TY - CHAP
T1 - III-V-Based Ferromagnetic Semiconductors
AU - Matsukura, Fumihiro
AU - Ohno, Hideo
PY - 2013/10
Y1 - 2013/10
N2 - III-V compound semiconductors such as GaAs and InAs alloyed with Mn exhibit ferromagnetism. The magnetic, electrical, and optical properties of ferromagnetic III-V semiconductors are first compiled along with the way to prepare the epitaxial films and the effect of postgrowth annealing. Theories available to explain the magnetism in these alloys are then presented. Because the ferromagnetic semiconductors are compatible with epitaxial III-V heterostructures, a number of device structures have been examined and shown to reveal a wide variety of phenomena that either cannot be realized or are very difficult to observe in ferromagnetic metal structures. The unique properties revealed by ferromagnetic semiconductor structures, ranging from reversible electric field control of ferromagnetic phase transition to generating velocity versus current-density curves of current-induced domain wall motion, are then reviewed. The prospect of realizing high-transition temperature is discussed in the last section.
AB - III-V compound semiconductors such as GaAs and InAs alloyed with Mn exhibit ferromagnetism. The magnetic, electrical, and optical properties of ferromagnetic III-V semiconductors are first compiled along with the way to prepare the epitaxial films and the effect of postgrowth annealing. Theories available to explain the magnetism in these alloys are then presented. Because the ferromagnetic semiconductors are compatible with epitaxial III-V heterostructures, a number of device structures have been examined and shown to reveal a wide variety of phenomena that either cannot be realized or are very difficult to observe in ferromagnetic metal structures. The unique properties revealed by ferromagnetic semiconductor structures, ranging from reversible electric field control of ferromagnetic phase transition to generating velocity versus current-density curves of current-induced domain wall motion, are then reviewed. The prospect of realizing high-transition temperature is discussed in the last section.
KW - (Ga,Mn)As
KW - (In,Mn)As
KW - Current-induced domain wall motion
KW - Current-induced magnetization switching
KW - Electric field control of ferromagnetism
KW - Ferromagnetic semiconductor
KW - Low-temperature annealing
KW - Molecular beam epitaxy
KW - P-d Zener model
KW - Strain and temperature dependence of magnetocrystalline anisotropy
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U2 - 10.1016/B978-0-444-63279-1.00007-1
DO - 10.1016/B978-0-444-63279-1.00007-1
M3 - Chapter
AN - SCOPUS:84904226043
SN - 9780444632791
SP - 315
EP - 358
BT - Nanomagnetism and Spintronics
PB - Elsevier Inc.
ER -