Hall Effect of a Compensated Magnetic Metal Proportional toMB2in the High-Field Limit

1969 ◽  
Vol 177 (2) ◽  
pp. 790-792 ◽  
Author(s):  
L. Berger
1992 ◽  
Vol 46 (1) ◽  
pp. 223-230 ◽  
Author(s):  
I. Avgin ◽  
D. L. Huber ◽  
W. Y. Ching
Keyword(s):  

2011 ◽  
Vol 317-319 ◽  
pp. 1136-1140 ◽  
Author(s):  
Brajalal Sinha ◽  
Sunjong Oh ◽  
Torati Sri Ramulu ◽  
Jaein Lim ◽  
Dong Young Kim ◽  
...  

Planar Hall effect sensor has been explored using multi-layer cross-shaped and bridge geometry. We present planar Hall effect in a ring-shaped geometry experimentally that shows progress of sensor sensitivity as well as output signals. Sensitivity improves about 170 times compare to cross-shaped geometry and about 1.4 times to bridge geometry in conventional measurement system. These values become 2.5 times larger at 20o measurement system. The presented ring geometry may take great potential in Planar Hall effect sensor applications.


1963 ◽  
Vol 34 (4) ◽  
pp. 777-780 ◽  
Author(s):  
K. K. N. Chang ◽  
R. D. Hughes
Keyword(s):  

1974 ◽  
Vol 25 (2) ◽  
pp. 489-494 ◽  
Author(s):  
W. Bohmeyer ◽  
W. Hoerstel

1960 ◽  
Vol 38 (7) ◽  
pp. 941-944 ◽  
Author(s):  
Richard Stevenson

Magneto-optical rotation by transmission through or reflection from solids is examined by the classical free electron theory, with the view of taking such a measurement using fields in the megagauss range. In general the rotation is a markedly non-linear function of the magnetic field, and in some cases can change in sign as the field increases. For very low fields the rotation varies directly with B, but in the high field limit the rotation varies inversely with the field. For substances in which the intercollision time of the electron is small, measurements of the Kerr rotation (i.e. by reflection) will give the electron mobility as a function of the magnetic field, and thus will give important data which can be used in conjunction with high field magnetoresistance experiments.


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