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2009 TWO DIMENSIONAL ELECTRON GASSpin splitting <strong>en</strong>hancem<strong>en</strong>t of fully populated Landau levelsThe effect known as “g-factor <strong>en</strong>hancem<strong>en</strong>t” is the promin<strong>en</strong>tmanifestation of electron-electron interactions in thestudy of a two-dim<strong>en</strong>sional electron gas (2DEG) in theregime of the integer quantum Hall effect. This effect isroutinely appar<strong>en</strong>t in magneto-transport experim<strong>en</strong>ts. Theyshow that thermal activation of charged carriers across theFermi <strong>en</strong>ergy located in betwe<strong>en</strong> spin split Landau levels(2DEG at odd filling factors) is ruled by the gap which cansignificantly surpass the so called bare gap expected fromsingle particle band structure models. As far, the effect of g-factor <strong>en</strong>hancem<strong>en</strong>t (at odd filling factors) has be<strong>en</strong> mostlyappar<strong>en</strong>t in experim<strong>en</strong>ts which probed the vicinity of theFermi level. As illustrated in figure. 35, the motivation ofour work was to check whether g-factor is also <strong>en</strong>hancedfor spin split Landau levels located deep below the Fermilevel.We have probed such states with magneto-luminesc<strong>en</strong>ceexperim<strong>en</strong>ts performed on 2DEG confined in aCdTe/CdMgTe quantum well. Focusing on the results oflow temperature experim<strong>en</strong>ts (100 mK) we investigate the<strong>en</strong>ergy positions of σ + and σ − luminesc<strong>en</strong>ce peaks relatedto fully occupied electronic 0th Landau level. The differ<strong>en</strong>ce∆ betwe<strong>en</strong> <strong>en</strong>ergies of these peaks is clearly notmonotonic with the magnetic field in contrast to the lineardep<strong>en</strong>d<strong>en</strong>ce expected wh<strong>en</strong> neglecting the effects ofelectron-electron interactions. As can be deduced fromfigure 36, we find that the oscillatory compon<strong>en</strong>t of ∆ isproportional to the spin polarization of the 2DEG. Notably,∆ = g e f f µ B B wh<strong>en</strong> spin polarization vanishes (at ev<strong>en</strong> fillingfactors). g e f f = 1.3 corresponds well to the combinedelectron-hole bare g-factor in our structure. Effects ofelectron-electron interactions are therefore concluded toaffect the spin splitting of fully occupied Landau levels locateddeep below the Fermi level and not only those in thevicinity of the Fermi <strong>en</strong>ergy.Figure 35: Scheme of Landau levels of a two-dim<strong>en</strong>sional electrongas at ev<strong>en</strong> (6) and odd (5) filling factors. Electron-electroninteraction is known to <strong>en</strong>hance the spin splitting at the Fermi<strong>en</strong>ergy if Landau level filling factor is odd. Enhanced or not<strong>en</strong>hanced spin splitting of fully occupied levels, deep below theFermi level, can be probed with polarization resolved magneto-luminesc<strong>en</strong>ceexperim<strong>en</strong>ts.Figure 36: a,b) Luminesc<strong>en</strong>ce spectra of a 2DEG confined ina 20 nm-wide modulation doped CdTe quantum well at two distinctmagnetic field corresponding to Landau level filling factor 5(a) and 4 (b). Note that spin splitting of the main peak is larger atsmaller field. c) Energy positions of the main σ + and σ − luminesc<strong>en</strong>cepeaks and their separation, ∆ as a function of the magneticfield. Note the increase of ∆ each time the Landau filling is odd.J. Kunc, K. Kowalik, F.J. Teran, P. Plochocka, D.K. Maude, M. PotemskiG. Karczewski, T. Wojtowicz (Institute of Physics, Polish Academy of Sci<strong>en</strong>ces, Warsaw, Poland)29

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