26 research outputs found
Spintronics: Fundamentals and applications
Spintronics, or spin electronics, involves the study of active control and
manipulation of spin degrees of freedom in solid-state systems. This article
reviews the current status of this subject, including both recent advances and
well-established results. The primary focus is on the basic physical principles
underlying the generation of carrier spin polarization, spin dynamics, and
spin-polarized transport in semiconductors and metals. Spin transport differs
from charge transport in that spin is a nonconserved quantity in solids due to
spin-orbit and hyperfine coupling. The authors discuss in detail spin
decoherence mechanisms in metals and semiconductors. Various theories of spin
injection and spin-polarized transport are applied to hybrid structures
relevant to spin-based devices and fundamental studies of materials properties.
Experimental work is reviewed with the emphasis on projected applications, in
which external electric and magnetic fields and illumination by light will be
used to control spin and charge dynamics to create new functionalities not
feasible or ineffective with conventional electronics.Comment: invited review, 36 figures, 900+ references; minor stylistic changes
from the published versio
Photon generation in ferromagnetic point contacts
We show theoretically that a significant spin accumulation can occur in electric point contacts between two
ferromagnetic electrodes with different magnetizations. Under appropriate conditions an inverse population of
spin-split electronic levels results in stimulated emission of photons in the presence of a resonant electromagnetic
field. The intensity of the emitted radiation can be several orders of magnitude higher than in typical semiconductor
laser materials for two reasons. (1) The density of conduction electrons in a metal point conduct is much
larger than in semiconductors. (2) The strength of the coupling between the electron spins and the electromagnetic
field that is responsible for the radiative spin-flip transitions is set by the magnetic exchange energy and can
therefore be very large as suggested by Kadigrobov et al. [Europhys. Lett. 67, 948 (2004)]