Phys. Status Solidi RRL 5, No. 12, A119 A123 (2011) / DOI /pssr

Size: px
Start display at page:

Download "Phys. Status Solidi RRL 5, No. 12, A119 A123 (2011) / DOI /pssr"

Transcription

1 Phys. Status Solidi RRL 5, No. 12, A119 A123 (2011) / DOI /pssr Full text on our homepage at FRONT COVER Establishing magnetic oxides as spin-selective tunnel barriers on mainstream semiconductors opens up a promising route towards highly efficient spin injection and detection. Europium oxide (EuO) is the only magnetic oxide predicted to be stable in direct contact with silicon. A throughout hard X-ray photoemission spectroscopy study (see the Letter by Caspers et al. on pp ) reveals the nearly ideal stoichiometry of EuO spin filter tunnel barriers grown by Oxide-MBE, with no silicon oxide or silicide formation being observed at the EuO/Si interface. This result clearly demonstrates the successful integration of a magnetic oxide tunnel barrier with silicon, opening up the future integration of magnetic oxides into functional spintronics devices. BACK COVER Eggeling et al. (pp ) investigated the size and magnetic free layer dependence of the vortex dynamics in relatively large spin-valve nanocontacts. A circular nanocontact confines the current flow through a spin-valve multilayer (upper cover image) incorporating a magnetic free layer and an unpinned artificial antiferromagnet as polarizer. Spin-torque driven magnetic vortex dynamics are observed in dependence on the magnetic properties, the contact size and the applied current, provoking microwave oscillations at zero external magnetic field. The oscillation spectra (lower image) show the evolution of single and multiple radio frequency modes as a function of the nanocontact size. These specific properties make spin-torque-driven devices suitable e.g. for nano-sized microwave sources, ultra-compact magnetic field sensors or fast and non-volatile magnetic memories. PREFACE Page A117 A118 S. N. Piramanayagam, Jagadeesh Moodera, Russell Cowburn, and Rachid Sbiaa Focus on Spintronics and Spin Physics NEW IN pss Page A124 Page A125 Page A127 A128 Recent and forthcoming publications in pss Conference calendar Information for authors

2 physica status solidi rrl A120 Page R. Sbiaa, H. Meng, and S. N. Piramanayagam Materials with perpendicular magnetic anisotropy for magnetic random access memory In this Review, the princple of spin-transfer torque magnetic random access memory (STT-MRAM) is explained: The magnetic tunnel junction device is sandwiched between two electrodes (cross-point architecture). The writing is based on the spin torque effect and the reading on tunnelling magnetoresistive effect. In contrast to field-based MRAM, the STT-MRAM does not require an external magnetic field. Since STT-MRAM is scalable, the transistor scales down with the device size. Materials with perpendicular magnetic anisotropy (PMA) are being investigated for their use in STT-MRAM multilayers such as Co/Pd and Co/Pt as well as FeCoB and future candidates such as FePt. RAPID RESEARCH LETTERS Page Alexander Makarov, Viktor Sverdlov, Dmitry Osintsev, and Siegfried Selberherr Reduction of switching time in pentalayer magnetic tunnel junctions with a composite free layer In this Letter the authors report a substantial decrease of the switching time in a pentalayer structure with a composite-free layer as compared to the pentalayer structure of similar dimensions with a monolithic free layer. The physical reasons for the switching time reduction at the same current density are discussed. Page Sylvain D. Brechet and Jean-Philippe Ansermet Heat-driven spin currents on large scales Brechet and Ansermet show that a three-current model of heat, spin-up and spin-down currents predicts the spin polarisation current to exist on large scales and to be proportional to the temperature gradient, corresponding to a spin Soret effect. They establish the existence of the spin current driven by a heat current over large distances in the absence of a charge current and at equilibrium of the spin channels. Thus, a heat current may also affect the magnetisation.

3 Phys. Status Solidi RRL 5, No. 12 (2011) A121 Page Taiebeh Tahmasebi, Seidikkurippu N. Piramanayagam, Rachid Sbiaa, Hang Khume Tan, Randall Law, Sunny Lua, and Tow Chong Chong Tailoring the growth of L1 0 -FePt for spintronics applications Ordered L1 0 -FePt with large magnetocrystalline anisotropy (K u ) and high saturation magnetization (M s ) enables potential scaling of spintronic devices down to 5 nm. FePt films need to be smooth and possess good (001) texture in order to achieve the desired properties for spintronics applications. This Letter focuses on the tailoring of L1 0 -FePt growth for such applications. The L1 0 -FePt magnetic layers deposited on Pd seed layers exhibit large ordering parameter, smoothness and strong perpendicular magnetic anisotropy. Page Sophie A. Morley, Nicholas A. Porter, and Christopher H. Marrows Magnetism and magnetotransport in sputtered Co-doped FeSi films Microelectronics manufacturing relies on planar processing for which thin films are needed. Sputtered films of cobaltdoped iron monosilicide have been fabricated and characterised. The non-centrosymmetric ε-phase is the predominant form of the material after annealing. It shows similar magnetic and magnetotransport properties to bulk single crystals in spite of the inherent disorder in a thin film. This includes a ratio of magnetic moment to carrier density of approximately unity, suggesting a high spin-polarisation in this silicon-based material. Page S. M. Mohseni, S. R. Sani, J. Persson, T. N. Anh Nguyen, S. Chung, Ye. Pogoryelov, and Johan Åkerman High frequency operation of a spin-torque oscillator at low field In this Letter the authors demonstrate a nanocontact spin-torque oscillator (STO) based on an orthogonal spinvalve architecture with an in-plane Co polarizer and an out-of-plane Co/Ni multilayer free layer. High frequency operation at low external fields is achieved by tailoring the Co/Ni layer properties to increase the strength of the perpendicular magnetic anisotropy, while simultaneously reducing the saturation magnetization.

