Muon transfer from deuterium to helium
/ Authors
M. Augsburger, P. Ackerbauer, W. Breunlich, M. Cargnelli, D. Chatellard, J. Egger, B. Gartner, F. Hartmann, O. Huot, R. Jacot-Guillarmod
and 16 more authors
P. Kammel, R. King, P. Knowles, A. Kosak, B. Lauss, J. Marton, M. Muehlbauer, F. Mulhauser, C. Petitjean, W. Prymas, L. Schaller, L. Schellenberg, H. Schneuwly, S. Tresch, T. Egidy, J. Zmeskal
/ Abstract
We report on an experiment at the Paul Scherrer Institute, Villigen, Switzerland measuring x rays from muon transfer from deuterium to helium. Both the ground-state transfer via the exotic (d{mu}{sup 3,4}He){sup *} molecules and the excited-state transfer from ({mu}d){sup *} were measured. The use of charge-coupled device detectors allowed x rays from 1.5 keV to 11 keV to be detected with sufficient energy resolution to separate the transitions to different final states in both deuterium and helium. The x-ray peaks of the (d{mu}{sup 3}He){sup *} and (d{mu}{sup 4}He){sup *} molecules were measured with good statistics. For the D{sub 2}+{sup 3}He mixture, the peak has its maximum at E{sub d{mu}}{sub {sup 3}He}=6768{+-}12 eV with full width at half maximum (FWHM) {gamma}{sub d{mu}}{sub {sup 3}He}=863{+-}10 eV. Furthermore, the radiative branching ratio was found to be {kappa}{sub d{mu}}{sub {sup 3}He}=0.301{+-}0.061. For the D{sub 2}+{sup 4}He mixture, the maximum of the peak lies at E{sub d{mu}}{sub {sup 4}He}=6831{+-}8 eV and the FWHM is {gamma}{sub d{mu}}{sub {sup 4}He}=856{+-}10 eV. The radiative branching ratio is {kappa}{sub d{mu}}{sub {sup 4}He}=0.636{+-}0.097. The excited-state transfer is limited by the probability to reach the deuterium ground state, q{sub 1s}. This coefficient was determined for both mixtures: q{sub 1s}{sup {sup 3}He}=68.9{+-}2.7%more » and q{sub 1s}{sup {sup 4}He}=90.1{+-}1.5%.« less
Journal: Physical Review A