Published December 1998 | Version v1
Journal article

Electron beam polarimetry

  • 1. Jefferson Laboratory 12000 Jefferson Avenue, Newport News, Virginia, 23606 (United States)

Description

Along with its well known charge and mass, the electron also carries an intrinsic angular momentum, or spin. The rules of quantum mechanics allow us to measure only the probability that the electron spin is in one of two allowed spin states. When a beam carries a net excess of electrons in one of these two allowed spin states, the beam is said to be polarized. The beam polarization may be measured by observing a sufficient number of electrons scattered by a spin-dependent interaction. For electrons, the useful scattering processes involve Coulomb scattering by heavy nuclei, or scattering from either polarized photons or other polarized electrons (known as Mott, Compton, and Moeller scattering, respectively). In this tutorial, we will briefly review how beam polarization is measured through a general scattering process, followed by a discussion of how the three scattering processes above are used to measure electron beam polarization. Descriptions of electron polarimeters based on the three scattering processes will be given. copyright 1998 American Institute of Physics

Additional details

Publishing Information

Journal Title
AIP Conference Proceedings
Journal Volume
451
Journal Issue
1
Journal Page Range
p. 23-39
ISSN
0094-243X
CODEN
APCPCS

Conference

Title
8. beam instrumentation workshop (BIW-98)
Dates
4-7 May 1998
Place
Stanford, CA (United States)

Optional Information

Secondary number(s)
CONF-980573--