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G. Kioseoglou SEMICONDUCTOR SPINTRONICS George Kioseoglou Materials Science and Technology, University of Crete Spin as new degree of freedom in quantum device structures
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G. Kioseoglou Research Activities Research activities are focused on electrical spin injection and detection of spin polarized electrons into semiconductors. magnetic contacts ZnMnSe Fe FeGa MnGa tunnel barriers Shottky Al 2 O 3 MgO semiconductors GaAs QWs Si InGaAs Quantum Dots Essential Requirements for Spintronics Devices Efficient electrical injection Efficient spin transport Control of spin carriers Effective detection
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G. Kioseoglou MBE growth (NRL) Comprehensive characterization magnetic (SQUID, FMR) transport (Hall, etc) structural (TEM, x-ray diff) composition (XRF) magneto-optical Theory and modeling MBE Growth and characterization
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G. Kioseoglou DMS as a spin contact :ZnMnSe n-ZnMnSe/AlGaAs/GaAs/AlGaAs spin-polarized electron injection giant Zeeman splitting ∆E=g B H g e ~ 30; spin splittings >> kT 100% spin polarized optical polarization GaAs ZnMnSe P circ = I ( +) - I ( -) I ( +) + I ( -) P spin = nn nn - + nn nn P spin = P circ (QWs) P spin = 2 P circ (bulk) PRB62, 8180 (2000)APL79, 3098 (2001)
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G. Kioseoglou Fe based GaAs Spin-LEDs Fe AlGaAs metalsemicond APL82, 4092 (2003) APL80, 1240 (2002) APL84, 4334 (2004) n-AlGaAs i-GaAs p-AlGaAs Fe + - ++ --
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G. Kioseoglou APL91, 122515 (2007) Spin injection from FeGa and MnGa into GaAs APL97, 041103 (2010) FeGa/Al 2 O 3 /GaAs MnGa/Al 2 O 3 /GaAs
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G. Kioseoglou Silicon Spintronics Si / Si-Ge $ 120 Billion - extensive technology - extensive infrastructure Si is an ideal host for SpinS Low spin-orbit scattering is basic material property - low atomic mass - crystal inversion symmetry - low nuclear hyperfine interaction Long spin lifetimes for both donor-bound and free electrons in Si
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G. Kioseoglou Electrical Spin Injection from Fe/Al 2 O 3 & Fe/SiO 2 into Si p-Si(001) substrate 150 nm p-Si 70 nm i-Si 70 nm n-Si Al 2 O 3 10 nm Fe ++ -- B.T. Jonker and G. Kioseoglou Nat. Phys. 3, 542 (2007) G. Kioseoglou et al, APL94, 122106 (2009) C.H. Li et al, APL95, 172101 (2009) P(TA) = 1.7 P(TO)
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G. Kioseoglou Quantifying electron spin polarization from EL direct gap Optical polarization Electron spin polarization ^ T1T1 ^ L ^ T2T2 6 - 8 - 5 1 25' so 7 + 8 + 15 2' indirect gap - the spin pol depends strongly on the phonon branch that mediates the opt transition Huge theoretical effort to understand spin orientation in Si p-type THEORY : P(TA) = 1.6 P(TO) Pengke Li and Hanan Dery, PRL105, 037204 (2010) 13% Experiment:P_TA sub =3.5% Spin injection efficiency 27%
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G. Kioseoglou GaAs InAs 1 nm electrical spin injection up to RT DP mechanism is suppressed Fe based InAs QD Spin-LEDs
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G. Kioseoglou reduced growth rate reduced density increased uniformity in size
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G. Kioseoglou Filling of the electronic shell-states Continuous evolution of shell intensity with bias G. Kioseoglou et al, PRL 101, 227203 (2008)
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G. Kioseoglou Another approach: P vs E Polarization exhibits maxima shifted with respect to intensity shell-peaks due to intershell exchange energy V x sp =7±2 meV V x sp =13.5±1 meV first measurement of the s-p and p-d intershell exchange energies a significant step towards understanding spin-polarized carriers in QDs G. Kioseoglou et al, PRL 101, 227203 (2008)
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G. Kioseoglou IMPACT ZnMnSe/GaAs PRB62, 8180 (2000) Fe/GaAs APL80, 1240 (2002) APL82, 4092 (2003) Fe/Si Nat Physics3, 542 (2007)
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G. Kioseoglou Dr. Jonker (NRL) Dr. Goswami (NRL)-microscopy Prof. Petrou (SUNY Buffalo) Dr. Pawel Hawrylak Quantum Theory Group, Institute for Microstructural Sciences, Ottawa Collaborations Prof. Hanan Dery University of Rochester, NY THEORY
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G. Kioseoglou
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Theory: 2 e-h pairs/QD – S z =-1 Initial state Final state s-p exchange between spin polarized electrons s-shell hole + p-shell elec s-shell exciton σ + The outgoing photon carries the initial-state exchange energy of the spin-polarized electrons
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G. Kioseoglou n-AlGaAs i-GaAs p-AlGaAs Fe + - ++ -- 100 mm
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