Stock material or miscellaneous articles – Composite – Of inorganic material
Reexamination Certificate
1999-07-09
2002-06-11
Yamnitzky, Marie (Department: 1774)
Stock material or miscellaneous articles
Composite
Of inorganic material
C428S917000, C313S504000, C313S506000, C257S040000, C257S103000, C427S066000
Reexamination Certificate
active
06403238
ABSTRACT:
BACKGROUND OF THE INVENTION
The invention relates to the use of the new poly(p-phenylenevinylene) derivative, poly[2-methoxy-5-(2′-ethyl-hexyloxy)-1,4-phenylene-1,2-ethenylene-2,5-dimethoxy-1,4-phenylene-1,2-ethenylene] (M3EH-PPV) as electroluminescent material. The invention is also directed to organic light-emitting diodes (OLEDs) based on the above material, which diodes are remarkable for a significantly increased operating temperature range, as well as to a process for manufacturing said OLEDs by applying said M3EH-PPV directly from a solution in the form of a film onto the substrate or the coated substrate.
The availability of semi-conducting organic polymers and the demonstration of suitability of these conjugated polymers in the production of light-emitting components [J. H. Bouroughes et al., Nature 347, 539 (1990); Tang, VanSlyke, Appl. Phys. Lett. 51, 913, (1987)] marked the onset of world-wide extensive work on developing organic luminescent diodes and, based thereon, on displays as well. In contrast to inorganic LEDs based essentially on ternary and quaternary A
3
B
5
compounds, which can be used in displays of higher resolution only up to a point and at high cost, the organic emitters are rated to have an enormous potential for cost-minimized displays. In contrast to liquid crystal displays, electroluminescent displays have the advantage of being self-luminous and thus, do not require an additional rear light source.
Based on LEDs including conjugated polymers, it has been possible to accomplish both large area luminous surfaces and high-resolution displays. The principal structure of these luminous cells is illustrated in FIG.
1
. In this example, the luminous polymer is embedded between a hole-donating contact layer, frequently consisting of indium tin oxide (ITO), and an electron-injecting contact layer (Ca/Al, Al, Mg/Ag). In this case, a light-transmitting material such as glass or plastic, e.g., PET is used as substrate. Further optimizations of the component structures, such as introducing additional electron-transporting layers, hole-transporting layers, and separating the charge carrier-transporting layers from the recombination zone resulted in a substantially increased performance of the components with respect to efficacy, luminance and lifetime.
A material frequently used for OLEDs, which is both hole-transporting and relevant for recombination, is poly[2-methoxy-5-(2′-ethylhexyloxy)-1,4-phenylenevinylenel] (n>5) referred to as MEH-PPV.
This polymer represents a special PPV derivative which is soluble and can be applied onto the substrate using suitable techniques such as knifing or spin coating.
Using MEH-PPV, it has been possible to produce both single-layer structures and multi-layer structures with success. Using said material, it has been possible to produce diodes having very high quantum yields in the case of single-layer structures [Braun and Heeger; Appl. Phys. Lett. 58, 1982, (1991)].
SUMMARY OF THE INVENTION
Although good results have been achieved by using MEH-PPV, it would certainly be possible to further improve the general properties of the OLEDs. For example, one drawback of MEH-PPV is its relatively low glass transition temperature (Tg) of ≦68° C., limiting the operating temperature range of OLEDs based on this material and thus, their applicability.
It was therefore the object of the present invention to provide organic light-emitting diodes (OLEDs) having improved general properties.
Surprisingly, the new PPV derivative, poly[2-methoxy-5-(2′-ethylhexyloxy)-1,4-phenylene-1,2-ethenylene-2,5-dimeth-oxy-1,4-phenylene-1,2-ethenylene] (M3EH-PPV), which has at least 5 repeat units of the following formula
was shown to be a completely soluble semiconductor material which is film-forming from a solution and is particularly suited as an electroluminescent material.
