Anomalous capture of thermal polarized neutrons in perfect ferromagnetic single crystals

1969 ◽  
Vol 19 (2) ◽  
pp. 278-280 ◽  
Author(s):  
R. Michalec ◽  
V. Štich
1960 ◽  
Vol 31 (5) ◽  
pp. S27-S29 ◽  
Author(s):  
L. Néel ◽  
R. Pauthenet ◽  
G. Rimet ◽  
V. S. Giron

Magnetization curves for iron single crystals above the ‘knee’ are derived on the basis of domain theory for the case where the specimen is finite and the field is applied in an arbitrary direction with respect to the crystal axes. The shape of the specimen is important for the magnetization process and it is shown that in many cases the demagnetizing field must be such as to make the field actually acting in the crystal have a direction of symmetry (e. g. [111] or [110]) whatever the direction of the applied field. The cases of an oblate spheroid with its equatorial plane a (100) plane of the crystal and of a long rod with arbitrary orientation are considered in detail. In these cases simple expressions for the magnetization curves are obtained. There is good agreement with the experimental results of various authors for both parallel and normal components of magnetization. A method for correcting for the effect of internal strains is indicated.


1979 ◽  
Vol 72 (4-5) ◽  
pp. 361-362 ◽  
Author(s):  
Yu.A. Alexandrov ◽  
L.N. Sedláková ◽  
B. Chalupa ◽  
R.T. Michalec ◽  
P. Mikula ◽  
...  

1949 ◽  
Vol 45 (1) ◽  
pp. 145-156 ◽  
Author(s):  
H. Lawton

Recent papers by Néel (8) and Lawton and Stewart (7) have provided an explanation of the process of magnetization in a single crystal, using the well-known ideas of the domain theory but bringing out the important role played by the demagnetizing field. These authors applied their ideas to two shapes of single crystals of iron, long rods and oblate spheroids, but in the latter case the only crystal orientation worked out in detail was that in which the equatorial plane was (100). The case of oblate spheroids of iron and iron-silicon where the equatorial plane is a (110) plane of the crystal, and the magnetic field is applied in this plane, are considered in detail in this paper. Calculations are made for In, the component of magnetization perpendicular to the applied field He, and comparison made with experimental measurements. This particular problem was considered by Bozorth and Williams (4) who calculated the torque per unit volume (i.e. the product InHe) experienced by the crystal in a magnetic field. Their calculations are, however, incomplete, because their picture of the magnetization process is not a valid one in moderate fields. Moreover, the demagnetizing field was taken into account only in assessing the size of the field H acting within the crystal, but not its direction.


1972 ◽  
Vol 41 (2) ◽  
pp. 143-144 ◽  
Author(s):  
H. Ackermann ◽  
D. Dubbers ◽  
M. Grupp ◽  
P. Heitjans ◽  
G.Zu Putlitz ◽  
...  

1975 ◽  
Vol 32 (1) ◽  
pp. 157-163 ◽  
Author(s):  
R. R. Birss ◽  
D. G. Lord ◽  
D. J. Martin ◽  
S. M. N. Momen ◽  
M. R. Parker

2010 ◽  
Vol 110 (1) ◽  
pp. 78-90 ◽  
Author(s):  
I. V. Kireeva ◽  
Yu. I. Chumlyakov ◽  
Z. V. Pobedennaya ◽  
I. V. Kretinina ◽  
E. Cesari ◽  
...  

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