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Singlet-to-triplet interconversion using hyperfine as well as ferromagnetic fringe fields
Author(s) -
M. Wohlgenannt,
Michael E. Flatté,
Nicholas J. Harmon,
F. Wang,
Andrew D. Kent,
Ferran Macià
Publication year - 2015
Publication title -
philosophical transactions of the royal society a mathematical physical and engineering sciences
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.074
H-Index - 169
eISSN - 1471-2962
pISSN - 1364-503X
DOI - 10.1098/rsta.2014.0326
Subject(s) - magnetoresistance , condensed matter physics , hyperfine structure , spintronics , electroluminescence , zeeman effect , magnetic field , ferromagnetism , spin (aerodynamics) , materials science , field (mathematics) , anisotropy , polaron , physics , nanotechnology , atomic physics , electron , optics , quantum mechanics , mathematics , layer (electronics) , pure mathematics , thermodynamics
Until recently the important role that spin-physics ('spintronics') plays in organic light-emitting devices and photovoltaic cells was not sufficiently recognized. This attitude has begun to change. We review our recent work that shows that spatially rapidly varying local magnetic fields that may be present in the organic layer dramatically affect electronic transport properties and electroluminescence efficiency. Competition between spin-dynamics due to these spatially varying fields and an applied, spatially homogeneous magnetic field leads to large magnetoresistance, even at room temperature where the thermodynamic influences of the resulting nuclear and electronic Zeeman splittings are negligible. Spatially rapidly varying local magnetic fields are naturally present in many organic materials in the form of nuclear hyperfine fields, but we will also review a second method of controlling the electrical conductivity/electroluminescence, using the spatially varying magnetic fringe fields of a magnetically unsaturated ferromagnet. Fringe-field magnetoresistance has a magnitude of several per cent and is hysteretic and anisotropic. This new method of control is sensitive to even remanent magnetic states, leading to different conductivity/electroluminescence values in the absence of an applied field. We briefly review a model based on fringe-field-induced polaron-pair spin-dynamics that successfully describes several key features of the experimental fringe-field magnetoresistance and magnetoelectroluminescence.

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