4 physica status solidi rrl A122 Page Moritz Eggeling, Theodoros Dimopoulos, Rudolf Heer, and Hubert Brückl Magnetic vortex excitation dependence on the magnetic free layer and size of spin-valve nanocontacts Spin-torque-driven vortex-oscillators can be applied as nano-sized microwave sources, ultra-compact magnetic field sensors or in fast and non-volatile magnetic memories. This Letter demonstrates the dependence of vortex dynamics on the free layer and the size of relatively large spin-valve nanocontacts, incorporating an unpinned artificial antiferromagnet. Nucleation current density, multiple mode excitation and magnetic field dependence are specifically addressed. Page Michael Lorenz, Matthias Brandt, Katja Mexner, Kerstin Brachwitz, Michael Ziese, Pablo Esquinazi, Holger Hochmuth, and Marius Grundmann Ferrimagnetic ZnFe 2 O 4 thin films on SrTiO 3 single crystals with highly tunable electrical conductivity Within the current search for spintronic materials with spin polarized conductivity, zinc ferrite (ZnFe 2 O 4 ) thin films grown on SrTiO 3 (001) and (111) single crystals are highly promising as magnetic semiconducting electrode in advanced all-oxide tunnel junctions and field effect transistors, as well as insulating barrier in spin filters. This is due to the highly tunable electrical conductivity coupled with high saturation magnetization. Page C. Caspers, M. Müller, A. X. Gray, A. M. Kaiser, A. Gloskovskii, C. S. Fadley, W. Drube, and C. M. Schneider Electronic structure of EuO spin filter tunnel contacts directly on silicon Hard X-ray photoemission spectroscopy reveals the nearly ideal stoichiometry of EuO spin filter tunnel barriers grown directly on silicon, and the absence of silicon oxide formation at the EuO/Si interface. These results demonstrate the successful integration of a magnetic oxide tunnel barrier with silicon, paving the way for the future integration of magnetic oxides into functional spintronics devices.

5 Phys. Status Solidi RRL 5, No. 12 (2011) A123 Page M. Ziese A spin-calorics device based on La 0.7 Sr 0.3 MnO 3 /SrRuO 3 superlattices In this Letter a spin-caloric device is proposed that consists of a wedge-shaped La 0.7 Sr 0.3 MnO 3 /SrRuO 3 superlattice (SL). Studies of SLs with various layer thicknesses show that the magnetic work can be strongly influenced by the engineering of the crystalline symmetry or the use of exchange biasing. A SL wedge in a rapidly varying magnetic field should therefore support a self-sustained Seebeck effect. Page H. S. Hsu, Y. Tung, Y. J. Chen, M. G. Chen, J. S. Lee, and S. J. Sun Defect engineering of room-temperature ferromagnetism of carbon-doped ZnO Room-temperature ferromagnetism observed in an air-annealed C:ZnO sample was associated with a ferromagnetic magnetic circular dichroism peak. This is related to the loss of carbon and the creation of defects in an air-annealed C:ZnO film by the reaction between carbon dopants and oxygen. In this Letter the authors suggest that a combination of carbon doping and a suitable post-annealing treatment has a strong impact on the defect-mediated ferromagnetism of C:ZnO. Page N. Sedlmayr, V. K. Dugaev, M. Inglot, and J. Berakdar Indirect interaction of magnetic domain walls E(R,q) mev q=p/4 q=p In this Letter the authors calculate the carrier-mediated interaction between domain walls in a ferromagnetic strip. The result is an oscillating function of both the interdomain wall distance and their relative orientations. Sedlmayr et al. go on to show how this can give rise to spiralling domain wall orientations in a strip. Such an interaction can have consequences for any tightly packed wire of domain walls R/l physica status solidi (RRL) is indexed in Cambridge Scientific Abstracts (CSA); Chemical Abstracts Service/ SciFinder (ACS); Current /Physical, Chemical & Earth Sciences, Materials Science Citation Index, Science Citation Index, Science Citation Index Expanded, Web of Science (Thomson ISI); FIZ Karlsruhe Databases (FIZ Karlsruhe); INSPEC (IET); SCOPUS (Elsevier); VINITI (All-Russian Institute of Science & Technological Information).

Wouldn t it be great if

Wouldn t it be great if IDEMA DISKCON Asia-Pacific 2009 Spin Torque MRAM with Perpendicular Magnetisation: A Scalable Path for Ultra-high Density Non-volatile Memory Dr. Randall Law Data Storage Institute Agency for Science Technology

More information

MAGNETORESISTANCE PHENOMENA IN MAGNETIC MATERIALS AND DEVICES. J. M. De Teresa

MAGNETORESISTANCE PHENOMENA IN MAGNETIC MATERIALS AND DEVICES. J. M. De Teresa MAGNETORESISTANCE PHENOMENA IN MAGNETIC MATERIALS AND DEVICES J. M. De Teresa Instituto de Ciencia de Materiales de Aragón, Universidad de Zaragoza-CSIC, Facultad de Ciencias, 50009 Zaragoza, Spain. E-mail:

More information

Perpendicular MTJ stack development for STT MRAM on Endura PVD platform

Perpendicular MTJ stack development for STT MRAM on Endura PVD platform Perpendicular MTJ stack development for STT MRAM on Endura PVD platform Mahendra Pakala, Silicon Systems Group, AMAT Dec 16 th, 2014 AVS 2014 *All data in presentation is internal Applied generated data

More information

Giant Magnetoresistance

Giant Magnetoresistance Giant Magnetoresistance This is a phenomenon that produces a large change in the resistance of certain materials as a magnetic field is applied. It is described as Giant because the observed effect is

More information

Spin Lifetime Enhancement by Shear Strain in Thin Silicon-on-Insulator Films. Dmitry Osintsev, Viktor Sverdlov, and Siegfried Selberherr

Spin Lifetime Enhancement by Shear Strain in Thin Silicon-on-Insulator Films. Dmitry Osintsev, Viktor Sverdlov, and Siegfried Selberherr 10.1149/05305.0203ecst The Electrochemical Society Spin Lifetime Enhancement by Shear Strain in Thin Silicon-on-Insulator Films Dmitry Osintsev, Viktor Sverdlov, and Siegfried Selberherr Institute for

