PSI Muons - ISIS

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$Single Crystal Diffraction: Shelx tutorial - ISIS$

Jess Brewer, UBC & TRIUMF: “Decay” and “Surface” muon beams
<strong>PSI</strong> muon beam time structure Pion decay time of 26 ns is “smearing” the proton beam structure in the muon beam. This results in a “continuous” muon beam. A µ + rate R of 10 5 /s means: average time between to µ + is 1/R = 10 µs. Probability p to have the next µ + at time t: p = 1 – exp(-Rt) (“pile-up”) Single µ + can be detected with very good time resolution (< 1ns), compared to a bunch width of 50-100 ns at pulsed beams. --> measurement of GHz frequencies and fast relaxation rates (>100 µs -1 ). But “accidental” background in µ-decay histograms.
Page 1 and 2: Wir schaffen Wissen - heute für mo
Page 3 and 4: n SINQ SwissFEL µSµS γ SLS
Page 5: The PSI isochronous cyclotron 2.2 m
Page 9 and 10: Continuous versus pulsed muon beams
Page 11 and 12: ● GPS “tells” kicker to send
Page 13 and 14: The new high-field µSR facility at
Page 18: Oxford Instrument 8/9.5 T Recondens
Page 22 and 23: Commissioning 2012, user operation
Page 24 and 25: Implantation Profiles of Low Energy
Page 26 and 27: Generation of polarized epithermal
Page 28 and 29: Characteristics of epithermal muons
Page 30 and 31: LE-µ + beam and LE-µSR spectromet
Page 32 and 33: Low energy µ + beam and set-up for
Page 34 and 35: Magnetic field profiles in supercon
Page 36 and 37: In-plane Anisotropy in detwinned YB
Page 38 and 39: Meissner effect in a strongly under
Page 40 and 41: Spatially homogeneous ferromagnetis
Page 42 and 43: “Cold” muonium from mesoporous
Page 44 and 45: Developments • Spin-rotator for L
Page 46 and 47: LEM spin-rotator installation Jan-1
Page 48: LEM group at PSI T. Prokscha, H. Sa

PSI Muons - ISIS

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