The disclosure relates to a light emitting device.
Compared to conventional light emitting diode (LED), an organic light emitting diode (OLED), a point source of light, may emit soft light which is similar to the characteristic of plane light source. The OLED can be manufactured into large area and to be transparent and made with a soft substrate to be flexible. Also, its luminance and color temperature may be adjusted. Moreover, it can be manufactured by printing to greatly reduce the manufacturing cost. Thus, the OLED has been widely developed.
However, it is an important issue to increase the efficiency of the OLED so far. The major research fields are divided into two aspects: increasing the efficiency of inner quantum and enhancing the efficiency of light extraction of lighting unite. Increasing the efficiency of inner quantum is subject to enhancement of speed rate of spontaneity radiation by electron and hole pairs. Current research proves that by adjusting the mode spatial distribution of electromagnetic wave according to Purcell effect by the electron and hole pairs, the speed rate of spontaneity radiation may be increased. In recent years, other research indicates that smaller mode volume can be generated by applying surface plasmon mode to enhance the Purcell effect. Furthermore, another experiment proves that the coupling reaction between the electron and hole pairs and surface plasmon mode with high density of states (DOS) can enhance the intensity of photoluminescence.
An embodiment of the disclosure provides a light emitting device comprising a substrate, a coupling unit and an organic light emitting unit. The coupling unit comprises a first conductive layer, a first light emitting layer and a second conductive layer. The first conductive layer is located on the substrate. The first light emitting layer is located between the first conductive layer and the second conductive layer. The organic light emitting unit is located adjacent to the second conductive layer.
The present disclosure will become more fully understood from the detailed description given hereinbelow, along with the accompanying drawings which are for illustration only, thus are not limitative of the present disclosure, and wherein:
In the following detailed description, for purposes of explanation, numerous specific details are set forth in order to provide a thorough understanding of the disclosed embodiments. It will be apparent, however, that one or more embodiments may be practiced without these specific details. In other instances, well-known structures and devices are schematically shown in order to simplify the drawing.
Please refer to
According to one embodiment of the disclosure, the organic light emitting unit 130 further comprises an electron transmission layer (not shown in the figure) disposed between the second electrode layer 135 and the second light emitting layer 133, and a hole transmission layer disposed between the second light emitting layer 133 and the first electrode layer 131 (not shown in the figure).
According to one embodiment of the disclosure, the substrate 110 is transparent, and the material of the substrate 110 is glass substrate or plastic substrate, but the material is not limited to the disclosure.
According to one embodiment of the disclosure, please refer to
Please refer to
According to one embodiment of the disclosure, the organic light emitting unit 130, shown in
In one embodiment, the second light emitting wavelength of the light emitted by the second light emitting layer 133 is less than the first light emitting wavelength of the light emitted by the first light emitting layer 122 of the coupling unit 120.
According to one embodiment of the disclosure, a light emitting device including multiple light emitting layers is disclosed. The same numerals in
Please refer to
In order to better understanding the above-mentioned and other purposes, features and advantages of the disclosure, the following provides exemplary embodiments to describe the light emitting device of the disclosure.