More information

TRANSVERSE SPIN TRANSPORT IN GRAPHENE

TRANSVERSE SPIN TRANSPORT IN GRAPHENE International Journal of Modern Physics B Vol. 23, Nos. 12 & 13 (2009) 2641 2646 World Scientific Publishing Company TRANSVERSE SPIN TRANSPORT IN GRAPHENE TARIQ M. G. MOHIUDDIN, A. A. ZHUKOV, D. C. ELIAS,

More information

The Physics of Ferromagnetism

The Physics of Ferromagnetism Terunobu Miyazaki Hanmin Jin The Physics of Ferromagnetism Springer Contents Part I Foundation of Magnetism 1 Basis of Magnetism 3 1.1 Basic Magnetic Laws and Magnetic Quantities 3 1.1.1 Basic Laws of

More information

Spin caloritronics in magnetic/non-magnetic nanostructures and graphene field effect devices Dejene, Fasil

Spin caloritronics in magnetic/non-magnetic nanostructures and graphene field effect devices Dejene, Fasil University of Groningen Spin caloritronics in magnetic/non-magnetic nanostructures and graphene field effect devices Dejene, Fasil DOI: 10.1038/nphys2743 IMPORTANT NOTE: You are advised to consult the

More information

MatSci 224 Magnetism and Magnetic. November 5, 2003

MatSci 224 Magnetism and Magnetic. November 5, 2003 MatSci 224 Magnetism and Magnetic Materials November 5, 2003 How small is small? What determines whether a magnetic structure is made of up a single domain or many domains? d Single domain d~l d d >> l

More information

Center for Spintronic Materials, Interfaces, and Novel Architectures. Voltage Controlled Antiferromagnetics and Future Spin Memory

Center for Spintronic Materials, Interfaces, and Novel Architectures. Voltage Controlled Antiferromagnetics and Future Spin Memory Center for Spintronic Materials, Interfaces, and Novel Architectures Voltage Controlled Antiferromagnetics and Future Spin Memory Maxim Tsoi The University of Texas at Austin Acknowledgments: H. Seinige,

More information

Contents. Acknowledgments

Contents. Acknowledgments MAGNETIC MATERIALS Fundamentals and Applications Second edition NICOLA A. SPALDIN University of California, Santa Barbara CAMBRIDGE UNIVERSITY PRESS Contents Acknowledgments page xiii I Basics 1 Review

More information

Ferromagnetism and Electronic Transport. Ordinary magnetoresistance (OMR)

Ferromagnetism and Electronic Transport. Ordinary magnetoresistance (OMR) Ferromagnetism and Electronic Transport There are a number of effects that couple magnetization to electrical resistance. These include: Ordinary magnetoresistance (OMR) Anisotropic magnetoresistance (AMR)

More information

Solid Surfaces, Interfaces and Thin Films

Solid Surfaces, Interfaces and Thin Films Hans Lüth Solid Surfaces, Interfaces and Thin Films Fifth Edition With 427 Figures.2e Springer Contents 1 Surface and Interface Physics: Its Definition and Importance... 1 Panel I: Ultrahigh Vacuum (UHV)

More information

Mon., Feb. 04 & Wed., Feb. 06, A few more instructive slides related to GMR and GMR sensors

Mon., Feb. 04 & Wed., Feb. 06, A few more instructive slides related to GMR and GMR sensors Mon., Feb. 04 & Wed., Feb. 06, 2013 A few more instructive slides related to GMR and GMR sensors Oscillating sign of Interlayer Exchange Coupling between two FM films separated by Ruthenium spacers of

More information

Planar Hall Effect in Magnetite (100) Films

Planar Hall Effect in Magnetite (100) Films Planar Hall Effect in Magnetite (100) Films Xuesong Jin, Rafael Ramos*, Y. Zhou, C. McEvoy and I.V. Shvets SFI Nanoscience Laboratories, School of Physics, Trinity College Dublin, Dublin 2, Ireland 1 Abstract.

More information

Advanced Lab Course. Tunneling Magneto Resistance

Advanced Lab Course. Tunneling Magneto Resistance Advanced Lab Course Tunneling Magneto Resistance M06 As of: 015-04-01 Aim: Measurement of tunneling magnetoresistance for different sample sizes and recording the TMR in dependency on the voltage. Content

More information

What so special about LaAlO3/SrTiO3 interface? Magnetism, Superconductivity and their coexistence at the interface

What so special about LaAlO3/SrTiO3 interface? Magnetism, Superconductivity and their coexistence at the interface What so special about LaAlO3/SrTiO3 interface? Magnetism, Superconductivity and their coexistence at the interface Pramod Verma Indian Institute of Science, Bangalore 560012 July 24, 2014 Pramod Verma

More information

Mesoscopic Spintronics

Mesoscopic Spintronics Mesoscopic Spintronics Taro WAKAMURA (Université Paris-Sud) Lecture 1 Today s Topics 1.1 History of Spintronics 1.2 Fudamentals in Spintronics Spin-dependent transport GMR and TMR effect Spin injection

More information

Physics Coral Gables, Florida 33124, USA

Physics Coral Gables, Florida 33124, USA Physics Coral Gables, Florida 33124, USA The Spin Battery barnes@physics.miami.edu Spin Battery Spin battery S. E. Barnes and S. Maekawa Phys. Rev. Lett. 98 246601 (2007) Except for solar cells, the generation

More information

From Spin Torque Random Access Memory to Spintronic Memristor. Xiaobin Wang Seagate Technology

From Spin Torque Random Access Memory to Spintronic Memristor. Xiaobin Wang Seagate Technology From Spin Torque Random Access Memory to Spintronic Memristor Xiaobin Wang Seagate Technology Contents Spin Torque Random Access Memory: dynamics characterization, device scale down challenges and opportunities

More information

Recent developments in spintronic

Recent developments in spintronic Recent developments in spintronic Tomas Jungwirth nstitute of Physics ASCR, Prague University of Nottingham in collaboration with Hitachi Cambridge, University of Texas, Texas A&M University - Spintronics

