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The dmvfinant contributions 6 and to these processes in the left-right models come from the box graphs involving the exchange of two W/t-fields and leads to a branching ratio for p _ e- conversion as follows; where ,= sin_6w M_ct, Similarly, for spin zero nuclei,the branching estimated to be: - scenerio, this branching Violating In this section, SUSY M_n] _] ratio turns out to be about 10-14 Models we will consider model based on supersymmetry, ( ratio for the p- ---,e+ conversion can be 8rsin2_w In the most optimistic 6.

Still the pion contamination has to be kept as low as possible, since the background level is roughly 10 -5 per stopped pion. A disadvantage of the simple signature and the structureless time distribution is the susceptibility to background from cosmic rays, which has to be suppressed with passive shielding or identified by the occurrence of additional signals in the detectors. 2 The ct_iilcictellccs, SINDRUM which lt)rlllS the i11aitl source of background ill II Experiment. The SINDRUM II spectrometer [5] has been designed for the se_uch for #,-e conversion with a sensitivity which is more them two orders of magnitude higher than achieved in the previous experiment.

The distribution of the distances of closest approach measured for M atom decays, detected by the coincidence of the energetic e+ and the atomic e-, is shown in Fig. 4. A cylindrical arrangement of 12 pure Csl crystals surrounds the MCP to observe the two 51l k(_ photons emitted froni _+ alinihilating in ttlc _1(_1. The soil(! _r, its e)lergy resolution resolution of its signals is 7 7_s FWIIM. To trigger coincidence relevant the data of the hodoscope, time-of-flight in the SINDRUM, by" reversing acquisition syst(,m in search :)0()f, FWIIM, alid tlw t,imillg of the ,_1 ---+ i_,/ co)lx'(,rsi()n, a triple the MCP, and at.

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Low Energy Muon Science [procs, intl wkshp 1993)


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