Author/Authors :
Bogorad، نويسنده , , P. and Brash، نويسنده , , E.J. and Cates، نويسنده , , G.D. and Cummings، نويسنده , , W.J. and Gorelov، نويسنده , , A. and Hasinoff، نويسنده , , M.D. and Hausser، نويسنده , , O. and Hicks، نويسنده , , K. and Holmes، نويسنده , , R. and Huang، نويسنده , , J.C. and Krieger، نويسنده , , D. and Kumar، نويسنده , , K.S. and Larson، نويسنده , , B. and Lorenzon، نويسنده , , W. and McCracken، نويسنده , , J. R. Michaux، نويسنده , , P، نويسنده ,
Abstract :
We describe a device used in experiment 1231 at LAMPF and in e683 at TRIUMF to study the spin dependence of the reaction μ− + 3He → 3H + vμ. In order to study the spin dependence, we needed to form and polarize muonic 3He and in the same volume detect the 1.9 MeV tritons created in the reaction. Furthermore, the recoil direction of the tritons had to be determined. The apparatus served both as a polarized target and as a detector. The detector, a gridded ion chamber, was incorporated inside a 51 polarized target that was filled with 8 atm of 3He and 100 Torr of N2 and rubidium metal. At the operating temperature of the device (205–230°C) the rubidium number density was approximately 1015 atoms/cm3. Muons that stopped in the target formed muonic helium atoms, which were then polarized by collisions with optically pumped Rb vapor. Two high-powered GaAlAs diode laser arrays were used to polarize the Rb in the 100 cm3 fiducial volume located inside the ion chamber. The ion chamber produced clean signals from the reaction tritons despite having to operate under the extreme conditions required for efficient optical pumping. The direction of the tritons was determined by analyzing the shapes of the ionization pulses. The muon polarization was measured using the decay electron asymmetry.
Keywords :
Muon , Pseudoscalar , ionization chamber , Polarized target