More information

Current-driven Magnetization Reversal in a Ferromagnetic Semiconductor. (Ga,Mn)As/GaAs/(Ga,Mn)As Tunnel Junction

Current-driven Magnetization Reversal in a Ferromagnetic Semiconductor. (Ga,Mn)As/GaAs/(Ga,Mn)As Tunnel Junction Current-driven Magnetization Reversal in a Ferromagnetic Semiconductor (Ga,Mn)As/GaAs/(Ga,Mn)As Tunnel Junction D. Chiba 1, 2*, Y. Sato 1, T. Kita 2, 1, F. Matsukura 1, 2, and H. Ohno 1, 2 1 Laboratory

More information

2D MBE Activities in Sheffield. I. Farrer, J. Heffernan Electronic and Electrical Engineering The University of Sheffield

2D MBE Activities in Sheffield. I. Farrer, J. Heffernan Electronic and Electrical Engineering The University of Sheffield 2D MBE Activities in Sheffield I. Farrer, J. Heffernan Electronic and Electrical Engineering The University of Sheffield Outline Motivation Van der Waals crystals The Transition Metal Di-Chalcogenides

More information

J 12 J 23 J 34. Driving forces in the nano-magnetism world. Intra-atomic exchange, electron correlation effects: Inter-atomic exchange: MAGNETIC ORDER

J 12 J 23 J 34. Driving forces in the nano-magnetism world. Intra-atomic exchange, electron correlation effects: Inter-atomic exchange: MAGNETIC ORDER Driving forces in the nano-magnetism world Intra-atomic exchange, electron correlation effects: LOCAL (ATOMIC) MAGNETIC MOMENTS m d or f electrons Inter-atomic exchange: MAGNETIC ORDER H exc J S S i j

More information

Page 1. A portion of this study was supported by NEDO.

Page 1. A portion of this study was supported by NEDO. MRAM : Materials and Devices Current-induced Domain Wall Motion High-speed MRAM N. Ishiwata NEC Corporation Page 1 A portion of this study was supported by NEDO. Outline Introduction Positioning and direction

More information

Spin orbit torque driven magnetic switching and memory. Debanjan Bhowmik

Spin orbit torque driven magnetic switching and memory. Debanjan Bhowmik Spin orbit torque driven magnetic switching and memory Debanjan Bhowmik Spin Transfer Torque Fixed Layer Free Layer Fixed Layer Free Layer Current coming out of the fixed layer (F2) is spin polarized in

More information

Observation of magnetization alignment switching in Fe3Si/FeSi2 artificial lattices by polarized neutron reflection

Observation of magnetization alignment switching in Fe3Si/FeSi2 artificial lattices by polarized neutron reflection Proc. Int. Conf. and Summer School on Advanced Silicide Technology 2014 JJAP Conf. Proc. 3 (2015) 011503 2015 The Japan Society of Applied Physics Observation of magnetization alignment switching in Fe3Si/FeSi2

More information

Ferromagnetism and Anomalous Hall Effect in Graphene

Ferromagnetism and Anomalous Hall Effect in Graphene Ferromagnetism and Anomalous Hall Effect in Graphene Jing Shi Department of Physics & Astronomy, University of California, Riverside Graphene/YIG Introduction Outline Proximity induced ferromagnetism Quantized

More information

From Hall Effect to TMR

From Hall Effect to TMR From Hall Effect to TMR 1 Abstract This paper compares the century old Hall effect technology to xmr technologies, specifically TMR (Tunnel Magneto-Resistance) from Crocus Technology. It covers the various

More information

introduction: what is spin-electronics?

introduction: what is spin-electronics? Spin-dependent transport in layered magnetic metals Patrick Bruno Max-Planck-Institut für Mikrostrukturphysik, Halle, Germany Summary: introduction: what is spin-electronics giant magnetoresistance (GMR)

More information

A Comparative Study on the Differences in the Evolutions of Thin Film Morphologies of Co-Al Binary System: Molecular Dynamics Study

A Comparative Study on the Differences in the Evolutions of Thin Film Morphologies of Co-Al Binary System: Molecular Dynamics Study Mat. Res. Soc. Symp. Proc. Vol. 777 2003 Materials Research Society T8.10.1 A Comparative Study on the Differences in the Evolutions of Thin Film Morphologies of Co-Al Binary System: Molecular Dynamics

More information

Recent Developments in Magnetoelectrics Vaijayanti Palkar

Recent Developments in Magnetoelectrics Vaijayanti Palkar Recent Developments in Magnetoelectrics Vaijayanti Palkar Department of Condensed Matter Physics & Materials Science Tata Institute of Fundamental Research Mumbai 400 005, India. Tata Institute of Fundamental

More information

MSE 7025 Magnetic Materials (and Spintronics)

MSE 7025 Magnetic Materials (and Spintronics) MSE 7025 Magnetic Materials (and Spintronics) Lecture 14: Spin Transfer Torque And the future of spintronics research Chi-Feng Pai cfpai@ntu.edu.tw Course Outline Time Table Week Date Lecture 1 Feb 24

More information

The exchange interaction between FM and AFM materials

The exchange interaction between FM and AFM materials Chapter 1 The exchange interaction between FM and AFM materials When the ferromagnetic (FM) materials are contacted with antiferromagnetic (AFM) materials, the magnetic properties of FM materials are drastically

More information

arxiv: v1 [cond-mat.mtrl-sci] 28 Jul 2008

arxiv: v1 [cond-mat.mtrl-sci] 28 Jul 2008 Current induced resistance change of magnetic tunnel junctions with ultra-thin MgO tunnel barriers Patryk Krzysteczko, 1, Xinli Kou, 2 Karsten Rott, 1 Andy Thomas, 1 and Günter Reiss 1 1 Bielefeld University,

More information

Mesoscopic Spintronics

Mesoscopic Spintronics Mesoscopic Spintronics Taro WAKAMURA (Université Paris-Sud) Lecture 5 Today s Topics 5.1 Spincaloritronics 5.2 Domain walls and skyrmions Spin Caloritronics Basics of thermoelectric effects The gradient

