Theory of the Galvanomagnetic Effects in Metals with Magnetic Breakdown: Semiclassical Approach

1965 ◽  
Vol 138 (1A) ◽  
pp. A88-A98 ◽  
Author(s):  
L. M. Falicov ◽  
Paul R. Sievert
1973 ◽  
Vol 8 (2) ◽  
pp. 527-535 ◽  
Author(s):  
C. E. T. Goncalves da Silva ◽  
L. M. Falicov

1998 ◽  
Vol 63 (8) ◽  
pp. 1187-1201 ◽  
Author(s):  
Jaroslav Zamastil ◽  
Lubomír Skála ◽  
Petr Pančoška ◽  
Oldřich Bílek

Using the semiclassical approach for the description of the propagation of the electromagnetic waves in optically active isotropic media we derive a new formula for the circular dichroism parameter. The theory is based on the idea of the time damped electromagnetic wave interacting with the molecules of the sample. In this theory, the Lambert-Beer law need not be taken as an empirical law, however, it follows naturally from the requirement that the electromagnetic wave obeys the Maxwell equations.


2002 ◽  
Vol 16 (20n22) ◽  
pp. 3355-3359
Author(s):  
I. MIHUT ◽  
C. C. AGOSTA ◽  
C. H. MIELKE ◽  
M. TOKOMOTO

The magnetic breakdown effect can be seen by the growth of new frequencies in the quantum oscillations in clean metals as a function of magnetic field. We have studied the variation of the amplitudes in the quantum oscillations in the resistance (the Shubnikov-de Haas effect) as a function of angle in the quasi-two dimensional-organic conductor κ-(BEDT-TTF)2Cu(NCS)2. The measurements were made by means of a radio frequency (rf) tank circuit (~ 50 MHz) at very high magnetic fields(50T-60T) and low temperature(500 mK). The geometry of the rf excitation we used excited in-plane currents, and therefore we measured the in-plane resistivity. In contrast to conventional transport measurements that measure the inter-plane resistivity, the in-plane resistivity is dominated by the magnetic breakdown frequencies. As a result we measured much higher breakdown frequency amplitudes than conventional transport experiments. As is expected, the angular dependence of the Shubnikov-de Haas frequencies have a 1/cosθ behavior. This is due to the change of the cross sectional area of the tubular Fermi surface as the angle with respect to the magnetic field is changed. The amplitude of the oscillations changes due to the spin splitting factor which takes into account the ratio between the spin splitting and the energy spacing of the Landau levels which also has 1/cosθ behavior. We show that our data agree with the semi-classical theory (Lifshitz-Kosevich formula).


2007 ◽  
Vol 41 (5) ◽  
pp. 546-549 ◽  
Author(s):  
R. Laiho ◽  
S. A. Nemov ◽  
A. V. Lashkul ◽  
E. Lähderanta ◽  
T. E. Svechnikova ◽  
...  

Physica ◽  
1958 ◽  
Vol 24 ◽  
pp. S174
Author(s):  
Sayed A. Ali ◽  
C.G. Grenier ◽  
J.M. Reynolds

1971 ◽  
Vol 31 (3) ◽  
pp. 768-775 ◽  
Author(s):  
Motohiro Iwami ◽  
Hiroyuki Matsunami ◽  
Tetsuro Tanaka

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