Author/Authors :
Marchand، نويسنده , , D. and Arvieux، نويسنده , , J. and Batigne، نويسنده , , G. and Bimbot، نويسنده , , L. and Biselli، نويسنده , , A. Fevrier-Bouvier، نويسنده , , J. and Breuer، نويسنده , , H. and Clark، نويسنده , , R. and Cuzon، نويسنده , , J.-C. and Engrand، نويسنده , , M. E. Foglio، نويسنده , , R. and Furget، نويسنده , , C. and Grave، نويسنده , , X. and Guillon، نويسنده , , Ayse B. and Guler، نويسنده , , H. and King، نويسنده , , P.M. and Kox، نويسنده , , S. ، نويسنده ,
Abstract :
The G 0 parity-violation experiment at Jefferson Lab (Newport News, VA) is designed to determine the contribution of strange/anti-strange quark pairs to the intrinsic properties of the proton. In the forward-angle part of the experiment, the asymmetry in the cross-section was measured for e ⇒ p elastic scattering by counting the recoil protons corresponding to the two beam-helicity states. Due to the high accuracy required to measure the few-part-per-million asymmetry, the G 0 experiment was based on a custom experimental setup with its own associated electronics and data acquisition (DAQ) system. Highly specialized time-encoding electronics provided time-of-flight spectra for each detector for each helicity state. More conventional electronics, processing only a small fraction of the events, was used for monitoring (mainly FastBus). The time-encoding electronics and the DAQ system have been designed to handle events from the 128 detector pairs at a mean rate of 2 MHz per detector pair with low deadtime and with minimal helicity-correlated systematic errors. In this paper, we outline the general architecture and the main features of the electronics and the DAQ system dedicated to G 0 forward-angle measurements.
Keywords :
High rate electronics , Electron scattering , parity violation , Time encoding