More information

Ferromagnetism. In free space, the flux density and magnetizing field strength are related by the expression

Ferromagnetism. In free space, the flux density and magnetizing field strength are related by the expression 1 Ferromagnetism B In free space, the flux density and magnetizing field strength are related by the expression H B =µ 0 H µ 0 =4π x 10-7 H.m -1, the permeability of free space. 2 Ferromagnetism B H For

More information

Directions for simulation of beyond-cmos devices. Dmitri Nikonov, George Bourianoff, Mark Stettler

Directions for simulation of beyond-cmos devices. Dmitri Nikonov, George Bourianoff, Mark Stettler Directions for simulation of beyond-cmos devices Dmitri Nikonov, George Bourianoff, Mark Stettler Outline Challenges and responses in nanoelectronic simulation Limits for electronic devices and motivation

More information

Chapter 103 Spin-Polarized Scanning Tunneling Microscopy

Chapter 103 Spin-Polarized Scanning Tunneling Microscopy Chapter 103 Spin-Polarized Scanning Tunneling Microscopy Toyo Kazu Yamada Keywords Spin-polarized tunneling current Spin polarization Magnetism 103.1 Principle Spin-polarized scanning tunneling microscopy

More information

Unclassified Unclassified Unclassified UL Standard Form 2981Rev. 2-89) (EG)

Unclassified Unclassified Unclassified UL Standard Form 2981Rev. 2-89) (EG) REPORT DOCUMENTATION PAGE 1 Form Approved R R OMB No. 0704-0188 Public reporting burden for this collection of information is estimated to average 1 hour per response, including the time for reviewing

More information

Electronic and Optoelectronic Properties of Semiconductor Structures

Electronic and Optoelectronic Properties of Semiconductor Structures Electronic and Optoelectronic Properties of Semiconductor Structures Jasprit Singh University of Michigan, Ann Arbor CAMBRIDGE UNIVERSITY PRESS CONTENTS PREFACE INTRODUCTION xiii xiv 1.1 SURVEY OF ADVANCES

More information

Giant Magnetoresistance

Giant Magnetoresistance Giant Magnetoresistance N. Shirato urse: Solid State Physics 2, Spring 2010, Instructor: Dr. Elbio Dagotto Department of Materials Science and Engineering, University of Tennessee, Knoxville, TN 37996

More information

Spin-resolved photoelectron spectroscopy

Spin-resolved photoelectron spectroscopy Spin-resolved photoelectron spectroscopy Application Notes Spin-resolved photoelectron spectroscopy experiments were performed in an experimental station consisting of an analysis and a preparation chamber.

More information

Challenges and Opportunities. Prof. J. Raynien Kwo 年

Challenges and Opportunities. Prof. J. Raynien Kwo 年 Nanoelectronics Beyond Si: Challenges and Opportunities Prof. J. Raynien Kwo 年 立 Si CMOS Device Scaling Beyond 22 nm node High κ,, Metal gates, and High mobility channel 1947 First Transistor 1960 1960

More information

VALLIAMMAI ENGINEERING COLLEGE

VALLIAMMAI ENGINEERING COLLEGE VALLIAMMAI ENGINEERING COLLEGE SRM Nagar, Kattankulathur 603 203 DEPARTMENT OF PHYSICS QUESTION BANK II SEMESTER PH8252 - PHYSICS FOR INFORMATION SCIENCE (Common to CSE & IT) Regulation 2017 Academic Year

More information

Magnetically Engineered Spintronic Sensors and Memory

Magnetically Engineered Spintronic Sensors and Memory Magnetically Engineered Spintronic Sensors and Memory STUART PARKIN, SENIOR MEMBER, IEEE, XIN JIANG, CHRISTIAN KAISER, ALEX PANCHULA, KEVIN ROCHE, AND MAHESH SAMANT Invited Paper The discovery of enhanced

More information

Challenges for Materials to Support Emerging Research Devices

Challenges for Materials to Support Emerging Research Devices Challenges for Materials to Support Emerging Research Devices C. Michael Garner*, James Hutchby +, George Bourianoff*, and Victor Zhirnov + *Intel Corporation Santa Clara, CA + Semiconductor Research Corporation

More information

A comparison study on hydrogen sensing performance of Pt/MoO3 nanoplatelets coated with a thin layer of Ta2O5 or La2O3

A comparison study on hydrogen sensing performance of Pt/MoO3 nanoplatelets coated with a thin layer of Ta2O5 or La2O3 Title Author(s) Citation A comparison study on hydrogen sensing performance of Pt/MoO3 nanoplatelets coated with a thin layer of Ta2O5 or La2O3 Yu, J; Liu, Y; Cai, FX; Shafiei, M; Chen, G; Motta, N; Wlodarski,

More information

Giant Magnetoresistance

Giant Magnetoresistance GENERAL ARTICLE Giant Magnetoresistance Nobel Prize in Physics 2007 Debakanta Samal and P S Anil Kumar The 2007 Nobel Prize in Physics was awarded to Albert Fert and Peter Grünberg for the discovery of

More information

Influence of exchange bias on magnetic losses in CoFeB/MgO/CoFeB tunnel junctions

Influence of exchange bias on magnetic losses in CoFeB/MgO/CoFeB tunnel junctions Influence of exchange bias on magnetic losses in CoFeB/MgO/CoFeB tunnel junctions Ryan Stearrett Ryan Stearrett, W. G. Wang, Xiaoming Kou, J. F. Feng, J. M. D. Coey, J. Q. Xiao, and E. R. Nowak, Physical

More information

Data Storage Institute, A*STAR (Agency for Science, Technology and Research), 5 Engineering Drive 1, Singapore

Data Storage Institute, A*STAR (Agency for Science, Technology and Research), 5 Engineering Drive 1, Singapore Phys. Status Solidi RRL 5, No. 12, 413 419 (2011) / DOI 10.1002/pssr.201105420 pss Materials with perpendicular magnetic anisotropy for magnetic random access memory Review@RRL R. Sbiaa *, H. Meng, and

