scholarly journals Measurement of the magnetic field-dependent refractive index of magnetic fluids in bulk

2008 ◽  
Vol 6 (3) ◽  
pp. 195-197 ◽  
Author(s):  
刘婷 Ting Liu ◽  
陈险峰 Xianfeng Chen ◽  
狄子昀 Ziyun Di ◽  
张军锋 Junfeng Zhang ◽  
李新碗 Xinwan Li ◽  
...  
2010 ◽  
Vol 39 (10) ◽  
pp. 1742-1746 ◽  
Author(s):  
卜胜利 PU Sheng-li ◽  
刘明 LIU Ming ◽  
孙国庆 SUN Guo-qing

1960 ◽  
Vol 15 (3) ◽  
pp. 220-226 ◽  
Author(s):  
Klaus Körper

Radial oscillations are excited in a homogeneous infinite plasma cylinder in a homogeneous axial magnetic field by a surface current which is homogeneous in the axial and azimuthal directions. The modes of oscillations corresponding to the axial and azimuthal components of current are not coupled, and so they may be analysed separately. The magnetic field in the plasma and vacuum is obtained, and the indices of refraction for both types of oscillations are discussed thoroughly. When the currents are parallel to the external magnetic field, the oscillations are characterized by the refractive index of Eccles. On the other hand, when the current is perpendicular to the magnetic field two resonance frequencies exist, which depend on the density of the plasma and the magnetic field strength. — In the latter case the radial characteristic oscillations of the plasma cylinder in an external magnetic field are considered.


The diamagnetism of free electrons in the presence of charged impurity centres which are sufficiently dilute to be non-interacting is calculated to first order in the strength of the potential of the impurity centre. This is done by combining the density-matrix treatment of Landau diamagnetism with the impurity-screening theory o f March & Murray. The susceptibility involves the integrated value of the impurity potential through the crystal, and its first derivative with respect to the magnetic field, B. If the impurity potential is assumed to have a value appropriate to B — 0, then the result for the change in diamagnetic susceptibility on alloying agrees with that of Kohn & Luming (1963). It is shown, however, that the impurity potential is modified in the presence of the magnetic field, and in particular it has angular dependence. The correction to the dia­magnetic susceptibility due to this self-consistency is shown to be significant (25% ). The relevance of the theory to experimental results on dilute alloys is briefly discussed. Finally, as a by-product of the investigation, we have obtained interesting results about the form of the field-dependent dielectric constant.


1995 ◽  
Vol 34 (Part 1, No. 8B) ◽  
pp. 4342-4344
Author(s):  
Jonathan P. Bird ◽  
Koji Ishibashi ◽  
Yuichi Ochiai ◽  
Yoshinobu Aoyagi ◽  
Takuo Sugano

2013 ◽  
Vol 26 (3) ◽  
pp. 036002 ◽  
Author(s):  
Chris S Kelley ◽  
James Naughton ◽  
Emma Benson ◽  
Ruth C Bradley ◽  
Vlado K Lazarov ◽  
...  

2010 ◽  
Vol 168-169 ◽  
pp. 173-176
Author(s):  
S.A. Migachev ◽  
M.F. Sadykov ◽  
M.M. Shakirzyanov ◽  
D.A. Ivanov

In a trigonal easy-plane -Fe2O3 antiferromagnet magnetic-field-dependent conic refraction due to the renormalization of the coefficients of elasticity effective magnetoelastic interaction is experimentally found in addition to the conventional internal conic refraction of the transverse elastic waves propagating along the trigonal C3 axis. It is shown that the deflection angle () of the energy flow from the C3 axis upon the internal conic refraction does not depend on the value of the magnetic field applied in the basis plane (HC3) and is a constant value determined by the correlation of the C14 and C44 coefficients of elasticity. The deflection angle of the energy flow upon the antiferromagnetic conic refraction () increases with increase in the field and tends to the  value at large H values. The obtained results agree well with the theory of this phenomenon in antiferromagnets and support its conclusions.


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