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JAPAN NANONET BULLETIN - 47th Issue - June 23, 2005

NANONET INTERVIEW

Hideo OHNO
Professor, Research Institute of Electrical Communication, Tohoku University

Crossing of magnetism and semiconductor physics
— Ferromagnetic semiconductors expand the possibilities of spintronics —

(Issued in Japanese: December 23, 2003)

The charge of electron enables semiconductors to process information, and its spin allows us to realize magnetic information storage devices. Even though these properties are normally utilized separately using magnetic and semiconductor materials, respectively, spintronics uses both properties in the same material. There are two approaches for designing advanced spintronic devices. One is to use both degrees of freedom in metal-based magnetic materials, and the other is in semiconductors. Prof. Ohno has expanded the possibilities of utilizing semiconductors with various structures and functions by making III-V semiconductors ferromagnetic.

The ferromagnetic semiconductor that Prof. Ohno developed was (In, Mn)As in which part of the indium atoms in InAs is replaced with manganese, which is a magnetic element. He said, “When I went to the IBM T. J. Watson Laboratory in 1988, joining Leo Esaki's group, I thought of conducting two kinds of research if I was given the chance. One was research which seemed too difficult to accomplish, and the other was research through which I could publish papers.” It was widely known then that if the Mn concentration was too high, a MnAs phase would nucleate before making InAs magnetic. However, he and his coworkers were able to synthesize single-phase (In, Mn)As by decreasing the crystal growth temperature to 250°C.

Several years later, he discovered that single-phase (In, Mn)As was ferromagnetic at low temperatures. Although he had an idea of causing semiconductors to have magnetism, he never expected that semiconductors would be ferromagnetic. A ferromagnetic material transforms to a paramagnetic material when it exceeds a transition temperature. He produced a field effect transistor using (In, Mn)As and was able to change the transition temperature of (In, Mn)As by applying an electric field. He showed that the transition temperature of (In, Mn)As increases as its carrier concentration increases in an applied electric field . This occurs because the Mn spins align in the same direction due to their interaction with charge carriers in the semiconductor. He says, “A semiconductor has the capability of changing the number of electrons. Although it has been about 26 to 27 centuries since human beings found magnetic materials, this was the first time that we prepared magnetic materials of which the properties could be altered after fabrication was complete.” However, unless the transition temperature drastically increases, these materials cannot be commercialized. As well as increasing the Mn concentration, he has been searching for other alloying elements with a stronger interaction between charge carriers and Mn spins because the interaction depends on the type of semiconductors.

The next generation magnetic device, MRAM (Magnetic Random Access Memory), where its memory bits are highly integrated, will require a high magnetic field or a large electric current to record data. The ferromagnetic semiconductor, (In, Mn)As, meets this requirement when it is used in a field effect transistor. When an electric field of about 1.5MV/cm is applied to (In, Mn)As, its coercive force decreases, and the magnetic field required for magnetization reversal falls to one fifth of that currently used. When data is recorded by a low magnetic field while applying an external electric field, and then the field is turned off, the coercive force is recovered, which means that a higher magnetic field will be required to rewrite data.

Prof. Ohno thinks the key to a scientific breakthrough is curiosity. “However, it takes more than curiosity. You have to decide what you are going to do and do it quickly. You need to design things in such a way that you can go through a number of trials without spending too much time. Then, quantity turns to quality at a certain point,” said Prof. Ohno. His research is fundamental, but he is always thinking about its applications. He says, “You can publish your paper no matter what your research is. There are lots of research areas, which others have not studied yet. However, time and resources are limited. The first thing you have to do is to choose what you will do or will not do, and then figure out how to deepen your research. After all, what you choose to do first will show your taste.

(Interviewer: Kuniko Ishiguro, Cosmopia Inc.)
Hideo OHNO
Hideo OHNO
Professor, Research Institute of Electrical Communication, Tohoku University
 
1977Graduated from Department of Electronic Engineering, Faculty of Engineering, The University of Tokyo
1979Master of Engineering, Graduate School of Engineering, The University of Tokyo
1982Doctor of Engineering, Graduate School of Engineering, The University of Tokyo
(July, 1979-June, 1980 Department of Electric Engineering, Cornell University, USA)
1982Lecturer, Department of Electrical Engineering, Faculty of Engineering, Hokkaido University
1983Associate Professor, Department of Electrical Engineering, Faculty of Engineering, Hokkaido University
(Sept., 1988-April, 1990 Visiting Researcher, IBM T.J. Watson Research Center, USA)
1994Professor, Department of Electronics, Faculty of Engineering, Tohoku University
1995~
present
Professor, Research Institute of Electrical Communication, Tohoku University
1992
~95
Researcher, Precursory Research for Embryonic Science and Technology (PRESTO), Japan Science and Technology Corporation (JST)
1997
~2000
Head Investigator, Scientific Research in Priority Areas “Spin-Controlled Semiconductor Nanostructures”, Ministry of Education, Science, Sports and Culture (MEXT)
1997
~2002
Project Leader, “Atomic Scale Dynamics of Non-Equilibrium Surface Layer and Synthesis of New Materials” Project, Research for the Future Program, Japan Society for the Promotion of Science (JPSJ)
2002~
present
Project Leader, the IT-Program of Research Revolution 2002, “Development of Universal Low-Power Spin Memory” Project, MEXT
2002~
present
Research Director “OHNO Semiconductor Spintronics” Project, Exploratory Research for Advanced Technology (ERATO), Japan Science and Technology Agency (JST)
 
1993
~1998
Editor, Japanese Journal of Applied Physics
1996
~2003
Associate Editor, Journal of Crystal Growth
1999~
present
Associate Editor, Virtual Journal of Nanoscale Science and Technology
2002~
present
Editorial Board, Semiconductor Science and Technology
2003~
present
Editorial Board, Superlattices and Microstructures
 
Award and Prizes
1998Japan IBM Science Award
2003The IUPAP Magnetism Prize
2005Japan Academy Prize

Fig. 1 Fig. 1 Large Image
Injection of spin-polarized holes into a light-emitting p-n diode using a ferromagnetic semiconductor (Ga,Mn)As.
(a) Sample structure. Spin-polarized holes h+ travel through the non-magnetic GaAs and recombine with spin-unpolarized electrons in the (In,Ga)As quantum well. I represents the current, and σ+ represents circularly polarized light emitted from the edge of the quantum well.
(b) The dependence of the polarization ΔP of the emitted light on the magnetic field B at each temperature. The solid and hollow symbols represent the degree of polarization when the magnetic field is swept in the positive and negative directions, respectively. The magnetic field was applied parallel with the easy axis of magnetization of the (Ga,Mn)As. The inset depicts the temperature dependence of the residual magnetization M in (Ga,Mn)As, where the degree of polarization of the zero magnetic field seen in the emitted light (squares) exhibits the same temperature dependence as the magnetization.
Fig. 2 Fig. 2 Large Image
Gate voltage dependence of Hall resistance in an (In,Mn)As FET structure close to the ferromagnetic transition temperature. When a gate voltage of VG= -125 V is applied, hysteresis is clearly observed. On the other hand, when VG= +125 V, the hysteresis disappears. This demonstrates that the applied field is able to switch the device between ferromagnetic and paramagnetic states.
Fig. 3 Fig. 3 Large Image
Curie temperatures calculated using mean-field theory for various III-V as well as group IV and II-VI semiconducting compounds containing 5% of Mn per cation (or 2.5% per atom) with 3.5x1020 holes per cm3.