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METALS, SUPERCONDUCTORS... 2009Temperature and magnetic field dep<strong>en</strong>d<strong>en</strong>ce of domain wall width and periodof Condon domain structure in AgDiamagnetic instability of electron gas in normal metals underquantizing magnetic field and low temperature is a resultof strong electron correlations induced by the magneticfield. It gives rise to a phase transition with formation ofcomplex domain patterns (Condon domains).hysteresis in magnetization curves, exist<strong>en</strong>ce of persist<strong>en</strong>tcurr<strong>en</strong>ts which results in a discontinuity of magnetic inductionalong the interface boundaries of regular domainpatterns. Still, there remain op<strong>en</strong> fundam<strong>en</strong>tal questionsrelated to the formation of Condon domain phase. As anexample, the important information about the size of thedomains, the domain wall width and surface <strong>en</strong>ergy of theinterface boundaries is still lacking. In our studies [N. Logoboyand W. Joss, Solid State Comm. 149, 2007 (2009)]we offer a way to calculate the expected values of domainwall width and period of the domain structure by means ofmeasurem<strong>en</strong>t of the value of the jump of magnetic inductionat the domain wall δB (figure 99 and figure 100).Figure 99: Temperature dep<strong>en</strong>d<strong>en</strong>ce of the DW width δ (a) andperiod of the domain structure D (b) at the conditions of the experim<strong>en</strong>t[Kramer et al., Phys. Rev. Lett. 95, 267209 (2005)].The solid lines correspond to the theory, the circles are calculatedfrom the temperature dep<strong>en</strong>d<strong>en</strong>ce of the measured jump of magneticinduction at the interface boundaries.The diamagnetic phase transition has received rec<strong>en</strong>tlymuch att<strong>en</strong>tion due to a number of unusual ph<strong>en</strong>om<strong>en</strong>a forthe physics of diamagnetism, e.g. formation of complexbranch structures, strong dep<strong>en</strong>d<strong>en</strong>ce of magnetic phase diagramson Fermi-surface topology, pres<strong>en</strong>ce of diamagneticFigure 100: Magneticfield dep<strong>en</strong>d<strong>en</strong>ce of the DW width δ (a)and period of the domain structure D (b) at the conditions of theexperim<strong>en</strong>t [Kramer et al., Phys. Rev. Lett. 95, 267209 (2005)].The solid lines correspond to the theory, the circles are calculatedfrom the temperature dep<strong>en</strong>d<strong>en</strong>ce of the measured jump of magneticinduction at the interface boundaries.W. JossN. Logoboy (The Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem, Israel and The Instituteof Superconductivity, Departm<strong>en</strong>t of Physics, Bar-Ilan University, Ramat-Gan, Israel)72

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