1. Field of the Invention
The present invention relates a photodetector, particularly to an infrared photodetector having the opening structure formed in order to increase the Schottky junction area between the light absorbing layer, and method of fabricating the same.
2. Description of the Prior Art
The current infrared photodetector adopts the absorption characteristics of semiconductor material at certain band. When the light is absorbed by the material, the electron-hole pair will be separated, and the electric signal will be outputted as the basis for judging the light intensity. The semiconductor materials often used in the infrared photodetector are germanium (Ge) and indium gallium arsenide (InGaAs) etc. The photodetector made by these materials has good photoelectric conversion efficiency at this infrared band. However, the cost of these materials is higher. They are toxic and hard to be integrated with current semiconductor process technology.
The silicon (Si) wafer is frequently used as the substrate for semiconductor process at present. It is a very inexpensive material, and the development of corresponding process technology is much mature. However, the problem faced by natural silicon substrate is that its energy band gap is only 1.12 eV at room temperature. It is to say when the energy of incident light is lower than 1.12 eV—the wavelength of incident light is larger than 1100 nm—the light cannot be absorbed by the silicon substrate. Thus, the detectable range of wavelength for Si-based photodetector will be limited seriously.
In the conventional technology, the metal nano-antennas structure is formed on the silicon substrate. The metal nano-antennas structure (smaller than 100 nm) is used to absorb light to produce the surface plasmon attenuation, and further jump the Schottky junction generated between metal and silicon substrate, in order to detect infrared. However, the Localized Surface Plasma Resonance (LSPR) produced by this metal nano-antennas structure is not significant at the infrared band. It is limited seriously by the polarization of incident light. The LSPR can only be activated by specific polarization of incident light. Thus, the electric signal output of this metal nano-antennas structure element will be unsatisfactory finally.
It is known that the fabrication method of the abovementioned conventional photodetector requires longer process time, more complex process and higher cost. In addition, it is also a big problem that the conventional technology is limit to the polarization of incident light. Namely, before the loss caused by the carrier formed by the surface plasmon attenuation is not considered, the photodetector fabricated by the abovementioned method is unable to convert the polarized incident light sources into the surface plasmon, it will limit the practicability of actual operation seriously, and cause the loss of some polarized incident light sources surely.
In view of this, the present invention provides a photodetector, which comprises a semiconductor substrate, a plurality of opening structures, and a light absorbing layer (including metal layer, silicide layer).
In an embodiment, the abovementioned light absorbing layer of metal layer comprises the gold (Au), silver (Ag), aluminum (Al), copper (Cu), titanium (Ti), nickel (Ni), platinum (Pt), chromium (Cr), tungsten (W), molybdenum (Mo), and cobalt (Co) etc.
In an embodiment, the abovementioned light absorbing layer of silicide layer comprises the platinum-silicon compound (PtxSi), nickel-silicon compound (NixSi), titanium-silicon compound (TixSi), cobalt-silicon compound (CoxSi), tungsten-silicon compound (WxSi) and molybdenum-silicon compound (MoxSi) etc., where x is an arbitrary number representing the ratio of metal and silicon.
In an embodiment, the abovementioned opening structure may be periodic structures, or non-periodic structures, which will produce the same effect.
In an embodiment, the depth of the abovementioned opening structures and the thickness of light absorbing layer can be optimized in accordance with the range of detected wavelength. Furthermore, the ratio of the thickness of the absorbing layer to the width of opening structure must be smaller than 0.5.
Another purpose is to provide a fabrication method of the abovementioned photodetector, which comprises the following steps:
Firstly, providing a semiconductor substrate is carried out. Then, forming a plurality of pattern on the semiconductor substrate, and making a plurality of light absorbing layer structures on the pattern of semiconductor substrate. Finally, a light absorbing layer (including metal layer, and silicide layer) is formed over the semiconductor substrate and a plurality of opening structures. The absorbing layer is formed across at least two opening structures.
In an embodiment, the step for forming a plurality of pattern on the abovementioned semiconductor substrate is completed by a lithography process (such as I-line, g-line, E-beam, KrF, ArF, DUV, Extreme UV lithography).
In an embodiment additionally, the step for forming a plurality of opening structures on the pattern of semiconductor substrate is completed by an etching process.
From the following description, it can further understand the features and advantages of the present invention. Please refer to
The foregoing aspects and many of the attendant advantages of this invention will become more readily appreciated as the same becomes better understood by reference to the following detailed description, when taken in conjunction with the accompanying drawings, wherein:
In the following description, the attached Figures will be used to describe the implementation of the present invention. In the Figures, the same symbol of element is used to represent the same element. In order to explain clearly, the size or thickness of the element may be exaggerated.
Please refer to
Firstly, as shown in Step S102 of
Then, as shown in Step S104 of
The Step S106 of
However, as the abovementioned description, the purpose of the present invention is to make the Schottky junction with large contact area between metal and silicon substrate.
Finally, in the Step S108, a light absorbing layer 30 is formed over the semiconductor substrate 10 and a plurality of opening 20 structures. The absorbing layer 30 is formed across at least two opening 20 structures. Furthermore, the ratio of the thickness of the absorbing layer 30 to the width of opening 20 structure must be smaller than 0.5.
As the abovementioned description, the photodetector fabricated by the method provided by the present invention is shown in
For example, the label of H065P13 means the size of the opening 20 structure is 0.65 μm and the period is 1.3 μm (i.e., the distance between two opening structures). Therefore, the size of the opening 20 structure is from 0.65 μm to 0.85 μm, but the present invention is not limited by this. 1.
At this moment, the image of scanning electronic microscope for the photodetector is shown in
Then, for the optical characteristics of the photodetector provided by the present invention, please refer to
Furthermore, as shown in
Finally, please refer to
In order to prove that the photodetector provided by the present invention has very good infrared conversion responsivity, the electric signal will be further measured for this photodetector. It is noted that in order to reach low energy consumption, the polarization is not added in the measurement process.
Please refer to
As shown in
Then, please refer to
Summarized from the abovementioned description, a plurality of periodic (or non-periodic) opening structure is formed in the present invention. The surface plasmon resonance and cavity effect can be generated by the continuous thin metal structures. The Schottky junction with large contact area can be produced between metal and silicon substrate. The hot electrons can be generated effectively through the attenuation of surface plasmon, in order to increase the photoelectric conversion of this Si-based photodetector. Meantime, through the design of abovementioned pattern, the photodetector will not be limited by the polarization of any incident light, and any polarization of infrared source can be collected effectively. This nontoxic, low-cost photodetector is compatible to current semiconductor process, which not only can reduce the required cost and time of process, but also can break through 1.12 eV energy band gap of silicon substrate. Thus, it is a breakthrough technology for Si-based photodetector photodetector to detect infrared effectively. Similarly, any semiconductor substrate used in the present invention can break through the limitation of energy band gap, and break through the detected wavelength range of semiconductor material.
It is understood that various other modifications will be apparent to and can be readily made by those skilled in the art without departing from the scope and spirit of this invention. Accordingly, it is not intended that the scope of the claims appended hereto be limited to the description as set forth herein, but rather that the claims be construed as encompassing all the features of patentable novelty that reside in the present invention, including all features that would be treated as equivalents thereof by those skilled in the art to which this invention pertains.
Number | Date | Country | Kind |
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103124103 | Jul 2014 | TW | national |
Number | Date | Country | |
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61937764 | Feb 2014 | US |