K. Aulenbacher et al., THE MAMI SOURCE OF POLARIZED ELECTRONS, Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 391(3), 1997, pp. 498-506
The present work describes the source of polarized electrons that is r
un at the 855 MeV race track microtron MAMI at the Johannes Gutenberg
Universitat in Mainz. The source is based on photoelectron emission fr
om (III-V)-semiconductors. Presently strained layer InGaP- or GaAsP-ca
thodes are used, which are processed to negative electron affinity by
coverage of the surface with a submonolayer of caesium and oxygen. Ele
ctron beams spin-polarized up to a degree of P = 55% at a quantum effi
ciency of QE = 2% or P = 75% at QE = 0.4%, respectively, are obtained.
The well-known but hitherto unsolved problem of limited cathode lifet
ime has been sidestepped by the attachment of an UHV load lock system
to the source electron gun. It allows quick replacement of cathodes wi
thout breaking the gun vacuum. Availabilities in excess of 85% are obt
ained regularly in beamtimes longer than 100 h. The source was mainly
applied in measurements of nucleon form factors via the reactions H-1(
(e) over right arrow,e'(p) over right arrow), D-2((e) over right arrow
,e'(p) over right arrow), D-2((e) over right arrow,e'(n) over right ar
row), and (3) (H) over right arrow e((e) over right arrow,e'n). More t
han 1600h beamtime have been accomplished in physics experiments with
polarized electron beams at MAMI tip to now.