Dephasing due to Spin–Wave Excitations in Ferromagnetic Metals

2003 ◽  
Vol 72 (5) ◽  
pp. 1155-1160 ◽  
Author(s):  
Yositake Takane
1974 ◽  
Vol 52 (8) ◽  
pp. 694-703 ◽  
Author(s):  
G. Lonzarich ◽  
A. V. Gold

High resolution measurements of the de Haas–van Alphen frequency associated with the minority-spin electron 'lens' sheets of the Fermi surface of iron have been carried out between 1 and 4.2 K. The variation of the frequency over this temperature range is found to be less than one part in 105 (the resolution of our experiment) and is virtually identical to that found for the corresponding electron lenses in molybdenum. By contrast, a variation of one part in 104 would be expected for the Fe lenses on the basis of a literal interpretation of the Stoner model, in which the exchange splitting of the energy bands is proportional to the magnetization at all temperatures. The absence of any significant change of the frequency with temperature can be understood if the magnetization decreases almost entirely by spin wave excitations, and if the spin waves have negligible effect on the exchange splitting.


2006 ◽  
Vol 600 (18) ◽  
pp. 4151-4154 ◽  
Author(s):  
T.M. Nguyen ◽  
M.G. Cottam

2017 ◽  
Vol 50 (18) ◽  
pp. 185003 ◽  
Author(s):  
M Zelent ◽  
N Tahir ◽  
R Gieniusz ◽  
J W Kłos ◽  
T Wojciechowski ◽  
...  

Physica B+C ◽  
1988 ◽  
Vol 150 (3) ◽  
pp. 423-424
Author(s):  
Shoichi Nagata ◽  
Shuji Ebisu ◽  
Satoshi Taniguchi

1974 ◽  
Vol 52 (8) ◽  
pp. 704-707 ◽  
Author(s):  
D. M. Edwards

It is shown that the de Haas–van Alphen (dHvA) effect in ferromagnetic metals can give information about the Stoner T2 term in the temperature dependence of the magnetization, without interference from spin wave contributions. In particular, the temperature dependence of the dHvA frequency for a very weak itinerant electron ferromagnet could distinguish clearly between conflicting theories of these materials.


1973 ◽  
Author(s):  
R. E. Dodd ◽  
L. K. Wilson ◽  
C. Vittoria ◽  
H. Lessoff ◽  
Hugh C. Wolfe ◽  
...  

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