1. Field of the Invention
The invention relates in general to a light emitting device and a method of manufacturing the same, and more particularly to an infrared light emitting device and a method of manufacturing the same.
2. Description of the Related Art
An infrared light emitting device is mainly applied to the optical communication industry. The current infrared light emitting device may be manufactured by a few methods, such as epitaxy, and by using a semiconductor element (III-V group element) as the material. However, the infrared light element with the middle or long wavelength must be manufactured at the low temperature, so expensive cooling equipment is needed. Alternatively, the conventional infrared light element needs to use a multi-layer film structure so that the processing complexity is increased. In addition, the ratio of the full width at half maximum (FWHM) Δλ to the peak wavelength (Peak) λ of the spectrum of the current infrared light element is not ideal.
The invention is directed to a light emitting device, which can emit infrared light with the narrower bandwidth in the high-temperature operation by designing the dielectric layers with different thicknesses to effectively control the waveguide mode of the dielectric layer.
According to a first aspect of the present invention, a light emitting device for generating infrared light is provided. The light emitting device includes a substrate, a first metal layer, a dielectric layer and a second metal layer. The substrate has a first surface. The first metal layer is formed on the first surface of the substrate. The dielectric layer is formed on the first metal layer. A thickness of the dielectric layer is greater than a particular value. The second metal layer is formed on the dielectric layer. When the light emitting device is heated, the dielectric layer has a waveguide mode such that the infrared light generated by the light emitting device is transmitted in the dielectric layer, and a wavelength of the infrared light generated in the waveguide mode relates to the thickness of the dielectric layer.
According to a second aspect of the present invention, a method of manufacturing a light emitting device for generating infrared light is provided. The method includes the steps of: providing a substrate having a first surface; forming a first metal layer on the first surface of the substrate; forming a dielectric layer, having a specific thickness, on the first metal layer; and forming a second metal layer on the dielectric layer. When the light emitting device is heated, the dielectric layer has a waveguide mode such that the infrared light generated by the light emitting device is transmitted in the dielectric layer, and a wavelength of the infrared light generated in the waveguide mode relates to the thickness of the dielectric layer.
According to a third aspect of the present invention, a light emitting device for generating infrared light is provided. The light emitting device includes a substrate, a first metal layer, a dielectric layer and a second metal layer. The substrate has a first surface. The first metal layer is formed on the first surface of the substrate. The dielectric layer is formed on the first metal layer. A thickness of the dielectric layer is smaller than 500 nanometers (nm). The second metal layer is formed on the dielectric layer. The second metal layer has at least one first hole.
The invention will become apparent from the following detailed description of the preferred but non-limiting embodiments. The following description is made with reference to the accompanying drawings.
The disclosure provides a light emitting device and a method of manufacturing the same. The light emitting device generates infrared light. The light emitting device includes a substrate, a first metal layer, a dielectric layer and a second metal layer. The substrate has a first surface. The first metal layer is formed on the first surface of the substrate. The dielectric layer is formed on the first metal layer, and a thickness of the dielectric layer is greater than a particular value. The second metal layer is formed on the dielectric layer. When the light emitting device is heated, the dielectric layer has a waveguide mode because the thickness of the dielectric layer is greater than the particular value, such that the infrared light generated by the light emitting device may be transmitted in the dielectric layer. In addition, a wavelength of the infrared light generated in the waveguide mode of the dielectric layer may be adjusted by adjusting the thickness of the dielectric layer. That is, the wavelength of the infrared light generated in the waveguide mode of the dielectric layer relates to the thickness of the dielectric layer.
First Embodiment
The first metal layer 230 serves as a background radiation suppressing layer and an infrared light reflecting layer having the functions of suppressing the background radiation emitted from the substrate 210 and reflecting the infrared light generated by the dielectric layer 250. Because the thickness of the second metal layer 270 of this embodiment is sufficiently small, the infrared light generated by the dielectric layer 250 may be partially reflected by the second metal layer 270 and partially transmitted through the second metal layer 270.
In this embodiment, the third metal layer 290 serves as a heating source of the light emitting device 20 when a current is conducted. When the current flows through the third metal layer 290, the light emitting device 20 is heated. When the light emitting device 20 is heated, the background radiation emitted from the substrate 210 is blocked by the first metal layer 230, and the emissivity of the first metal layer 230 is very low so that the first metal layer will not emit a lot of thermal radiation. Furthermore, the thickness of the dielectric layer 250 is greater than the particular value, so the dielectric layer 250 has a waveguide mode. The thermal radiation generated by the dielectric layer 250 is restricted in the first metal layer 230 and the second metal layer 270 to oscillate back and forth, and to be transmitted in the dielectric layer 250. After the dielectric layer 250 absorbs the thermal radiation, the electrons of the dielectric layer 250 make the transition from an outer orbit to an inner orbit, and the thermal radiation is converted into optical energy. The result obtained after the thermal radiation of the dielectric layer 250 is repeatedly transmitted and repeatedly resonates in the dielectric layer 250 greatly increases the light intensity of a specific wavelength of infrared light.
In detail, the substrate 210 may be a conductor substrate, an insulation substrate or a semiconductor substrate. The material of the first metal layer 230 is selected from the group consisting of gold (Au), silver (Ag) and a metal having the reflectivity and emissivity respectively ranging from 0.5 to 1 and from 0 to 0.5 in the middle infrared light wave band. The material of the dielectric layer 250 may be oxide, nitride or any other dielectric material or insulation material. The second metal layer 270 includes at least one of silver (Ag) and a metal having the reflectivity ranging from 0.5 to 1 in the middle infrared light wave band. The third metal layer 290 includes at least one of molybdenum (Mo) and a metal having the electrical conductivity ranging from 103 to 6×105(1/cm-Ohm).
