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Microporous phase-separated films of polymer blends for enhanced outcoupling of light from OLEDs

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Abstract

Thin microporous films were formed by dropcasting a toluene solution containing various ratios of polystyrene:polyethylene glycol blends on a glass substrate, with OLEDs on the ITO that coated the opposite side of that substrate. We demonstrate for the first time that such easily-fabricated films with surface and bulk micropores in the index-matching polystyrene can serve as random microlens-like arrays to improve forward OLED light extraction by up to ~60%. A theoretical interpretation of the angular emission profile of the device, considering the geometrical change at the substrate/air interface and the scattering by the pores within the films, was established in excellent agreement with the experiments. The use of such blended thin films provides an economical method, independent of the OLED fabrication technique, for improving the outcoupling efficiency.

©2011 Optical Society of America

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Figures (3)

Fig. 1
Fig. 1 (a) Schematic demonstration of the microporous structure formation of the PS:PEG mixed film during the drying process following dropcasting; note that the actual pore density is not uniform. (b) SEM images of the surface and cross section of a film with 48:12 mg/mL PS:PEG. (c) The principle of the OLED outcoupling enhancement by the PS:PEG film.
Fig. 2
Fig. 2 Effect of 200 μL PS:PEG 54:6 mg/mL in toluene that were dropcast on the backside of the OLED’s ITO/glass substrate. (a) Images of two pixels with and without the PS:PEG film, each biased at 6 V. The dropcast area is 1 × 1 in.2 (b) Overall emission spectra of the devices with (red open circles) and without (black solid squares) the PS:PEG film. The current density in each device was J = 55 mA/cm2 (c) Angular emission intensity profile of the device with (red open circles) and without (black solid squares) the PS:PEG film. In each device J = 5.5 mA/cm2 The solid lines are the Lambertian emission profiles. The dashed purple line is the simulated emission profile. We note that the enhancement was essentially independent of J and consequently, of course, the brightness L, in agreement with other studies [16].
Fig. 3
Fig. 3 The surface SEM images of the PS:PEG films with different weight ratios, but constant total concentration of 60 mg/mL. The scale bar in the insets is 10 μm.

Tables (1)

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Table 1 Comparison of Outcoupling Enhancement Factor by PS:PEG Films with Different Weight Ratios Total Concentration: 60 mg/mL) a

Equations (5)

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I 1 ( θ 1 ) = I 0 ( θ 0 ) sin θ 0 d θ 0 sin θ 1 d θ 1 = n P S : P E G 2 cos θ 1 n o r g 2 cos θ 0 I 0 ( θ 0 ) = n P S : P E G 2 cos θ 1 n o r g 2 1 ( n P S : P E G n o r g sin θ 1 ) 2 I 0 ( θ 0 )
I 2 ( θ 2 ) = n a i r 2 cos θ 2 n o r g 2 1 ( n a i r n o r g sin θ 2 ) 2 I 0 ( θ 0 ) ,
I 2 ( θ 2 ) = 1 2 π n a i r 2 cos θ 2 n o r g 2 1 ( n a i r n o r g sin θ 2 ) 2 ,
I 1 ' ( θ 1 ) = { C 1 w h e n θ 1 θ c C 2 w h e n θ 1 > θ c ,
I 2 ' ( θ 2 ) = C 1 n a i r 2 cos θ 2 n P S : P E G 2 1 ( n a i r n P S : P E G sin θ 2 ) 2 .
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