Difference between revisions of "Forest Bhabha Scattering"
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=Matrix element for scattering= | =Matrix element for scattering= | ||
+ | |||
+ | According to the Feynman RUles for QED: | ||
+ | |||
+ | the term | ||
+ | |||
+ | ig_e \gamma^{\me} | ||
+ | |||
+ | used at the vertex to describe the interaction beetween the two spinor states entering the vertex and forming a photon which will "connect" this vertex with the next one. | ||
+ | |||
<math>\mathcal{M}_s = \,</math> | <math>\mathcal{M}_s = \,</math> | ||
<math>e^2 \left( \bar{u}_{3} \gamma^\nu u_4 \right) \frac{1}{(p_1+p_2)^2} \left( \bar{u}_{2} \gamma_\nu u_{1} \right) </math> | <math>e^2 \left( \bar{u}_{3} \gamma^\nu u_4 \right) \frac{1}{(p_1+p_2)^2} \left( \bar{u}_{2} \gamma_\nu u_{1} \right) </math> |
Revision as of 15:47, 14 April 2012
Bhabha (electron -positron) Scattering
Bhabha scattering identifies the scatterng of an electron and positron (particle and anti-particle). There are two processes that can occur
1.) scattering via the exchange of a virtual photon
2.) annihilation in which the e+ and e- spend some time as a photon which then reconverts back to an e+e- pair
variables
Let:
- initial electron 4-momentum
- u_1 \equiv initial electron spinor
- p_2 \equiv final electron 4-momentum
- u_2 \equiv final electron spinor
- p_3 \equiv initial positron 4-momentum
- \bar{u}_3 \equiv initial positron spinor
- p_4 \equiv finial positron 4-momentum
- finial positron spinor
Matrix element for scattering
According to the Feynman RUles for QED:
the term
ig_e \gamma^{\me}
used at the vertex to describe the interaction beetween the two spinor states entering the vertex and forming a photon which will "connect" this vertex with the next one.
Matrix element for annihilation