Magneto-Resistance Effect of Ni3Fe Single Crystals

1980 ◽  
Vol 19 (4) ◽  
pp. 623-626 ◽  
Author(s):  
Toshio Mizorogi ◽  
Yoshiaki Matsuo ◽  
Takeharu Minegishi
1951 ◽  
Vol 83 (4) ◽  
pp. 768-776 ◽  
Author(s):  
G. L. Pearson ◽  
H. Suhl

1999 ◽  
Vol 313 (3-4) ◽  
pp. 294-304 ◽  
Author(s):  
R.M. Langan ◽  
S.N. Gordeev ◽  
M. Oussena ◽  
P.A.J. de Groot ◽  
A.G.M. Jansen ◽  
...  

In heat conductivity measurements between 2 and 4·5° K twenty-seven pure metals have been subjected to a magnetic field of 4 kOe. Of these, Cd, Sn, Pb, Zn, Ga, Ag, Tl and In show appreciable magneto-resistance effects. Single crystals of Cd, Sn and Pb were investigated and of Zn and Ga, single crystals of different orientations. Ag, Tl and In were polycrystalline specimens. Transverse and longitudinal fields were applied, the effect being always greater in the transverse case. Single crystals of Zn, Sn, Cd and a specimen of Tl were investigated in transverse fields up to 18·5 kOe. The thermal resistance of the cadmium crystal was increased by a factor of 1000 at 2·3° K, and the use of this effect in a thermal switch has been suggested. In transverse fields the thermal resistance of all metals was found to rise linearly except for very small fields. Indications of saturation effects were only obtained in longitudinal fields. The results have been discussed on the basis of existing theory.


The Hall effect in single crystals of tin shows oscillations at temperatures below 4.2 K when B lies along, or very near, the [001] axis. The amplitude of the oscillations has a sharp maximum 1° away from the axis and has vanished by 4°. The oscillations are explained in terms of the migration of electrons by magnetic breakdown between the e 5 1 and δ 1 1 orbits, as has already been invoked to account for oscillatory magneto-resistance. To account for the existence of off-axis Hall oscillations when, as is known, breakdown is confined to a fairly narrow central zone, it is found necessary to include collisions of the electrons with impurities even though these are rare enough for ω c т to be as large as 200. The theory is developed in terms of diffusion of electrons on a limited orbit-network, and an explicit expression derived for the angular variation of oscillatory amplitude, which is found to agree well when independent estimates of the relevant parameters are used.


Low -temperature measurements of transverse magneto-resistance were made on 24 single crystals of pure aluminium in magnetic fields up to 20 kG. In contrast with the theory, neither complete saturation of magneto-resistance nor quadratic variation with field were observed in any orientation. The anisotropy of themagneto-resistance was small, but showed a pattern consistent with symmetry requirements. These results appear inexplicable on a basis of Harrison’s four orthogonal plane wave model of the aluminium Fermi surface, but can be explained qualitatively in terms of a slightly different Fermi surface which touches the corners of the second Brillouin zone. This model is not inconsistent with other experimental results.


The experiments to be described in this paper, deal with the change of resistance of single crystals of iron caused by a magnetic field perpendicular to the direction of the current. In two earlier papers, it has been shown that both the phenomena of magneto-striction and change of resistance in a longitudinal magnetic field were very different when measured in different directions in the crystal. And the results led to the conclusion that the change of resistance in the latter case was due to the change of orientation of the atoms accompanying magnetization, any direct influence of the field on the resistance being negligible. With these results in mind it seemed important to determine how the change of resistance in a transverse magnetic field depended on the crystal structure, and whether this more complicated effect, dealing with two directions in the crystal instead of one, would fit in with the results previously obtained. Many measurements of this phenomenon have been made for soft iron, and it has generally been accepted that there is only a decrease of resistance, slow at first, then rapid, finally approaching a saturation value. Occasionally an initial increase has been found, but this has not been considered genuine, being accounted for by the presence of a longitudinal component of magnetization due to imperfect orientation of the rod in the magnetic field.


2019 ◽  
Author(s):  
V. Harimohan ◽  
A. Bharathi ◽  
P. D. Babu ◽  
R. Rajaraman ◽  
C. S. Sundar

1937 ◽  
Vol 33 (1) ◽  
pp. 145-153 ◽  
Author(s):  
C. J. Milner

A method of growing single-crystal resistance specimens free, to a large extent, from strains and impurities is described. The magneto-resistance effect in cadmium single crystals has been studied in some detail at the temperature of liquid nitrogen, using sufficiently high magnetic fields to observe the linear effect found by Kapitza.Although it proved impossible, in general, to determine the orientation of individual crystals, the experiments suggest that the “critical field” of the linear effect is dependent on the orientation of the crystal with respect to the current and magnetic field, and not on the perfection of the crystal lattice.


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