The present invention relates to a novel photo sensor and its preparation method, especially to a novel structure of photo sensor and its preparation method. The present invention discloses semiconductor material for the invented photo sensor and its assembly, and assembly comprising the invented photo sensor, and method for preparation thereof. The present invention discloses a mechanism for photo sensor that provides additional photo sensing region adjacent to surface of photo transistor in order to enhance the sensitivity of photo sensor, as well as process for preparation of the mechanism.
In the conventional photo transistor, taking the NPN type photo transistor as an example, the major photo sensing region locates at the base-collector junction. When the depletion region at the base-collector junction receives incident light, electron-hole pairs are generated. Holes with positive charge are swapped from the depletion region by the built-in electrical field and enter the base region, forming photo current. Such photo current excites greater emitter current and forward biases the base-emitter junction, thus generates a collector terminal current that has a gain.
In the photo transistor as shown in
When light beams project to a semiconductor layer, power of the light would exponentially decay along its penetration depth. As a result, light with the strongest power may be detected at the surface region of the semiconductor layer. If the photo detection region 12a of the photo transistor is positioned at this surface region, better detection efficiency may be obtained. However, the photo detection region of the conventional photo transistor is the depletion region of its base-collector junction, which is not positioned at or close to the surface of the semiconductor layer. Improvements in the photo detection efficiency are needed.
To estimate range of wavelength of detectable light of a semiconductor material, the following formula may be used:
wherein λ is wavelength of detectable light (μm); Eg represents energy band-gap of the semiconductor material (eV).
From the above equation it may be known that, since the energy band-gap of single-crystalline silicon is about 1.12 eV, wavelength of light detectable by conventional pure silicon-based photo transistor is approximately smaller than 1,100 nm. In order to detect grater wavelengths such as 1,310 nm or 1,550 nm, as used in the optical fiber communication system, III-V semiconductor components are used. However, the III-V materials are expensive and their preparation process is not compatible with the most popular silicon base CMOS processes. It is thus necessary to provide a novel photo sensor that is able to detect wavelengths in a range covering what are used in the optical fiber communication systems. It is also necessary to provide a novel photo sensor whose preparation process may be compatible with the most popular silicon base CMOS processes.
The objective of this invention is to provide a novel photo sensor, wherein photo detective region is provided at adjacent to its surface, so to improve the detection efficiency of photo sensors.
Another objective of this invention is to provide a photo sensor with effectively extended range of detectable wavelengths.
Another objective of this invention is to provide a photo sensor whose preparation process may be compatible with popular silicon-based semiconductor processes.
Another objective of this invention is to provide a photo sensor with an enlarged base-emitter junction whereby its light detective region is enlarged.
Another objective of this invention is to provide a photo sensor with modified base-emitter junction, whereby range of detectible wavelength is extended.
Another objective of this invention is to provide a novel process for preparation of photo sensor that is compatible with popular silicon-based semiconductor processes.
Another objective of this invention is to provide a method for preparation of photo sensor that is compatible with the standard Silicon-Germanium BiCMOS process.
According to this invention, a novel photo sensor is disclosed. The invented photo sensor comprises: a first polar semiconductor layer; a second polar semiconductor layer exhibiting a polarity opposite to that of said first polar semiconductor layer, surrounded by said first polar semiconductor layer and having a junction with said first polar semiconductor layer and a region exposed to incident light; a third polar semiconductor layer exhibiting a polarity opposite to that of said second polar semiconductor layer, surrounded by said second polar semiconductor layer and having a junction with said second polar semiconductor layer and a region exposed to said incident light; a fourth polar semiconductor layer exhibiting a polarity opposite to that of said second polar semiconductor layer, surrounded by said second polar semiconductor layer and having a junction with said second polar semiconductor layer and a region exposed to said incident light; and necessary electrodes to pick up photo detection signals from said photo sensor; wherein said third polar semiconductor layer and said fourth polar semiconductor layer are isolated.
The equivalent circuit of the invented photo sensor may be understood as a conventional photo transistor integrated with a surface photo sensor. The structure of the surface photo sensor is in substance identical with the emitter-base structure of the photo transistor and may be prepared in the preparation of the photo transistor. The depletion region at junction of the surface photo sensor is positioned at adjacent to the light incident surface of the element, so to detect incident light at its surface regions and to generate electron-hole pairs in a larger quantity. When an N-P-N type photo transistor is included in the photo sensor of this invention, holes generated by incident light may enter the base of the photo transistor directly. As a result, greater output current may be obtained at the collector of the photo transistor. This invention also discloses semiconductor material comprising the invented photo sensor, assembly comprising the invented photo sensor and methods for preparation of said photo sensor, said semiconductor material and said photo sensor assembly.
These and other objectives and advantages of this invention may be clearly understood from the detailed description by referring to the following drawings.
The followings are detailed description of the photo sensor of the present invention, when implemented under the basic structure of a P-N-P type photo transistor.
