Bhabha scattering

Deriving unpolarized cross section

Matrix elements

Both the scattering and annihilation diagrams contribute to the transition matrix element. By letting k and k' represent the four-momentum of the positron, while letting p and p' represent the four-momentum of the electron, and by using Feynman rules one can show the following diagrams give these matrix elements:

Notice that there is a relative sign difference between the two diagrams.

Square of matrix element

To calculate the unpolarized cross section, one must average over the spins of the incoming particles (s_e- and s_e+ possible values) and sum over the spins of the outgoing particles. That is,

First, calculate ${\displaystyle |\mathcal{M}{|}^2}$:

Scattering term (t-channel)

Magnitude squared of M

Sum over spins

Next, we'd like to sum over spins of all four particles. Let s and s' be the spin of the electron and r and r' be the spin of the positron.

Now that is the exact form, in the case of electrons one is usually interested in energy scales that far exceed the electron mass. Neglecting the electron mass yields the simplified form:

Annihilation term (s-channel)

The process for finding the annihilation term is similar to the above. Since the two diagrams are related by crossing symmetry, and the initial and final state particles are the same, it is sufficient to permute the momenta, yielding

(This is proportional to ${\displaystyle (1+{\cos }^2\theta )}$ where ${\displaystyle \theta }$ is the scattering angle in the center-of-mass frame.)

Solution

Evaluating the interference term along the same lines and adding the three terms yields the final result

${\displaystyle \frac{\overline{|\mathcal{M}{|}^2}}{2e^4}=\frac{u^2+s^2}{t^2}+\frac{2u^2}{st}+\frac{u^2+t^2}{s^2}}$

Simplifying steps

Completeness relations

The completeness relations for the four-spinors u and v are

${\displaystyle \sum _{s=1,2}{u}_p^{(s)}{\overline{u}}_p^{(s)}=p/+m}$

${\displaystyle \sum _{s=1,2}{v}_p^{(s)}{\overline{v}}_p^{(s)}=p/-m}$

where

${\displaystyle p/={\gamma }^{\mu }{p}_{\mu }}$ (see Feynman slash notation)

${\displaystyle \overline{u}=u^{†}{\gamma }^0}$

Trace identities

To simplify the trace of the Dirac gamma matrices, one must use trace identities. Three used in this article are:

1. The Trace of any product of an odd number of ${\displaystyle {\gamma }_{\mu }}$'s is zero
2. ${\displaystyle \mathrm{Tr}({\gamma }^{\mu }{\gamma }^{\nu })=4{\eta }^{\mu \nu }}$
3. ${\displaystyle \mathrm{Tr}\left({\gamma }_{\rho }{\gamma }_{\mu }{\gamma }_{\sigma }{\gamma }_{\nu }\right)=4\left({\eta }_{\rho \mu }{\eta }_{\sigma \nu }-{\eta }_{\rho \sigma }{\eta }_{\mu \nu }+{\eta }_{\rho \nu }{\eta }_{\mu \sigma }\right)}$

Using these two one finds that, for example,

Uses

Bhabha scattering has been used as a luminosity monitor in a number of e⁺e⁻ collider physics experiments. The accurate measurement of luminosity is necessary for accurate measurements of cross sections.

Small-angle Bhabha scattering was used to measure the luminosity of the 1993 run of the Stanford Large Detector (SLD), with a relative uncertainty of less than 0.5%.

Electron-positron colliders operating in the region of the low-lying hadronic resonances (about 1 GeV to 10 GeV), such as the Beijing Electron–Positron Collider II and the Belle and BaBar "B-factory" experiments, use large-angle Bhabha scattering as a luminosity monitor. To achieve the desired precision at the 0.1% level, the experimental measurements must be compared to a theoretical calculation including next-to-leading-order radiative corrections. The high-precision measurement of the total hadronic cross section at these low energies is a crucial input into the theoretical calculation of the anomalous magnetic dipole moment of the muon, which is used to constrain supersymmetry and other models of physics beyond the Standard Model.