A glass substrate is provided. An aluminum metal with thickness of 20 nm is deposited on the glass substrate by thermally evaporation before Alq3 organic light emitting material with thickness 130 nm is thermally sputtered on it at 180 degrees Celsius. Then, another aluminum metal with thickness 20 nm is deposited on the Alq3 organic light-emitting material. However, these materials do not limit the disclosure, and the actual application is based on the claims of the disclosure. A semiconductor laser device with continuous wavelength of 405 nm or pulse pattern is applied to the phosphor photoluminescence, and light with a fixed incident angle is emitted to excite the Phosphor. Please refer to
Test of Surface Plasmon Resonance of the Coupling Unit 120
Structure (a) is Alq3 organic light emitting material/glass structure without metal; Structure (b) is single layer metal aluminum/Alq3 organic light emitting layer/glass structure (e.g., MD structure); Structure (c) is single layer aluminum metal/Alq3 organic light emitting layer/single layer aluminum metal (e.g., MDM structure). The requirement of the fabrication is the same as embodiment 1. Then, the above three structures are excited by the phosphor photoluminescence with the wavelength of 405 nm. The result shows in
According to the above description, it may be assumed that the intensity of phosphor of single-metal-layered structure (b) is weakened because of energy loss of surface plasmon and the blocking of the metal layer. In order to further test and analyze the coupling unit and attributes of PL spectrum, variable angle of the PL spectrum is measured and polarized by trans-magnetic (TM). The variable angles, wavelengths of phosphor and the intensities of photoluminescence of each wavelength are all depicted on a three-dimensional vector grey scale view, the dispersion curves are compared based on the theory and experiment. Thus, it is proved that the phosphor of the coupling unit is indeed generated from the radiation emitted by radiant surface plasmon mode or other light mode inside the coupling unit. Alternatively, the comparison and analysis of the dispersion curves of the coupling unit and the theoretical structures are applied by sample transmittance or reflection spectrum measurement experiment.
Please refer to
The dispersion curves are calculated by the result of measurement of the reflection and transmittance of the coupling unit. Please refer to
kx=√{square root over (∈d)}(ω/c0)sin θ
ω=1240/λ (eV)
After calculation, the points are depicted on the dispersion curves diagram. The diagram shows that the experiment points are indeed located in the radiation zone at left side of the lightline air and approach the theoretical curves of the odd function mode. The slight differentiation of the two curves is due to when the theoretical dispersion curve of the MDM structure is calculated, the thickness of the two layer metal is assumed to be semi-infinite for easily calculating the boundary condition. However, the actual condition is that the coupling unit has a limited thickness. The theoretical values of the dispersion curves in
The total thickness of non-metal in the coupling unit affects the characteristics of the surface plasmon. Thus, the thickness should be designed according to the characteristics of the surface plasmon and the thickness may not be greater than the wavelength of the spontaneity radiation on the structure. Moreover, taking the transmittance of the photon into consideration, the thicknesses of the upper and lower metal layers of the MDM structure may not be too thick, but the thicknesses are at least 3 to 30 nm, and the upper and lower metal layers are coated by evaporation, sputtering or plating.
The MDM structure is applied to an OLED unit. An insulation layer (silicon dioxide with 10 to 30 nm) is formed between the first electrode layer and the upper metal layer (second conductive layer) of the MDM structure. blue ray emitted by the OLED unit is applied to excite the light emitting layer of the MDM structure, such as yellow ray, to mix together to produce white ray, and the MDM structure is designed to gain a certain energy band. Please refer to Table 1, which is a reference of thicknesses of light emitting materials of MDM structure. The Table 1 shows that the wavelengths of the light emitting materials corresponding to the light emitting materials with different refractive index have appropriate thicknesses to improve optical gains.
Adjusting the thickness of organic layer makes the greatest coupling of the surface plasmon match the light emitting wavelength of the organic material as well as further reducing the thickness of the conductive layer to enhance the optical gain effect.
The foregoing description of the exemplary embodiments of the disclosure has been presented only for the purposes of illustration and description and is not intended to be exhaustive or to limit the disclosure to the precise forms disclosed. Many modifications and variations are possible in light of the above teaching.
Number | Date | Country | Kind |
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102144912 A | Dec 2013 | TW | national |
This patent application is a divisional patent application of U.S. patent application Ser. No. 14/144,080 filed on Dec. 30, 2013 and entitled “LIGHT EMITTING DEVICE,” which is a non-provisional application claims priority under 35 U.S.C. §119(a) on Patent Application No(s). 102144912 filed in Taiwan, R.O.C. on Dec. 6, 2013, the entire contents of which are hereby incorporated by reference.
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Number | Date | Country | |
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20160035798 A1 | Feb 2016 | US |
Number | Date | Country | |
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Parent | 14144080 | Dec 2013 | US |
Child | 14884553 | US |