Having nearly equivalent optical properties, M3EH-PPV surprisingly has improved thermal properties compared to MEH-PPV. Thus, the glass transition temperature (Tg) of M3EH-PPV measured using differential scanning calorimetry (DSC) is 108° C., being 40 K above that of MEH-PPV. The properties of the M3EH-PPV according to the invention are summarized in FIG.
2
.
M3EH-PPV can be prepared using condensation polymerization of 2-methoxy-5-(2′-ethylhexyloxy)terephthalaldehyde and 2,5-dimethoxy-p-xylylenebis(diethyl-phosphonate) under the action of a strongly basic condensation agent such as potassium tert-butylate, sodium ethylate or sodium hydride in an organic solvent such as for instance benzene, chlorobenzene, toluene, or xylene according to the HORNER METHOD (cf., e.g., DD 51 436, D 84 272). A second and more cost-effective way of prepation is presented by the inverse condensation polymerization of 2,5-dimethoxyterephthalaldehyde with 2-methoxy-5-(2′-ethylhexyloxy)-p-xylylenebis(diethyl-phosphonate), because 2,5-dimethoxyterephthalaldehyde is a more readily available starting material compared to 2-methoxy-5-(2′-ethylhexyloxy)terephthalaldehyde.
The bisphosphonates required as condensation components are readily available from the corresponding bis(halo-methyl) compounds and triethylphosphite using the Michaelis-Arbusov Reaction, for example.
Owing to the significantly higher Tg value, the use of M3EH-PPV as electroluminescent material in organic light-emitting diodes (OLEDS) results in OLEDs having an extended operating temperature range and thus, provides more user-friendly components. The invention is therefore directed to OLEDs including one or more active layers coated on a substrate, at least one of the light-emitting active layers being constituted of M3EH-PPV. In the meaning of the invention, “active layer” is to denote that the layer is capable of emitting light (light-emitting layer) when applying an electric field, and/or that it will improve the injection and/or transport of positive and/or negative charges (charge injection or charge transport layer). Thus, the OLEDs of the invention in their most elementary variant may comprise a charge carrier-injecting contact layer coated on the substrate, on which contact layer the light-emitting M3EH-PPV layer is situated, which is covered by a second contact layer injecting charge carriers of the opposite sign, wherein one of the contact layers must be optically transparent.
As a result of the solubility of the material according to the invention, the M3EH-PPV may also be used as a blend with other electrically active materials.
For building up the OLEDs of the invention, all the layer structures and materials are possible, in principle, which are known to a person skilled in the art and used for such layers, such as those described in U.S. Pat. No. 5,408,109, U.S. Pat. No. 5,247,190 or U.S. Pat. No. 5,719,467. Conventionally, the OLEDs include an electroluminescent layer between a cathode and an anode, wherein at least one of the electrodes must be transparent. In addition, one or more electron injection and/or electron transport layers may be introduced between the electroluminescent layer and the cathode, and/or one or more hole injection and/or hole transport layers may be introduced between the electroluminescent layer and the anode. Metals or metallic alloys, e.g., Ca, Mg, Al, In, Mg/Ag may be used as cathode. Metals such as Au or other metallic, conductive materials, e.g. ITO, on a transparent substrate may be used as anode.
In operation, the cathode is set to a negative potential with respect to the anode. As a result, electrons are injected from the cathode into the electron injection layer/electron transport layer or directly into the light-emitting layer. At the same time, holes are injected from the anode into the hole injection layer/hole transport layer or directly into the light-emitting layer.
Under the influence of an applied voltage, the injected charge carriers will move towards each other through the active layers. This results in electron/hole pairs at the boundary surface between the charge transport layer and the
Heine Günter
Helbig Manfred
Hörhold Hans-Heinrich
Pfeiffer Steffen
Uhlig Albrecht
Norris McLaughlin & Marcus P.A.
Yamnitzky Marie
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