Spin precession and inverted Hanle effect in a semiconductor near a finite-roughness ferromagnetic interface

被引:175
作者
Dash, S. P. [1 ]
Sharma, S. [2 ,3 ]
Le Breton, J. C. [2 ,4 ,5 ]
Peiro, J. [4 ,5 ]
Jaffres, H. [4 ,5 ]
George, J. -M. [4 ,5 ]
Lemaitre, A. [6 ]
Jansen, R. [3 ]
机构
[1] Chalmers, Dept Microtechnol & Nanosci, SE-41296 Gothenburg, Sweden
[2] Netherlands Fdn Fundamental Res Matter FOM, NL-3502 GA Utrecht, Netherlands
[3] Spintron Res Ctr, Natl Inst Adv Ind Sci & Technol AIST, Tsukuba, Ibaraki 3058568, Japan
[4] Unite Mixte Phys CNRS Thales, F-91767 Palaiseau, France
[5] Univ Paris 11, F-91405 Orsay, France
[6] CNRS, Lab Photon & Nanostruct, F-91460 Marcoussis, France
来源
PHYSICAL REVIEW B | 2011年 / 84卷 / 05期
关键词
ROOM-TEMPERATURE; ELECTRICAL DETECTION; SILICON; POLARIZATION; SPINTRONICS; MAGNETORESISTANCE; ELECTRONICS; TRANSPORT; INJECTION; DEVICES;
D O I
10.1103/PhysRevB.84.054410
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Although the creation of spin polarization in various nonmagnetic media via electrical spin injection from a ferromagnetic tunnel contact has been demonstrated, much of the basic behavior is heavily debated. It is reported here that, for semiconductor/Al(2)O(3)/ferromagnet tunnel structures based on Si or GaAs, local magnetostatic fields arising from interface roughness dramatically alter and even dominate the accumulation and dynamics of spins in the semiconductor. Spin precession in inhomogeneous magnetic fields is shown to reduce the spin accumulation up to tenfold, and causes it to be inhomogeneous and noncollinear with the injector magnetization. The inverted Hanle effect serves as the experimental signature. This interaction needs to be taken into account in the analysis of experimental data, particularly in extracting the spin lifetime tau(s) and its variation with different parameters (temperature, doping concentration). It produces a broadening of the standard Hanle curve and thereby an apparent reduction of tau(s). For heavily doped n-type Si at room temperature it is shown that tau(s) is larger than previously determined, and a new lower bound of 0.29 ns is obtained. The results are expected to be general and to occur for spins near a magnetic interface not only in semiconductors but also in metals and organic and carbon-based materials including graphene, and in various spintronic device structures.
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页数:11
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