nuclear acoustic resonance
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2021 ◽  
Vol 119 (17) ◽  
pp. 174001
Author(s):  
Laura A. O'Neill ◽  
Benjamin Joecker ◽  
Andrew D. Baczewski ◽  
Andrea Morello

2010 ◽  
Vol 203 (2) ◽  
pp. 203-207 ◽  
Author(s):  
J. Mende ◽  
N. Elmiladi ◽  
C. Höhl ◽  
K. Maier

2008 ◽  
Author(s):  
Bernhard R. Tittmann ◽  
P.M. Lenahan ◽  
David Spears ◽  
Rhys Williams

2006 ◽  
Author(s):  
J Herberg ◽  
R Maxwell ◽  
B Tittmann ◽  
P Lenahan ◽  
S Yerkes ◽  
...  

2005 ◽  
Author(s):  
J Herberg ◽  
R Maxwell ◽  
B Tittmann ◽  
P Lenahan ◽  
S Yerkes ◽  
...  

The ground configuration of the europium ion, Eu 3+ , 4f 6 , 7 F, is split by spin-orbit interaction into a series of levels J = 0 to 6. There are matrix elements of the electronic Zeeman interaction Z e and hyperfine interaction Z hfs between states of different J . In particular, for the lowest state, the singlet J = 0, matrix elements to the first excited state J = 1 produce contributions to the nuclear Zeeman and electric quadrupole interactions in J = 0. Formulae for these are listed by Bleaney & Leask (1994) for three tetragonal compounds. One of these is EuVO 4 , for which existing measurements by optical ‘hole-burning’ are discussed, together with the possibility of nuclear orientation and dynamic nuclear polarization. Experiments using nuclear acoustic resonance are suggested in a following paper.


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