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Measuring the dipole orientation in OLEDs

: Flämmich, M.; Roth, S.; Danz, N.; Michaelis, D.; Bräuer, A.; Gather, M.-C.; Meerholz, K.


Heremans, P.L. ; Society of Photo-Optical Instrumentation Engineers -SPIE-, Bellingham/Wash.:
Organic Photonics IV : 12-15 April 2010, Brussels, Belgium
Bellingham, WA: SPIE, 2010 (Proceedings of SPIE 7722)
ISBN: 978-0-8194-8195-5
Paper 77220D
Conference "Organic Photonics" <4, 2010, Brussels>
Fraunhofer IOF ()
organic light emitting diode; optical simulation; in-situ characterization; dipole emitter orientation

The orientation of the emissive dipole moments in organic light-emitting diodes (OLEDs) has a major impact on the optical outcoupling efficiency and, consequently, on the device performance as well as on possible optimization strategies. In this contribution we discuss a general method to quantify the amounts of parallel and perpendicular emissive sites in OLEDs. The presented in-situ-method is based on measurements of the far-field emission of an electrically operating device and corresponding optical reverse simulations. For the reverse simulation we take advantage of the fact that perpendicular dipoles only contribute to transverse-magnetic polarized light emission. In general, the method can be applied to all classes of emissive materials for OLEDs, including small-molecule and dendrimer materials. In the present study we utilize bottom emitting polymeric OLEDs with two different stack architectures: (A) a conventional OLED stack optimized for maximum performance and (B) a well adapted OLED stack, where the contribution of perpendicularly oriented dipoles to the radiation pattern in air is optically enhanced. We demonstrate that for OLED (A) perpendicular dipoles are "invisible" in the optical far-field, because almost all light from perpendicularly oriented dipoles is trapped inside the OLED stack. Consequently, no information about the emitter orientation can be gained from the radiation pattern of this device. In contrast, OLED (B) clearly shows that the radiation pattern is generated by 93.5 % parallel and 6.5 % perpendicular dipoles. Assuming a Gaussian distribution of dipole orientations in the particular emissive material, the dipoles stagger around the preferred parallel direction with an 1/e-angle of ± 22°.