More information

(a) (b) Supplementary Figure 1. (a) (b) (a) Supplementary Figure 2. (a) (b) (c) (d) (e)

(a) (b) Supplementary Figure 1. (a) (b) (a) Supplementary Figure 2. (a) (b) (c) (d) (e) (a) (b) Supplementary Figure 1. (a) An AFM image of the device after the formation of the contact electrodes and the top gate dielectric Al 2 O 3. (b) A line scan performed along the white dashed line

More information

MAGNETO-RESISTANCE AND INDUCED DOMAIN STRUCTURE IN TUNNEL JUNCTIONS

MAGNETO-RESISTANCE AND INDUCED DOMAIN STRUCTURE IN TUNNEL JUNCTIONS Mat. Res. Soc. Symp. Proc. Vol. 674 001 Materials Research Society MAGNETO-RESISTANCE AND INDUCED DOMAIN STRUCTURE IN TUNNEL JUNCTIONS M. Hehn, O. Lenoble, D. Lacour and A. Schuhl Laboratoire de Physique

More information

0.002 ( ) R xy

0.002 ( ) R xy a b z 0.002 x H y R xy () 0.000-0.002 0 90 180 270 360 (degree) Supplementary Figure 1. Planar Hall effect resistance as a function of the angle of an in-plane field. a, Schematic of the planar Hall resistance

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION DOI: 10.1038/NNANO.2014.16 Electrical detection of charge current-induced spin polarization due to spin-momentum locking in Bi 2 Se 3 by C.H. Li, O.M.J. van t Erve, J.T. Robinson,

More information

Universal valence-band picture of. the ferromagnetic semiconductor GaMnAs

Universal valence-band picture of. the ferromagnetic semiconductor GaMnAs Universal valence-band picture of the ferromagnetic semiconductor GaMnAs Shinobu Ohya *, Kenta Takata, and Masaaki Tanaka Department of Electrical Engineering and Information Systems, The University of

More information

Influence of Size on the Properties of Materials

Influence of Size on the Properties of Materials Influence of Size on the Properties of Materials M. J. O Shea Kansas State University mjoshea@phys.ksu.edu If you cannot get the papers connected to this work, please e-mail me for a copy 1. General Introduction

More information

Saroj P. Dash. Chalmers University of Technology. Göteborg, Sweden. Microtechnology and Nanoscience-MC2

Saroj P. Dash. Chalmers University of Technology. Göteborg, Sweden. Microtechnology and Nanoscience-MC2 Silicon Spintronics Saroj P. Dash Chalmers University of Technology Microtechnology and Nanoscience-MC2 Göteborg, Sweden Acknowledgement Nth Netherlands University of Technology Sweden Mr. A. Dankert Dr.

More information

Cover Page. The handle holds various files of this Leiden University dissertation

Cover Page. The handle   holds various files of this Leiden University dissertation Cover Page The handle http://hdl.handle.net/1887/24306 holds various files of this Leiden University dissertation Author: Verhagen, T.G.A. Title: Magnetism and magnetization dynamics in thin film ferromagnets

More information

From nanophysics research labs to cell phones. Dr. András Halbritter Department of Physics associate professor

From nanophysics research labs to cell phones. Dr. András Halbritter Department of Physics associate professor From nanophysics research labs to cell phones Dr. András Halbritter Department of Physics associate professor Curriculum Vitae Birth: 1976. High-school graduation: 1994. Master degree: 1999. PhD: 2003.

More information

Semiconductor industry.

Semiconductor industry. Semiconductor industry www.theiet.org/inspec Inspec the premier source for semiconductor research The Inspec Database has nearly 11 million records in total, containing abstracts and indexing to global

More information

Temperature dependence of spin diffusion length in silicon by Hanle-type spin. precession

Temperature dependence of spin diffusion length in silicon by Hanle-type spin. precession Temperature dependence of spin diffusion length in silicon by Hanle-type spin precession T. Sasaki 1,a), T. Oikawa 1, T. Suzuki 2, M. Shiraishi 3, Y. Suzuki 3, and K. Noguchi 1 SQ Research Center, TDK

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Engineered doping of organic semiconductors for enhanced thermoelectric efficiency G.-H. Kim, 1 L. Shao, 1 K. Zhang, 1 and K. P. Pipe 1,2,* 1 Department of Mechanical Engineering, University of Michigan,

More information

Semiconductor Physical Electronics

Semiconductor Physical Electronics Semiconductor Physical Electronics Sheng S. Li Department of Electrical Engineering University of Florida Gainesville, Florida Plenum Press New York and London Contents CHAPTER 1. Classification of Solids

More information

arxiv: v1 [physics.app-ph] 1 May 2017

arxiv: v1 [physics.app-ph] 1 May 2017 Magnetic Skyrmions for Cache Memory Mei-Chin Chen 1 and Kaushik Roy 1 1 School of Electrical and Computer Engineering, Purdue University, West Lafayette, 47906, USA * chen1320@purdue.edu ABSTRACT arxiv:1705.01095v1

More information

Designing Magnetic Droplet Soliton Nucleation Employing Spin Polarizer

Designing Magnetic Droplet Soliton Nucleation Employing Spin Polarizer Designing Magnetic Droplet Soliton Nucleation Employing Spin Polarizer Morteza Mohseni 1, and Majid Mohseni 1,* 1 Faculty of Physics, Shahid Beheshti University, Evin, 19839 Tehran, Iran Abstract We show

More information

Low Energy Spin Transfer Torque RAM (STT-RAM / SPRAM) Zach Foresta April 23, 2009

Low Energy Spin Transfer Torque RAM (STT-RAM / SPRAM) Zach Foresta April 23, 2009 Low Energy Spin Transfer Torque RAM (STT-RAM / SPRAM) Zach Foresta April 23, 2009 Overview Background A brief history GMR and why it occurs TMR structure What is spin transfer? A novel device A future

More information

Introduction to magnetic recording + recording materials

Introduction to magnetic recording + recording materials Introduction to magnetic recording + recording materials Laurent Ranno Institut Néel, Nanoscience Dept, CNRS-UJF, Grenoble, France I will give two lectures about magnetic recording. In the first one, I

More information

Low dimensional magnetism Experiments

Low dimensional magnetism Experiments Low dimensional magnetism Experiments Olivier Fruchart Brasov (Romania), Sept. 2003 1 Introduction...................................... 2 2 Ferromagnetic order................................. 2 2.1 Methods.....................................