In this embodiment, the third metal layer 290 is formed on a second surface 213 of the substrate 210, which is disposed opposite to the first surface 211. However, the third metal layer 290 is not restricted to be formed on the second surface 213 of the substrate 210, and may also be formed between the substrate 210 and the first metal layer 230. Alternatively, the third metal layer 290 is directly replaced with the first metal layer 230 serving as a heating source. Alternatively, the third metal layer 290 is not needed and the substrate 210 may be directly heated.
In this embodiment, the thickness of the dielectric layer 250 has a particular value so that the dielectric layer 250 has a waveguide mode and the infrared light generated when the light emitting device is heated may be transmitted in the dielectric layer 250. Furthermore, after the infrared light is repeatedly transmitted and repeatedly resonates in the dielectric layer 250, the infrared light having the ratio of the FWHM (Δλ) to the peak wavelength (λ) may be obtained to be about 3%, which is better than the ratio of the FWHM to the peak wavelength in the infrared light emitting device 1 shown in
Second Embodiment
If the physical property between the first metal layer 330 and the substrate 310, such as the bonded strength, is too low and the first metal layer 330 is directly formed on the substrate 310, the firmness therebetween may become poor. Thus, the first metal adhesive layer 320 having the physical property ranging between the substrate 310 and the first metal layer 330 is selected to enhance the firmness between a first surface 311 of the substrate 310 and a first surface 331 of the first metal layer 330. Similarly, the second metal adhesive layer 340 having the physical property ranging between the first metal layer 330 and the dielectric layer 350 is selected to enhance the firmness between a second surface 332 of the first metal layer 330 and a first surface 351 of the dielectric layer 350. Thus, when the light emitting device 30 is heated to the high temperature, the possibility of generating peel off between the substrate and the first metal layer, or between the first metal layer and the dielectric layer can be greatly reduced.
The materials of the first metal adhesive layer 320 and the second metal adhesive layer 340 are selected from the group consisting of transition metals, including titanium (Ti), chromium (Cr), tantalum (Ta), zirconium (Zr) and the like, a metal having the surface bonding strength greater than 20 MPa, a metal having the surface bonding strength greater than gold (Au) and silicon dioxide (SiO2), and combinations thereof.
Third Embodiment
The second metal layer 470 has at least one hole 471. So, when the light emitting device 40 is heated, the infrared light transmitted in the waveguide mode of the dielectric layer 450 may be transmitted through the hole 471. Thus, the thickness of the second metal layer 470 of this embodiment is not particularly restricted to any specific range. In addition, the at least one hole 471 may be formed by way of lithography.
Furthermore, because the second metal layer 470 has at least one hole 471, it is also possible to induce the surface plasma modes in the interface between the dielectric layer 450 and the second metal layer 470, and the interface between the second metal layer 470 and the air when the light emitting device 40 is heated. That is, when the light emitting device 40 is heated, the dielectric layer 450 has two modes including a surface plasma mode and a waveguide mode. The infrared light generated in the waveguide mode relates to the thickness of the dielectric layer 450. In the surface plasma mode, the infrared light is generated by the electric field oscillation around the interface between the dielectric layer 450 and the second metal layer 470 and the interface between the second metal layer 470 and the air. Because the frequency of the electric field oscillation relates to the arranging periodicity of the holes, the infrared light generated in the surface plasma mode relates to the arranging periodicity of the holes 471 of the second metal layer 470. Thus, the arranging periodicity of the holes 471 may be reduced so that the wavelength of the infrared light generated in the surface plasma mode may be reduced and the wavelength of the infrared light generated in the surface plasma mode is different from the wavelength of the infrared light generated in the waveguide mode.
According to the actual experimental results, as shown in
Fourth Embodiment
In other embodiments of this disclosure, the thickness of the dielectric layer is greater than the particular value such that the dielectric layer has the waveguide mode and the infrared light can be thus generated. Thus, the thickness of the dielectric layer is reduced in this embodiment so that the infrared light generated by the light emitting device is generated in the surface plasma mode.
In this embodiment, the thickness of the dielectric layer 550 is smaller than the particular value, such as 500 nm, such that the dielectric layer 550 and the second metal layer 570 generate the surface plasma mode and are coupled to the first metal layer 530. The surface plasma mode generated by the dielectric layer 550 and the second metal layer 570 and the induced surface plasma mode coupling between the dielectric layer 550 and the first metal layer 530 become stronger as the thickness of the dielectric layer 550 gets smaller. Thus, the refractive index of the dielectric layer 550 is changed, thereby influencing the infrared wavelength generated by the dielectric layer 550, as shown in
While the invention has been described by way of examples and in terms of preferred embodiments, it is to be understood that the invention is not limited thereto. On the contrary, it is intended to cover various modifications and similar arrangements and procedures, and the scope of the appended claims therefore should be accorded the broadest interpretation so as to encompass all such modifications and similar arrangements and procedures.
Number | Date | Country | Kind |
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99107890 A | Mar 2010 | TW | national |
This is a continuation-in-part application of U.S. application Ser. No. 11/591,640, filed Nov. 2, 2006, and claims the benefit of Taiwan application Serial No. 99107890, filed Mar. 17, 2010, the subject matter of which is incorporated herein by reference.
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Number | Date | Country | |
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20100213492 A1 | Aug 2010 | US |
Number | Date | Country | |
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Parent | 11591640 | Nov 2006 | US |
Child | 12728377 | US |