As known by those skilled in the art, in the semiconductor material as shown in
Now refer to
In the preparation of the semiconductor material of
Thereafter, at 53 an N layer 32 is formed in the first P layer 33 at selected areas. In this embodiment, N layer 32 is surrounded by the first P layer 33. The N layer 32 may be formed by doping impurities using any available method, including thermal diffusion and ion implantation. It is also possible to form the N layer 32 above selected areas within the area defined by the first P layer 33. When forming the N layer 32, any applicable method may be used. For example, it is possible to deposit a material layer on the first P layer 33 and then dope in the added material layer to perform the negative polarity. It is also possible to dope the added material layer during its preparation, so to form the N layer 32 directly. Here, any available method in forming and doping the material layer may be applied. The process in this step is similar to that of step 52. Detailed description is thus omitted. The N layer 32 so obtained will function as base 42 of the photo sensor.
Further, at 54 second P layer 31 and third P layer 34 are formed in selected areas within the area defined by the N layer 32. Method to form the second and third P layers 31, 34 may be similar with that of the previous step, provided that dopants used in this step are different from that of Step 53. In the present invention, second and third P layers 31 and 34 are isolated without contacts between them.
In the above-described process, all reaction conditions may be determined according actual needs. Materials of the substrates of the first P layer, the N layer, and second and the third P layers may be identical or different. Dopants added to first, second and third P layers may be identical or different. However, if substrate materials and dopants for second and third P layers are identical, number of steps in the process and preparation costs may be reduced. This, of course, is not any requirement or limitation. In some preferred embodiments, material of first P layer 33 may be crystalline silicon. Material for N layer 32 may be SiGe. Material for second and third P layers 31, 34 may be poly silicon. The second and third P layers 31, 34 may function as emitter layer and surface photo sensor electrode of the invented photo sensor, respectively, depending on electrodes connected thereto and concentrations of dopants.
At 55, electrodes 43, 42, 41 and 44 are connected to the first P layer 33, the N layer 32 and the second and third P layers 31 and 34 of the photo sensing semiconductor material so prepared. The photo sensor is thus prepared. The electrodes may be connected to the related layers using any applicable method, including screen printing, deposition, spitting, vapor deposition, plating etc. The photo sensor so prepared may contain a plurality of photo sensor units prepared in wafer. Therefore, at 56 the wafer is cut to obtain units of photo sensor and the units are packaged at 57.
In some embodiments of this invention, electrodes are connected to the photo sensing semiconductor material after cutting. In addition, it is possible to form particular wires to connect a plurality of photo sensors before they are cut. Furthermore, in some other embodiments, the substrates are prepared from transparent materials. In some further embodiments a reflection layer (not shown) is provided at the lower surface (non-incident side) of the substrate 30 to further enhance its photo sensing effects. It is also preferable to prepare the electrodes using transparent materials such as ITO and TO.
The photo sensor so prepared has two depletion regions to detect incident lights and to convert such lights into current outputs. If compared with the conventional photo transistor, the invented photo sensor provides an additional junction 32b between its N layer 32 and third P layer 34, in addition to the junction 32a between its base and collector. As a result, no matter the incident light is visible light with short wavelengths (such as 400-700 nm) or long wavelength light (such as light waves with the wavelength of 1,310 nm as used in the optical fiber communication system), they may effectively detected by the invented photo sensor.
Nevertheless, the equivalent circuit of the invented photo sensor includes a photo transistor (including first P layer, N layer and second P layer in the above example) and a surface photo sensor (including third P layer and N layer). In them, one terminal of the surface photo sensor happens to be base of the photo transistor. When the incident light reaches the surface photo sensor, carriers (electrons) so generated will enter the base directly, so that amplified currents are output from collector of the photo transistor. The photo reaction efficiency of this invention is thus far higher than that of the conventional photo transistors.
The photo sensor of this invention may be prepared by using the standard SiGe BiCMOS process. No special process modification is needed. In the process, the structure of the surface photo sensor and the emitter-base structure of the photo transistor are identical and may be prepared simultaneously. The process is thus made simplified. With the invented structure, the junction depletion region of the SiGe surface photo sensor locates at the SiGe region. Since the energy band-gap of the SiGe material is smaller than that of pure silicon, the SiGe surface photo sensor of this invention may be used to detect lights with longer wavelengths. As a result, the detectable range may be extended to include infrared wavelengths, whereby the invented photo sensor may be used in the optical fiber communication system.
In addition, in the circuit of
In the photo sensor of this invention, the emitter of the photo transistor does not provide any photo detection function. Therefore, it is preferable to reduce the area of the emitter in the light incident surface. On the other hand, the region of the surface photo sensor is preferably expanded to as much as possible in order to further enhance the photo detective effects. In some embodiments of the present invention, the region of the surface photo sensor electrode has a ring shape and surrounds the emitter region. Such design may further increase the photo detective effects of this invention.
As the present invention has been shown and described with reference to preferred embodiments thereof, those skilled in the art will recognize that the above and other changes may be made therein without departing from the spirit and scope of the invention.