Møller scattering

Møller scattering is the name given to electron-electron scattering in Quantum field theory, named after the Danish physicist Christian Møller. The electron interaction that is idealized in Møller scattering forms the theoretical basis of many familiar phenomena such as the repulsion of electrons in the helium atom. While formerly many particle colliders were designed specifically for electron-electron collisions, more recently electron-positron colliders have become more common. Nevertheless, Møller scattering remains a paradigmatic process within the theory of particle interactions. Møller scattering is the name given to electron-electron scattering in Quantum field theory, named after the Danish physicist Christian Møller. The electron interaction that is idealized in Møller scattering forms the theoretical basis of many familiar phenomena such as the repulsion of electrons in the helium atom. While formerly many particle colliders were designed specifically for electron-electron collisions, more recently electron-positron colliders have become more common. Nevertheless, Møller scattering remains a paradigmatic process within the theory of particle interactions. We can express this process in the usual notation, often used in particle physics: In quantum electrodynamics, there are two tree-level Feynman diagrams describing the process: a t-channel diagram in which the electrons exchange a photon and a similar u-channel diagram. Crossing symmetry, one of the tricks often used to evaluate Feynman diagrams, in this case implies that Møller scattering should have the same cross section as Bhabha scattering (electron-positron scattering). In the electroweak theory the process is instead described by four tree-level diagrams: the two from QED and an identical pair in which a Z boson is exchanged instead of a photon. The weak force is purely left-handed, but the weak and electromagnetic forces mix into the particles we observe. The photon is symmetric by construction, but the Z boson prefers left-handed particles to right-handed particles. Thus the cross sections for left-handed electrons and right-handed differ. The difference was first noticed by the Russian physicist Yakov Zel'dovich in 1959, but at the time he believed the parity violating asymmetry (a few hundred parts per billion) was too small to be observed. This parity violating asymmetry can be measured by firing a polarized beam of electrons through an unpolarized electron target (liquid hydrogen, for instance), as was done by an experiment at the Stanford Linear Accelerator Center, SLAC-E158. The asymmetry in Møller scattering is where me is the electron mass, E the energy of the incoming electron (in the reference frame of the other electron), G F {displaystyle G_{ m {F}}} is Fermi's constant, α {displaystyle alpha } is the fine structure constant, Θ cm {displaystyle Theta _{ ext{cm}}} is the scattering angle in the center of mass frame, and θ W {displaystyle heta _{ m {W}}} is the weak mixing angle, also known as the Weinberg angle. The Møller scattering can be calculated from the QED point-of-view, at the tree-level, with the help of the two diagrams showed on this page. This two diagrams are contributing at leading order from the QED point-of-view. If we are taking in account the weak force, which is unified with the electromagnetic force at high energy, then we have to add two tree-level diagram for the exchange of a Z 0 {displaystyle Z^{0}} boson. Here we will focuse our attention on a strict tree-level QED computation of the cross section, which is rather instructive but maybe not the most accurate description from a physical point-of-view. Before the derivation, we write the 4-momenta as ( p 1 {displaystyle p_{1}} and p 2 {displaystyle p_{2}} for incoming electrons, p 3 {displaystyle p_{3}} and p 4 {displaystyle p_{4}} for outgoing electrons, and m = m e {displaystyle m=m_{e}} ): p 1 = ( E , 0 , 0 , p ) ,   p 2 = ( E , 0 , 0 , − p ) , {displaystyle p_{1}=(E,0,0,p),~p_{2}=(E,0,0,-p),} p 3 = ( E , p sin ⁡ θ , 0 , p cos ⁡ θ ) ,   p 4 = ( E , − p sin ⁡ θ , 0 , − p cos ⁡ θ ) . {displaystyle p_{3}=(E,psin heta ,0,pcos heta ),~p_{4}=(E,-psin heta ,0,-pcos heta ).}