µALCR  
 Canadian Inst. for Advanced Research 
 
 and 
 Dept. of Physics & Astronomy, 
 
 Univ. of British Columbia, Vancouver, BC, Canada V6T 1Z1
This page is under construction at     
 
 /~jess/musr/
First let's talk about the acronym: 
when these phenomena were first discovered in 1985-1986 at TRIUMF, 
the term ``level-crossing resonance'' (LCR) was used to describe 
the situation where the muon Zeeman splitting matches that of another 
spin system which can thus exchange polarization with the muon ensemble 
in a sort of ``flip-flop'' mutual transition.  
Shortly thereafter, similar experiments were begun at PSI, 
where the proponents pointed out quite correctly that the 
levels never actually cross; this being an intrinsically 
quantum mechanical phenomenon, the energy eigenstates of the 
combined system avoid crossing, so that the proper 
terminology is ``avoided level crossing'' (ALC) 
[resonance].  
In an effort to keep everyone relatively happy, I have adopted 
the acronym µALCR, the meaning of which 
I trust is obvious now to all concerned.  
-    Nuclear Quadrupolar µALCR: 
  
  
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  The first such phenomenon observed in µSR was 
  the resonant relaxation of muons in copper at the 
  longitudinal field where the muon Zeeman splitting matches 
  the splitting of the Cu nuclear quadrupole moment in the 
  electric field gradient (EFG) due to the interstitial muon.  
  This possibility was predicted by Anatole Abragam in 1984.  
  Almost the same thing was suggested a few years earlier by 
  Tom McMullen and Eugene Zaremba, but we misunderstood and 
  looked for a resonance in transverse field. 
      ``Doh!'' 
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 -    Paramagnetic µALCR: 
  
  
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  In the case of a paramagnetic system, the unpaired electron 
  couples to both the muon and a nearby nucleus via 
  their respective hyperfine (HF) interactions, thus allowing the 
  muon and nuclear spins to ``flip-flop'' much more strongly 
  than through mere nuclear dipolar couplings.  
  This picture may be a little oversimplified. . . .
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  This was first observed in the ``muonated radical'' formed by 
  addition of muonium (Mu) to a double C=C bond in the 
  tetramethylethylene molecule.  The time dependence of the 
  muon polarization on and off a resonant LF was also 
  observed at that time.  
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  Similar behaviour was seen in 
  C6F6 µ., 
  the muonated radical formed by addition of Mu to a C=C 
  bond in hexafluorobenzene.  
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 -    Applications of µALCR: 
  
  
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  Quadrupolar µALCR is often used to determine 
  the muon site in diamagnetic solids or to confirm the formation of 
  a diamagnetic molecule incorporating the muon, as in this example.  
  (There are prettier cases, but I don't have the figures for them 
  handy.)  
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  Paramagnetic µALCR has found many applications to 
  the study of radicals in chemistry, many of which are difficult 
  or impossible to detect by other means.  Since the difference between 
  the ``muonated'' radical and the analogous ``hydrogenated'' version 
  (formed by addition of an H atom to a double bond) is mainly in the 
  configuration of a single bond (due to the lighter mass of the muon), 
  much can be learned about the behaviour and structure of such molecules 
  using µALCR.  
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  Paramagnetic µALCR is also an important tool 
  for determining the local electronic structure of the Mu* centre 
  in various semiconductors, where the HF couplings to various 
  nearby nuclei (and the orientation dependence of the µALCR 
  spectrum) reveal minute details of the muon's location and environment.  
  The examples shown are GaP and GaAs, the first 
  materials studied by this method.  Such measurements have since 
  been extended to 29Si-enriched silicon and 
  13C-enriched diamond and well as many other systems. 
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  I include this pretty spectrum from copper chloride 
  just for aesthetics.  
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