More information

ECE 340 Lecture 39 : MOS Capacitor II

ECE 340 Lecture 39 : MOS Capacitor II ECE 340 Lecture 39 : MOS Capacitor II Class Outline: Effects of Real Surfaces Threshold Voltage MOS Capacitance-Voltage Analysis Things you should know when you leave Key Questions What are the effects

More information

Black phosphorus: A new bandgap tuning knob

Black phosphorus: A new bandgap tuning knob Black phosphorus: A new bandgap tuning knob Rafael Roldán and Andres Castellanos-Gomez Modern electronics rely on devices whose functionality can be adjusted by the end-user with an external knob. A new

More information

Antiferromagnetic Spintronics

Antiferromagnetic Spintronics Lecture II Antiferromagnetic Spintronics Alireza Qaiumzadeh Radboud University (RU) Institute for Molecules and Materials (IMM) Theory of Condensed Matter group (TCM) Interesting but useless! Nobel Lectures

More information

Material Science II. d Electron systems

Material Science II. d Electron systems Material Science II. d Electron systems 1. Electronic structure of transition-metal ions (May 23) 2. Crystal structure and band structure (June 13) 3. Mott s (June 20) 4. Metal- transition (June 27) 5.

More information

J 12 J 23 J 34. Driving forces in the nano-magnetism world. Intra-atomic exchange, electron correlation effects: Inter-atomic exchange: MAGNETIC ORDER

J 12 J 23 J 34. Driving forces in the nano-magnetism world. Intra-atomic exchange, electron correlation effects: Inter-atomic exchange: MAGNETIC ORDER Driving forces in the nano-magnetism world Intra-atomic exchange, electron correlation effects: LOCAL (ATOMIC) MAGNETIC MOMENTS m d or f electrons Inter-atomic exchange: MAGNETIC ORDER H exc J S S i j

More information

Spintronics. Seminar report SUBMITTED TO: SUBMITTED BY:

Spintronics.  Seminar report SUBMITTED TO: SUBMITTED BY: A Seminar report On Spintronics Submitted in partial fulfillment of the requirement for the award of degree of Electronics SUBMITTED TO: SUBMITTED BY: www.studymafia.org www.studymafia.org Preface I have

More information

Nanoelectronics 12. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture

Nanoelectronics 12. Atsufumi Hirohata Department of Electronics. Quick Review over the Last Lecture Nanoelectronics 12 Atsufumi Hirohata Department of Electronics 09:00 Tuesday, 20/February/2018 (P/T 005) Quick Review over the Last Lecture Origin of magnetism : ( Circular current ) is equivalent to a

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION SUPPLEMENTARY INFORMATION Reversible Electric Control of Exchange Bias in a Multiferroic Field Effect Device S. M. Wu 1, 2, Shane A. Cybart 1, 2, P. Yu 1, 2, M. D. Abrodos 1, J. Zhang 1, R. Ramesh 1, 2

More information

Making the Invisible Visible: Probing Antiferromagnetic Order in Novel Materials

Making the Invisible Visible: Probing Antiferromagnetic Order in Novel Materials Making the Invisible Visible: Probing Antiferromagnetic Order in Novel Materials Elke Arenholz Lawrence Berkeley National Laboratory Antiferromagnetic contrast in X-ray absorption Ni in NiO Neel Temperature

More information

MAGNETIC MATERIALS. Fundamentals and device applications CAMBRIDGE UNIVERSITY PRESS NICOLA A. SPALDIN

MAGNETIC MATERIALS. Fundamentals and device applications CAMBRIDGE UNIVERSITY PRESS NICOLA A. SPALDIN MAGNETIC MATERIALS Fundamentals and device applications NICOLA A. SPALDIN CAMBRIDGE UNIVERSITY PRESS Acknowledgements 1 Review of basic magnetostatics 1.1 Magnetic field 1.1.1 Magnetic poles 1.1.2 Magnetic

More information

SPINTRONICS. Waltraud Buchenberg. Faculty of Physics Albert-Ludwigs-University Freiburg

SPINTRONICS. Waltraud Buchenberg. Faculty of Physics Albert-Ludwigs-University Freiburg SPINTRONICS Waltraud Buchenberg Faculty of Physics Albert-Ludwigs-University Freiburg July 14, 2010 TABLE OF CONTENTS 1 WHAT IS SPINTRONICS? 2 MAGNETO-RESISTANCE STONER MODEL ANISOTROPIC MAGNETO-RESISTANCE

More information

Supplementary Figures

Supplementary Figures Supplementary Figures Supplementary Figure 1: Bloch point formation during skyrmion annihilation. Skyrmion number in layers with different z-coordinate during the annihilation of a skyrmion. As the skyrmion

More information

Lecture 6 NEW TYPES OF MEMORY

Lecture 6 NEW TYPES OF MEMORY Lecture 6 NEW TYPES OF MEMORY Memory Logic needs memory to function (efficiently) Current memories Volatile memory SRAM DRAM Non-volatile memory (Flash) Emerging memories Phase-change memory STT-MRAM (Ferroelectric

More information

Materials Research for Advanced Data Storage

Materials Research for Advanced Data Storage Materials Research for Advanced Data Storage University of Alabama Center for Materials for Information Technology Fall Review November 18, 2002 Center for Materials for Information Technology (MINT) at

More information

Stretching the Barriers An analysis of MOSFET Scaling. Presenters (in order) Zeinab Mousavi Stephanie Teich-McGoldrick Aseem Jain Jaspreet Wadhwa

