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Juliana Marques Ramos 1,2 German Thesis Advisor: Reiner Vianden 2 , Brazilian Thesis Advisor: Artur Wilson Carbonari 1 Collaborators: João Guilherme Martins Correia, Rafael Sá de Freitas and ISOLDE collaboration Carrier Mobility and Magnetic Interactions in TiO 2 1 Instituto de Pesquisãs Energéticas e Nucleares, São Paulo University, Brazil 2 Helmholtz-Instituts für Strahlen- und Kernphysik, Bonn University, Germany

Juliana Marques Ramos 1,2 German Thesis Advisor: Reiner Vianden 2, Brazilian Thesis Advisor: Artur Wilson Carbonari 1 Collaborators: João Guilherme Martins

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Juliana Marques Ramos1,2German Thesis Advisor: Reiner Vianden2, Brazilian Thesis Advisor: Artur Wilson Carbonari1

Collaborators: Joo Guilherme Martins Correia, Rafael S de Freitasand ISOLDE collaboration Carrier Mobility and Magnetic Interactions in TiO21Instituto de Pesquiss Energticas e Nucleares, So Paulo University, Brazil2Helmholtz-Instituts fr Strahlen- und Kernphysik, Bonn University, Germany

1Non volatility +Current control trough spin- Increase density of information stored per unit area and the speed of data processing;- Reduces energy consumption;[1] FERT, A. Review of Modern Physics, v. 80 n.4, 1517, 2008.[2] MOLNAR, V. S.; READ, D. New materials for semiconductor spin-electronics.Proceedings of the IEEE. v.91, p.715-726, 2003.[3] WOLF, S. A.;et. al.Spintronics: A Spin-Based Electronics Vision for the Future.Science,v. 294, p-1488-1495, 2001.Current control trough spin + Optic properties- The combination of the two materials in a single chip would function of various devices: - Gather logic, communication skills, collective storage and detection [1]. To magnetic semiconductorsThe control of spin-dependent phenomena in semiconductors can lead to devices such as spin light-emitting diodes (spin-LEDs), spin field effect transistors (spin-FETs) e spin qubits for quantic computers [2, 3]. MotivationFrom magnetic metals...

2Fe dopingCandidate as DMS [1] Defects produced by the dopingCandidate as DMS [1,2]Related works[1] J. M. D. Coey, M. Venkatesan and C. B. Fitzgerald, Nature Materials, 4 (2005) 173.

[2] S. K. S. Patel, S. Kurian, N. S. Gajbhiye, AIP Advances, 2 (2012) 012107.RTFM

The absence of any sextet in fit-derived Mssbauer spectraclearly showed that the ferromagnetic componentin the samples is not due to metallic iron and iron oxide."3Results

Presence of magnetizations saturation as a function of the field; Presence of the hysteresis curve M (H); Low coercive field (applications which require switching) Significant remanent magnetization (non volatile behavior)4Results

Rapid increase of the magnetization at a certain critical temperature; Subtle anomaly near 50 K; The magnetization of a paramagnet also increases when we decreasethe temperature. 5Considerations- Value of coercive field (low) and remanence.- Macroscopic measurements provide only indications of a possible existenceof FM long-range order (not to be confused with FM correlations that occurseven at high temperature). - To be sure of ferromagnetic long-range ordering- Origin of FM: existence of clusters?

carry out neutron diffraction and observe magnetic diffraction peaks.PAC Spectroscopy

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Coincidence

Magnetic interaction:Quadrupole interaction:

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PAC Results: TiO2 + 3% FeProbe nuclei diffused!Sample has still a lot of defects!Vzz ~ 6 x 1021 V/m2 Site 1: ~ 0.2 Site 2: ~ 0.8Site 1: ~ 3 % Site 2: ~ 25 % Site 1: f ~ 40 % Site 2: f ~ 60 %

PAC Results: TiO2 + 3% FeSite 1Site 2Vzz = 6 x 1021 V/m2Vzz = 7 x 1021 V/m2 = 0.28 (0.01) = 0.71 (0.01) = 4 % (0.05) = 20 % (0.08)f = 23 % (2)f = 77 % (7)L = 1,74 (0.13) Mrad/s B = 0,115 TL = 13,6 (1.1) Mrad/s B = 0,925 T13 K27 KSite 1Site 2Vzz = 6 x 1021 V/m2Vzz = 7 x 1021 V/m2 = 0.27 (0.01) = 0.7 (0.01) = 2 % (0.01) = 15 % (0.1)f = 22 % (2.1)f = 80 % (6)L = 1,74 (0.11) Mrad/s B = 0,115 TL = 13,76 (1.01) Mrad/s B = 0,945 T70 K: (too weak)/no magnetic ordering

PAC Results: TiO2

IS 481 PAC Results: TiO2 111mCd

PAC Results: TiO2 181Hf

After the EC decay of the 111In and the following Auger process, the 111Cd atom is in a highly unstable charged state. In semiconductor oxides, depending on the electronic and structural properties of the impurityhost system, the 111Cd probe can trap some electron holes for a time long enough (in the order of ns) to reach the sensitive intermediate state of the 111Cd nuclei.

In the time interval of the PAC coincidence detection, transitions between different charge states out of the equilibrium can occur producing a time-dependent EFG at the 111Cd site.

SummaryRoom temperature ferromagnetismTwo electric quadrupole interactionsWeak magnetism: not applicable in spintronic!Time dependent EFG at 111Cd site

Future WorkX-ray absorption fine structure (EXAFS) measurementsNeutron diffraction: long-range ferromagnetic ordering?To be sure of ferromagnetic long-range ordering we will carry out neutron diffraction and observed magnetic diffraction peaks.

Looking for a Post Doc position

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Reactor team!

Dr. Reiner Vianden

Me! Mr. Marius Arenz IS481: Poster SectionDr. Patrick KesslerThank you! Obrigada! Danke sehr!15