4m^{*2}t^2\over (t-m_\pi^2)^2} - |
---|
21 | {4(g_{NN}^\sigma g_{NN}^\omega)^2(2s+t-4m^{*2})m^{*2}\over |
---|
22 | (t-m_\sigma^2)(t-m_\omega^2)}, \nonumber |
---|
23 | \end{eqnarray} |
---|
24 | and |
---|
25 | \begin{eqnarray} |
---|
26 | E(s,t) = &{(g_{NN}^\sigma)^4\left( t(t+s)+4m^{*2}(s-t)\right)\over |
---|
27 | 8(t-m_\sigma^2)(u-m_\sigma^2) }+ |
---|
28 | {(g_{NN}^\omega)^4(s-2m^{*2})(s-6m^{*2}))\over 2(t-m_\omega^2)(u-m_\omega^2) } - \nonumber\\ |
---|
29 | &{6(g_{NN}^\pi)^4(4m^{*2}-s-t)m^{*4}t\over (t-m_\pi^2)(u=m_pi^2) }+ |
---|
30 | {3(g_{NN}^\sigma g_{NN}^\pi)^2 |
---|
31 | m^{*2} (4m^{*2}-s-t)(4m^{*2}-t) \over (t-m_\sigma^2)(u-m_\pi^2) } + \nonumber\\ |
---|
32 | &{3(g_{NN}^\sigma g_{NN}^\pi)^2 |
---|
33 | t(t+s)m^{*2}\over 2(t-m_\pi^2)(u-m_\sigma^2) } + |
---|
34 | {(g_{NN}^\sigma g_{NN}^\omega)^2 |
---|
35 | t^2-4m^{*2}s-10m^{*2}t+24m^{*4}\over4(t-m_\sigma^2)(u-m_\omega^2) } + \nonumber\\ |
---|
36 | &{(g_{NN}^\sigma g_{NN}^\omega)^2 |
---|
37 | (t+s)^2-2m^{*2}s+2m^{*2}t\over 4(t-m_\omega^2)(u-m_\sigma^2)} + |
---|
38 | {3(g_{NN}^\omega g_{NN}^\pi)^2 |
---|
39 | (t+s-4m^{*2})(t+s-2m^{*2})\over (t-m_\omega^2)(u-m_\pi^2)} + \nonumber\\ |
---|
40 | &{3(g_{NN}^\omega g_{NN}^\pi)^2 |
---|
41 | m^{*2} (t^2-2m^{*2}t)\over (t-m_\pi^2)(u-m_\omega^2)}. \\ |
---|
42 | \end{eqnarray} |
---|
43 | Here, in this first release, the in-medium mass was set to the free mass, and the nucleon |
---|
44 | nucleon coupling constants used were 1.434 for the $\pi$, 7.54 for the $\omega$, and 6.9 for |
---|
45 | the $\sigma$. This formula was used for elementary hadron-nucleon differential cross-sections |
---|
46 | by scaling teh center of mass energy squared accordingly. |
---|
47 | |
---|
48 | Finite size effects were taken into account at the meson nucleon vertex, |
---|
49 | using a phenomenological form factor (cut-off) at each vertex. |
---|