Stretching the Barriers An analysis of MOSFET Scaling. Presenters (in order) Zeinab Mousavi Stephanie Teich-McGoldrick Aseem Jain Jaspreet Wadhwa Stretching the Barriers An analysis of MOSFET Scaling Presenters (in order) Zeinab Mousavi Stephanie Teich-McGoldrick Aseem Jain Jaspreet Wadhwa Why Small? Higher Current Lower Gate Capacitance Higher

More information

Optical studies of current-induced magnetization

Optical studies of current-induced magnetization Optical studies of current-induced magnetization Virginia (Gina) Lorenz Department of Physics, University of Illinois at Urbana-Champaign PHYS403, December 5, 2017 The scaling of electronics John Bardeen,

More information

Materials and Devices in Electrical Engineering

Materials and Devices in Electrical Engineering Examination WS 01/02 Materials and Devices in Electrical Engineering Monday 11 th of March, 9:00 to 11:00, SR 203, International Department building It is allowed to use any kind of media (books, scripts,

More information

Magnetism in correlated-electron materials

Magnetism in correlated-electron materials Magnetism in correlated-electron materials B. Keimer Max-Planck-Institute for Solid State Research focus on delocalized electrons in metals and superconductors localized electrons: Hinkov talk outline

More information

Spin-torque nano-oscillators trends and challenging

Spin-torque nano-oscillators trends and challenging Domain Microstructure and Dynamics in Magnetic Elements Heraklion, Crete, April 8 11, 2013 Spin-torque nano-oscillators trends and challenging N H ext S Giovanni Finocchio Department of Electronic Engineering,

More information

Artificially layered structures

Artificially layered structures http://accessscience.com/popup.ap x?id=053450&name=print Close Window ENCYCLOPEDIA ARTICLE Artificially layered structures Manufactured, reproducibly layered structures having layer thicknesses approaching

More information

Room-temperature perpendicular magnetization switching through giant spin-orbit torque from sputtered Bi x Se (1-x) topological insulator material

Room-temperature perpendicular magnetization switching through giant spin-orbit torque from sputtered Bi x Se (1-x) topological insulator material Room-temperature perpendicular magnetization switching through giant spin-orbit torque from sputtered Bi x Se (1-x) topological insulator material Mahendra DC 1, Mahdi Jamali 2, Jun-Yang Chen 2, Danielle

More information

V High frequency magnetic measurements

V High frequency magnetic measurements V High frequency magnetic measurements Rémy Lassalle-Balier What we are doing and why Ferromagnetic resonance CHIMP memory Time-resolved magneto-optic Kerr effect NISE Task 8 New materials Spin dynamics

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION DOI: 1.138/NMAT3449 Topological crystalline insulator states in Pb 1 x Sn x Se Content S1 Crystal growth, structural and chemical characterization. S2 Angle-resolved photoemission measurements at various

More information

Spin pumping in Ferromagnet-Topological Insulator-Ferromagnet Heterostructures Supplementary Information.

Spin pumping in Ferromagnet-Topological Insulator-Ferromagnet Heterostructures Supplementary Information. Spin pumping in Ferromagnet-Topological Insulator-Ferromagnet Heterostructures Supplementary Information. A.A. Baker,, 2 A.I. Figueroa, 2 L.J. Collins-McIntyre, G. van der Laan, 2 and T., a) Hesjedal )

More information

Nanoxide electronics

Nanoxide electronics Nanoxide electronics Alexey Kalabukhov Quantum Device Physics Laboratory MC2, room D515 Alexei.kalaboukhov@chalmers.se Playing Lego with oxide materials: G. Rijnders, D.H.A. Blank, Nature 433, 369 (2005)

More information

single-electron electron tunneling (SET)

single-electron electron tunneling (SET) single-electron electron tunneling (SET) classical dots (SET islands): level spacing is NOT important; only the charging energy (=classical effect, many electrons on the island) quantum dots: : level spacing

More information

Nanoxide electronics

Nanoxide electronics Nanoxide electronics Alexey Kalabukhov Quantum Device Physics Laboratory MC2, room D515 Alexei.kalaboukhov@chalmers.se Playing Lego with oxide materials: G. Rijnders, D.H.A. Blank, Nature 433, 369 (2005)

More information

Lecture 20: Semiconductor Structures Kittel Ch 17, p , extra material in the class notes

Lecture 20: Semiconductor Structures Kittel Ch 17, p , extra material in the class notes Lecture 20: Semiconductor Structures Kittel Ch 17, p 494-503, 507-511 + extra material in the class notes MOS Structure Layer Structure metal Oxide insulator Semiconductor Semiconductor Large-gap Semiconductor

More information

SPIN TRANSFER TORQUES IN HIGH ANISOTROPY MAGNETIC NANOSTRUCTURES

SPIN TRANSFER TORQUES IN HIGH ANISOTROPY MAGNETIC NANOSTRUCTURES CRR Report Number 29, Winter 2008 SPIN TRANSFER TORQUES IN HIGH ANISOTROPY AGNETIC NANOSTRUCTURES Eric Fullerton 1, Jordan Katine 2, Stephane angin 3, Yves Henry 4, Dafine Ravelosona 5, 1 University of

More information

Supporting Online Material for

Supporting Online Material for www.sciencemag.org/cgi/content/full/327/5966/662/dc Supporting Online Material for 00-GHz Transistors from Wafer-Scale Epitaxial Graphene Y.-M. Lin,* C. Dimitrakopoulos, K. A. Jenkins, D. B. Farmer, H.-Y.

More information

MODELING OF THE ADVANCED SPIN TRANSFER TORQUE MEMORY: MACRO- AND MICROMAGNETIC SIMULATIONS

MODELING OF THE ADVANCED SPIN TRANSFER TORQUE MEMORY: MACRO- AND MICROMAGNETIC SIMULATIONS MODELING OF THE ADVANCED SPIN TRANSFER TORQUE MEMORY: MACRO- AND MICROMAGNETIC SIMULATIONS Alexander Makarov, Viktor Sverdlov, Dmitry Osintsev, Josef Weinbub, and Siegfried Selberherr Institute for Microelectronics

More information