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Muon measurements

Here Al is actually a weighted average of electron and muon measurements, as well as decays to n y and n e e see Kirkby and Nir in Particle Data Group (2008). [Pg.136]

Fig. 1. Schematic for /zSR and fiLCR experiments. For pSR the muon spin polarization vector starts off in the x direction (open arrow). It then precesses about an effective field (the vector sum of the external field and the internal hyperfine field), which is normally approximately the z direction. The muons are detected in the M counter, and positrons from muon decay are detected in the L or R counters. For pLCR, the muon spin polarization is initially along the external field or t axis (solid arrow). The positron rates in the F and B counters are measured as a function of external field. A sharp decrease in the asymmetry of the F and B counting rates signifies a level crossing. Fig. 1. Schematic for /zSR and fiLCR experiments. For pSR the muon spin polarization vector starts off in the x direction (open arrow). It then precesses about an effective field (the vector sum of the external field and the internal hyperfine field), which is normally approximately the z direction. The muons are detected in the M counter, and positrons from muon decay are detected in the L or R counters. For pLCR, the muon spin polarization is initially along the external field or t axis (solid arrow). The positron rates in the F and B counters are measured as a function of external field. A sharp decrease in the asymmetry of the F and B counting rates signifies a level crossing.
The Mu spin Hamiltonian, with the exception of the nuclear terms, was first determined by Patterson et al. (1978). They found that a small muon hyperfine interaction axially symmetric about a (111) crystalline axis (see Table I for parameters) could explain both the field and orientation dependence of the precessional frequencies. Later /xSR measurements confirmed that the electron g-tensor is almost isotropic and close to that of a free electron (Blazey et al., 1986 Patterson, 1988). One of the difficulties in interpreting the early /xSR spectra on Mu had been that even in high field there can be up to eight frequencies, corresponding to the two possible values of Ms for each of the four inequivalent (111) axes. It is only when the external field is applied along a high symmetry direction that some of the centers are equivalent, thus reducing the number of frequencies. [Pg.579]

A AH < kT has important consequences. As the temperature is lowered to where AHg, kT, strong electron-phonon interactions must manifest themselves. Direct evidence for mode softening and strong electron-phonon coupling in the internal Ty < T < 250 K has been provided by measurements of the Mdssbauer recoiless fraction and the X-ray Debye-Waller factor as well as of muon-spin rotation Therefore, it would be... [Pg.18]


See other pages where Muon measurements is mentioned: [Pg.2886]    [Pg.449]    [Pg.133]    [Pg.134]    [Pg.135]    [Pg.137]    [Pg.252]    [Pg.348]    [Pg.349]    [Pg.28]    [Pg.205]    [Pg.242]    [Pg.569]    [Pg.570]    [Pg.571]    [Pg.582]    [Pg.584]    [Pg.33]    [Pg.18]    [Pg.68]    [Pg.4]    [Pg.339]    [Pg.163]    [Pg.217]    [Pg.252]    [Pg.241]    [Pg.253]    [Pg.256]    [Pg.140]    [Pg.1043]    [Pg.1210]    [Pg.1212]    [Pg.33]    [Pg.22]    [Pg.30]    [Pg.30]    [Pg.13]    [Pg.190]    [Pg.227]    [Pg.554]    [Pg.555]    [Pg.556]    [Pg.567]    [Pg.569]   
See also in sourсe #XX -- [ Pg.493 ]




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