Charged pion polarizability (CPP) experiment at Jefferson Lab

The group is leading an experiment at Jefferson Lab’s Hall D to measure the electromagnetic polarizability of the charged pion using the Primakoff reaction gamma Nucleus -> pi+ pi- Nucleus .   The diagram below illustrates the general principle of the experiment.  At very low momentum transfer to the recoil nucleus, the incident photon interacts with a photon from the nuclear Coulomb field. In this low momentum transfer limit, the production amplitude is related through known kinematic factors to  the amplitude for gamma gamma -> pi+ pi- . In this process two photons collide to create two charged pions. The gamma gamma -> pi+ pi-  amplitude is related to the pion Compton scattering amplitude by “crossing symmetry”,  which is a formal technique from quantum mechanics.   Sensitivity to the electromagnetic polarizability of the charged pion is obtained from the Compton scattering amplitude.

To learn more about what an electromagnetic polarizability is, especially for an elementary particle, go the web page for the Spin-polarizability Experiment at Mainz.

Resources:

Undergraduate Honors Thesis’s:

Christian Haughwout
Design and Prototyping of MWPC Preamp Electronics for use in the Charged Pion Polarizability Experiment at Jefferson Lab

Robert Johnston
Design, Construction, and Simulation of Multi-wire Proportional Chambers for the Charged Pion Polarizability Experiment at Jefferson Lab

Jordan Kornfeld
Jefferson National Laboratory Charged Pion Polarizability Experiment: Monte Carlo Simulation Using GEANT4 and Construction of Multi-wire Proportional Chambers

Andrew Schick
Developing Methods for Measuring the Pion Polarizability

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