We have outlined a detector and electronics system which is capable of making a high-precision measurement of the positive muon lifetime in a time-structured beam. Our collaboration is capable of carrying out this experiment following a three year plan, commensurate with PSI scheduling.
In the first year following acceptance of this proposal, most of the work will take place at our home institutions. Critical items include: 1) PMT and base testing and selection; 2) Mechanical design of the detector; 3) Engineering stages for the WFD; 4) Prototyping of tiles; 5) Construction of two complete SuperTriangles and a mechanical support 6) Construction of sample targets. Having met these milestones, we will require a test period at PSI as outlined below. The residual polarization of the sulfur target will be compared to that in a non-depolarizing target such as Al.
In the second year, we will complete construction of the µLan
Detector and build the WFD. Tests of both subsystems will take place
at home institutions. At this stage, the DAQ system will take on a
more final form, given the best technology at the time (improvements
in tape drives, onboard processors, etc.). The PMTs and bases will
undergo a rigorous evaluation prior to installation. Each completed
tile will be subjected to uniformity and initial gain settings using a
106Ru source. We envision constructing a source assembly with a
magnetic channel to isolate the high-end of the beta spectrum, near
3 MeV. The clock system will be purchased and tested. At the end of
this year, the detector and electronics should be complete. The
system will be transported to PSI for debugging using a DC beam.
Among critical milestones during the testing will be to further
establish the level of residual polarization when using the sulfur
target. Conversely, we will use an Al target to measure the level of
symmetry in the diametrically opposed tile pairs of the detector.
Detailed background studies will be made. Finally, we hope to measure
to approximately 20 ppm. If the chopped beam is
available, we will make tests of the cycling and measure the effect of
dephasing.
In the third year, we expect that PSI will have developed the chopped beam and that the detector and electronics will be complete. Full commissioning and data taking will take place.
An compact list of beam requests and milestones, as presented at the beginning of this document is given next.