Active solid-state devices (e.g. – transistors – solid-state diode – Incoherent light emitter structure – With particular semiconductor material
Reexamination Certificate
1999-06-18
2001-07-17
Tran, Minh Loan (Department: 2826)
Active solid-state devices (e.g., transistors, solid-state diode
Incoherent light emitter structure
With particular semiconductor material
C257S099000, C313S503000, C313S506000
Reexamination Certificate
active
06262441
ABSTRACT:
BACKGROUND OF THE INVENTION
Field of the Invention
The invention relates to an organic light emitting diode, i.e. a light emitting diode including an organic polymer and/or certain low molecular weight organic compounds.
As more and more data and information are being exchanged, the visualization of these, preferably in communication technology terminals, is becoming increasingly important. This presentation of information usually takes place through the use of pixel matrix display devices which, where appropriate, include additional predefined icons. Known technologies of pixel matrix devices include, for example, cathode ray tubes, although these, given the space they require, the electric power they absorb and their weight, are ruled out for use in mobile and portable electronic equipment. Significantly more suitable for this purpose are flat panel displays, which these days are predominantly based on liquid crystal display (LC display) technology.
Simple, monochrome, passive matrix driven LC displays have the advantage of being able to be fabricated cost effectively while absorbing little electric power, being lightweight and requiring little space. Using such displays also entails serious drawbacks, however. To be specific, the displays, given their technological/physical principle, are not self emitting, i.e. they can be read and discerned reliably only under particularly favorable ambient light conditions. A further significant limitation lies in the seriously restricted viewing angle of the display.
The problem of lacking contrast under non-optimal ambient light conditions can be ameliorated by an additionally fitted back lighting. However, that amelioration entails a number of drawbacks. The back lighting, for example, causes the thickness of the LC flat panel display to be many times greater. That is to say, while LC displays without backlighting can be fabricated with a thickness of <1 mm, the total thickness of backlit LC displays is typically several millimeters. Apart from the lamps or fluorescent tubes, the major contribution to the increase in thickness comes from the plastic light guide (diffusor) required for homogeneous illumination of the display area. An essential drawback of backlighting furthermore resides in the fact that most of the electric power absorbed is required for illumination. Moreover, operating the light sources (lamps and fluorescent tubes) requires a higher voltage which is usually generated from batteries or storage cells with the aid of voltage up converters.
Better performance than with LC displays driven in passive mode can be achieved with active matrix LC displays, where each pixel with its three primary colors has a thin film transistor (TFT) assigned to it. TFT technology is very complex, however, and due to the high process temperatures encountered the substrates used must meet high requirements; the price for active matrix LC displays is correspondingly high.
The switching time of an individual liquid crystal pixel is typically a few milliseconds—due to the physical principle of reorientation of a molecule in the electric field—and, moreover, is markedly temperature dependent. At low temperatures, for example, the sluggish, delayed image generation, for example in the case of transport (navigation systems in motor vehicles) is an annoying feature. In the case of applications where rapidly changing information or pictures are being displayed, for example in video applications, LC technology is therefore only conditionally suitable.
Other display technologies have either not yet reached the degree of maturity of technical applicability, for example flat panel CRTs (CRT=Cathode Ray Tube), or their use, particularly in portable electronic equipment, faces serious drawbacks due to specific characteristics: high operating voltage in the case of vacuum fluorescent displays and inorganic thin film electroluminescent displays or high costs in the case of displays based on inorganic light emitting diodes.
The abovementioned drawbacks can be circumvented through the use of displays based on organic light emitting diodes (OLEDs), i.e. electroluminescent diodes (in this context see, for example, U.S. Pat. No. 4,356,429 and U.S. Pat. No. 5,247,190). This novel technology has many and diverse advantages, compared with LC displays, of which the following are the essential ones:
Due to the principle of self emissivity, the need for backlighting is obviated, resulting in a distinct reduction in space required, power absorbed and weight.
The typical switching times of pixels are in the order of magnitude of 1 &mgr;s and thus allow rapid image sequences to be displayed without difficulty.
The switching times are not subject to annoying lag at low temperatures.
The reading angle is significantly greater than with LC displays and is almost 180°.
The polarisers required with LC displays can be dispensed with, so that greater brightness can be achieved even with a multiplexed display.
Organic light emitting diodes, in contrast to other display technologies, can be fabricated even on flexible substrates and in nonplanar geometries.
Fabrication and assembly of displays based on organic light emitting diodes is simpler, compared with LC displays, and can therefore be achieved more cost-effectively. Typically, assembly and fabrication proceed as follows.
The substrate, for example glass, is coated all over with a transparent electrode (bottom electrode, anode), for example formed of indium tin oxide (ITO). The fabrication of pixel matrix displays requires both the transparent bottom electrode and the top electrode (cathode) to be patterned. Both electrodes are customarily patterned in the form of parallel conductor tracks, the conductor tracks of bottom electrode and top electrode running perpendicular to one another. Patterning of the bottom electrode is effected through the use of a photolithographic process including wet chemical etching procedures, the details of which are known to those skilled in the art. The resolution achievable by these methods is essentially limited by the photolithographic steps and the nature of the bottom electrode. According to the prior art, this allows both pixel sizes and non emitting gaps between the pixels having a size of a few micrometers to be achieved. The length of the strip shaped conductor tracks of the bottom electrode can be as much as many centimeters. Depending on the lithographic mask used, it is even possible to fabricate emitting areas having sizes up to a few square centimeters. The sequence of the individual emitting areas can be regular (pixel matrix display) or variable (icons).
On top of the substrate bearing the patterned transparent bottom electrode, one or more organic layers are applied. These organic layers can be formed of polymers, oligomers, low molecular weight compounds or mixtures thereof. The application of polymers, for example polyaniline, poly(p-phenylene-vinylene) and poly(2-methoxy-5-(2′-ethyl)-hexyloxy-p-phenylene-vinylene) customarily employs processes from the liquid phase (application of a solution through the use of spin coating or knife coating), whereas gas phase deposition is preferred for low molecular weight and oligomeric compounds (vapor deposition or “physical vapor deposition”, (PVD). Examples of low molecular weight compounds, preferably those transporting positive charge carriers are: N,N′-bis-(3-methylphenyl)-N,N′-bis-(phenyl)-benzidine (m-TPD),4,4′,4″-Tris-[N-(3-methylphenyl)-N-phenyl-amino]-triphenylamine(m-MTDATA) and 4,4′,4″-Tris-(carbazol-9-yl)-triphenylamine (TCTA). The emitter used is, for example, the aluminum (III) salt of hydroxyquinoline (Alq), which may be doped with suitable chromophores (quinacridone derivatives, aromatic hydrocarbons etc.). If required, additional layers can be present which affect the electrooptical characteristics as well as the long term characteristics, for example layers of copper phthalocyanine. The total thickness of the layer sequence can be between 10 nm and 10 &mgr;m
Böhler Achim
Kowalsky Wolfgang
Metzdorf Dirk
Wiese Stefan
Greenberg Laurence A.
Lerner Herbert L.
Siemens Aktiengesellschaft
Stemer Werner H.
Tran Minh Loan
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