|
To investigate the possibility of polarized charge injection at
the interface between a ferromagnetic metal and an organic material,
we fabricated planar light-emitting organic diodes (OLEDs) having
as cathode and anode thin films of different ferromagnetic metals
with unequal coercive forces.
As recombination luminescence arises from the singlet exciton,
we expect, for bipolar injection of polarized charge carrier injection,
a modulation of the electroluminescence (EL) intensity when the
relative orientation of the electrode magnetization switches, under
the influence of an external magnetic field, from parallel to antiparallel.
Measurements on such OLEDs show that the EL intensity increases
when the magnetization configuration changes from parallel to antiparallel.
Measurements on OLEDs having one non-magnetic and one magnetic electrode,
however, show that the EL intensity also changes, namely when the
magnetic field reaches the coercive field of the magnetic layer.
This result suggests that the modulation of the EL signal in the
OLED with two ferromagnetic electrodes does not arise from spin-polarized
charge carriers injected from the ferromagnetic layers into the
organic material, but rather due to an electric field dependence
of the EL intensity combined with magnetic stray fields from the
electrodes.
| OLED with Ni and permalloy electrodes, T
= 300 K. (a) Hysteresis loop of an OLED having a Ni anode
and a nonmagnetic cathode (Ca). (b) Corresponding OLED EL intensity
measurement. The offset between the minima of the the two branches
of the curve is a measure of the stray field of the ferromagnetic
layer. (c) Theoretically expected hysteretic behavior of the
electroluminescence. |
|