gauge feelds in condensed matter

Ngày tải lên: 24/04/2014, 17:20

Ngày tải lên: 24/01/2014, 17:36

... theoretical breakthroughs First, Ginzburg and Landau (GL) created a theory describing the transition between the superconducting and the normal phases (Ginzburg and Landau, 1950) It can be noted that, ... (Rajagopal and Wilczek, 2001), (Nardulli, 2002), (Schafer, 2003) and (Casalbuoni and Nardulli, 2003) I found also the following books quite useful (Schrieffer, 1964), (Tinkham, 19...

Ngày tải lên: 24/04/2014, 17:13

Ngày tải lên: 24/04/2014, 17:23

Ngày tải lên: 08/05/2014, 12:51

... explanation without intent to infringe Library of Congress Cataloging -in- Publication Data Weinberger, P (Peter) Magnetic anisotropies in nanostructured matter / Peter Weinberger p cm (Series in condensed ... in turn As an example simply consider the magnetic moments in bulk Fe and for Fe(100) In the bulk case (innite system) in each unit cell the same magnetic moment p...

Ngày tải lên: 04/06/2014, 14:26

... matrix M : ˜ 1 ˜ ˜ U = M J (11 ) By introducing new function according to ˜ ψ0 = , k2 − k2 (12 ) we define the inverse matrix: 1 ˜ ˜ −G0 ˜ 1 ˜ −(ε ε) G1 , M = ψ0 ˜ ˜ −G0 ( μ μ ) 1 G1 ⎞ ⎛ k1 k3 k − ...                     Electromagnetic Waves Propagation in Complex Matter Edited by Ahmed A Kishk Published by InTech Janeza Trdine 9, 510 00 Rijeka, Croatia Copyright © 2 011 InTec...

Ngày tải lên: 19/06/2014, 21:20

... dipole in such a medium was examined and the corresponding radiation patterns were presented  12 Electromagnetic Waves Propagation in Complex Matter Electromagnetic Waves 10 (a) Case ε = (b) View in ... ⎪ ⎩ H = (k2 ez + ∂ ∇) ∂ ∇(m⊥ ψ m ) − ∇ × ∇ × (m⊥ ψ0 ) ∂z ∂z m ψ0 = ψ1 + ( 22 Electromagnetic Waves Propagation in Complex Matter Electromagnetic Waves 2...

Ngày tải lên: 19/06/2014, 21:20

... circuitry-engineering modeling of high-frequency radio-engineering devices and investigation of the propagation of electromagnetic waves in media of intricate geometry in the presence of strong discontinuities ... Isolines Ex (c) Amplitude Ey (d) Isolines Ey Fig Amplitude Ex and isolines, amplitude Ey and isolines of the electromagnetic field strength 39 40 Electromagnetic Wav...

Ngày tải lên: 19/06/2014, 21:20

... without introducing complex parameters In closing, we note that a monochromatic wave is infinite in space and time, has infinitesimal energy absorption in a material medium, and transfers infinitesimal ... 48 Electromagnetic Waves Propagation in Complex Matter appear in the case of going to the complex representation W(t)=U(t)+iV(t) when the real oscillation Е(t) is s...

Ngày tải lên: 19/06/2014, 21:20

... =0.001 -5 -6.0x10 -5 -8.0x10 -5 0 .5 0.3 0 .5 f1=0.7 f1=0.7 f1=0.3 -4 -1.0x10 2. 75 =0.001 QD=0.0 (a)  -5 -4.0x10 0.7 -5 0.3 0 .5 0.0 -2.0x10 5. 0x10 =0.0001 QD=0.0 QD=0.0   -5 2.5x10 -4 8.0x10 ... kG He 5. 5 1.97  1010 rad s-1 kG Table Physical parameters for FeF2 and MnF2 6.0x10 -5 4.0x10 -4 4.0x10 -5 -4 -4 3.0x10 -5 1.5x10 1.0x10 -5 -4 2.0x10 -5 2.0x10 -4 2.0x10...

Ngày tải lên: 19/06/2014, 21:20