Inverse shift of absorption peak versus applied dc magnetic field in interlayer exchange-coupled trilayer ferromagnetic films with inplane uniaxial anisotropy

2009 ◽  
Vol 246 (10) ◽  
pp. 2352-2358 ◽  
Author(s):  
Jihong Chen ◽  
Jiangwei Chen ◽  
Dongming Tang ◽  
Baoshan Zhang ◽  
Yi Yang ◽  
...  
Keyword(s):  
Magnetic Field ◽  
Uniaxial Anisotropy ◽  
Absorption Peak ◽  
Dc Magnetic Field ◽  
Ferromagnetic Films ◽  
Peak Versus ◽  
Interlayer Exchange

Electrical Anisotropy of Thin Metal Films Growing on Dielectric Substrates

2002 ◽  
Vol 7 (2) ◽  
pp. 45-52
Author(s):  
L. Jakučionis ◽  
V. Kleiza
Keyword(s):  
Magnetic Field ◽  
Thin Films ◽  
Uniaxial Anisotropy ◽  
Metal Films ◽  
Thin Layers ◽  
Electrical Anisotropy ◽  
Electrical Field ◽  
Dielectric Substrates ◽  
Unequal Probability ◽  
Conductive Thin Films

Electrical properties of conductive thin films, that are produced by vacuum evaporation on the dielectric substrates, and which properties depend on their thickness, usually are anisotropic i.e. they have uniaxial anisotropy. If the condensate grow on dielectric substrates on which plane electrical field E is created the transverse voltage U⊥ appears on the boundary of the film in the direction perpendicular to E. Transverse voltage U⊥ depends on the angle γ between the applied magnetic field H and axis of light magnetisation. When electric field E is applied to continuous or grid layers, U⊥ and resistance R of layers are changed by changing γ. It means that value of U⊥ is the measure of anisotropy magnitude. Increasing voltage U0 , which is created by E, U⊥ increases to certain magnitude and later decreases. The anisotropy of continuous thin layers is excited by inequality of conductivity tensor components σ0 ≠ σ⊥. The reason of anisotropy is explained by the model which shows that properties of grain boundaries are defined by unequal probability of transient of charge carrier.

Effect of Magnetic Fields on the Resistance and Microstructure of Al-Cu Alloy during Solidification Processing

2011 ◽  
Vol 287-290 ◽  
pp. 2916-2920
Author(s):  
Chun Yan Ban ◽  
Peng Qian ◽  
Xu Zhang ◽  
Qi Xian Ba ◽  
Jian Zhong Cui
Keyword(s):  
Magnetic Field ◽  
Magnetic Fields ◽  
Turning Points ◽  
Probe Method ◽  
Solidification Processing ◽  
Ac Magnetic Field ◽  
Dc Magnetic Field ◽  
Cu Alloy ◽  
The Difference ◽  
Good Agreement

The resistance of Al-21%Cu alloy under no magnetic field, DC magnetic field and AC magnetic field from liquid to solid was measured by a four-probe method. The difference of resistance versus temperature curves (R-T curves) was analyzed. It is found that the R-T curves of Al-21%Cu alloy are monotone decreasing and have two obvious turning points. Under DC magnetic field, the liquidus and solidus temperatures of the alloy both decrease, while under AC magnetic field, the liquidus and solidus temperatures both increase. There is a good agreement between the microstructure of quenching sample and R-T curves. The mechanism of the effect of magnetic fields was discussed.

New Nuclear-Spin-Induced Cotton-Mouton Effect in Fluids at High DC Magnetic Field

ChemPhysChem ◽  
2012 ◽  
Vol 13 (5) ◽  
pp. 1325-1331 ◽  
Author(s):  
Guo-hua Yao ◽  
Ming He ◽  
Dong-ming Chen ◽  
Tian-jing He ◽  
Fan-chen Liu
Keyword(s):  
Magnetic Field ◽  
Nuclear Spin ◽  
Dc Magnetic Field
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