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
TWO-DIMENSIONAL ELECTRON GAS 2009Spin polarisation of a disordered GaAs 2D electron gas in a strong in-planemagnetic fieldAn in-plane magnetic field couples to the spins of a 2Dsystem, and can thus be used to probe the impact of manybody effects on the ground state of the 2D electron gas (2-DEG). For example, the longitudinale resistance under parallelmagnetic field g<strong>en</strong>erally exhibits a saturation or a kinkfor a magnetic field B = B p signaling the complete spin polarizationof the 2D system [T. Okamoto et al., Phys. Rev.Lett. 82, 3875 (1999)].pres<strong>en</strong>t in disordered systems and should under no circumstancesbe interpreted as evid<strong>en</strong>ce for a ferromagnetic instability.Using high magnetic fields up to 32 T, we report on the particularlyrich parallel field physics occurring in 2D electrongas in GaAs, revealing an interplay betwe<strong>en</strong> these spin effects,disorder, and orbital effects. The magneto resistancekink usually associated with the 2-DEG complete spin polarizationis observed up to B p ∼ 30 T, and shifts down continuouslyon more than 20 T as the electron d<strong>en</strong>sity (andconsequ<strong>en</strong>tly mobility) is lowered in the sample (see figure37(a). This reduction of B p with decreasing electrond<strong>en</strong>sity is consist<strong>en</strong>t with the predicted electron-electron interaction<strong>en</strong>hancem<strong>en</strong>t of the spin susceptibility at low d<strong>en</strong>sity,favoring the 2-DEG polarization. However, the absolutevalue of B p remains 2-3 times smaller than the one calculatedat T = 0K for a disorder-free system, and extrapolatesto B p = 0 at a relatively “high” electron d<strong>en</strong>sity, wher<strong>en</strong>o ferromagnetic states have ever be<strong>en</strong> observed. We arguethis behaviour is due to the localization of electrons whichare subsequ<strong>en</strong>tly subtracted from the total free carrier d<strong>en</strong>sity[B.A. Piot et al. Phys. Rev. B 80, 115337 (2009)]. Inthis situation the Fermi sea appears effectively smaller andless magnetic field is required to fully polarize the system.This approach is motivated by the strong mobility dropmeasured as the electron d<strong>en</strong>sity is decreased in this veryregion. The temperature dep<strong>en</strong>d<strong>en</strong>ce of B p , which dep<strong>en</strong>dson the effective size of the Fermi sea, corresponds to thepolarization of a smaller Fermi sea, and indicates that thefraction of localized states increases as the electron d<strong>en</strong>sityis reduced. From this temperature behavior, a d<strong>en</strong>sity of delocalizedelectron can be estimated, and used to re-plot theexperim<strong>en</strong>tal B p of figure 37(b) (triangles), giving a betterquantitative agreem<strong>en</strong>t with theory.In summary, the magnetic field at which complete spin polarizationoccurs is dramatically reduced both by electronlocalization and electron-electron interaction <strong>en</strong>hanced atlow carrier d<strong>en</strong>sity. The large value of the extrapolatedcarrier d<strong>en</strong>sity for full spin polarization at zero magneticfield simply reflects the large number of localized electronsFigure 37: (a) Magneto resistance for differ<strong>en</strong>t electron d<strong>en</strong>sities.(b) Field associated with the complete spin polarization B pas a function of the electron d<strong>en</strong>sity (circles and squares), and asa function of the “corrected” electron d<strong>en</strong>sity (triangles). TheoreticalT = 0 K calculations of the magnetic field for full spin polarizationincluding many-body effects: Random Phase Approximation(RPA) [Y. Zhang and S. D. Sarma, Phys. Rev. Lett. 96,196602 (2006)], and Quantum Monte Carlo Calculation (QMC)[A. L. Subasi and B. Tanatar, Phys. Rev. B 78, 155304 (2008)].B.A. Piot, D. K. MaudeU. G<strong>en</strong>nser, A. Cavanna, D. Mailly (<strong>Laboratoire</strong> de Photonique et de Nanostructures, Marcoussis, France)30
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2009 MAGNETIC SYSTEMSMagnetotranspo
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2009 MAGNETIC SYSTEMSHigh field tor
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2009 MAGNETIC SYSTEMSNuclear magnet
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2009 MAGNETIC SYSTEMSStructural ana
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2009 MAGNETIC SYSTEMSEnhancement ma
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2009 MAGNETIC SYSTEMSInvestigation
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2009 MAGNETIC SYSTEMSField-induced
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2009 MAGNETIC SYSTEMSMagnetic prope
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2009Biology, Chemistry and Soft Mat
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BIOLOGY, CHEMISTRY AND SOFT MATTER
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2009 APPLIED SUPERCONDUCTIVITYMagne
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2009 APPLIED SUPERCONDUCTIVITYPhtha
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2009Magneto-Science105
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MAGNETO-SCIENCE 2009Study of the in
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MAGNETO-SCIENCE 2009Magnetohydrodyn
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MAGNETO-SCIENCE 2009112
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 MAGNET DEVELOPMENT AND INSTRUM
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2009 PROPOSALSProposals for Magnet
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2009 PROPOSALSSpin-Jahn-Teller effe
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2009 PROPOSALSQuantum Oscillations
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2009 PROPOSALSThermoelectric tensor
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2009 PROPOSALSDr. EscoffierCyclotro
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2009 PROPOSALSHigh field magnetotra
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2009 THESESPhD Theses 20091. Nanot
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2009 PUBLICATIONS[21] O. Drachenko,
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2009 PUBLICATIONS[75] S. Nowak, T.
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Contributors of the LNCMI to the Pr
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Institut Jean Lamour, Nancy : 68Ins
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Lawrence Berkeley National Laborato