Patent Application
20100289107
The present application claims priority from French Application for Patent No. 09 53289 filed May 18, 2009, the disclosure of which is hereby incorporated by reference.
The invention relates to the field of photodiodes and more particularly to photodiodes produced in matrices.
Photodiode technology relies on two key parameters.
The first parameter is the sensitivity of the photodiode, which represents the capacity of the photodiode to collect photogenerated charge carriers. This parameter controls the intensity of the current generated for a given illumination.
The second parameter is the dark current, which represents the current flowing through the photodiode when no light illuminates the photodiode. This parameter controls the difference in intensity of the current generated for a given difference in illumination.
A relatively large portion of the electrons generated in the photodiode do not contribute to the photocurrent as they are trapped by structural defects or recombination zones. Likewise, in the case of photodiode matrix sensors, the reduction in size creates influencing effects between adjacent photodiodes, degrading the performance of all the diodes.
In this regard, the reader may refer to the document “Deep Trench isolation for crosstalk suppression in active pixel sensors with 1.7 nm pixel pitch”, by B. J. Park et al., Japanese Journal of Applied Physics, Vol. 46, No. 4B, 2454-2457 (2007), the disclosure of which is incorporated by reference, which describes the production of deep isolation trenches and their use in matrix photosensors so as to limit neighboring effects.
However, deep isolation trenches may play a similar role to structural defects or recombination centers. It will be recalled that recombination centers destroy charge carriers by combining them with carriers of opposite charge, for example by combining holes with electrons.
This is because deep isolation trenches generally comprise an insulating material and are produced in a semiconductor medium. Moreover, an inherent property to silicon/oxide or silicon/nitride interfaces is to have a positive surface charge capable of attracting the photogenerated electrons. It will therefore be understood that deep isolation trenches act as traps for the photogenerated electrons.
It is therefore desirable to minimize or eliminate the trapping of photogenerated electrons in the vicinity of the deep isolation walls.
There is also a need for a device of the photodiode type in which the trapping of the photogenerated electrons in the vicinity of the deep isolation walls is minimized or eliminated.
In an embodiment, a photodiode comprises a first doped layer and a second doped layer that have a common face, at least one deep isolation trench having a face contiguous with the first doped layer and the second doped layer, and wherein a free face of the second doped layer is in contact with a conducting layer.
This photodiode furthermore includes a protective layer capable of generating a layer of negative charge at the interface between, on one side, the first doped layer and the second doped layer and, on the other side, the deep isolation trench.
The protective layer may be produced by implantation of p-type doping species.
The protective layer may be produced by implantation of species chosen from boron and indium.
The protective layer may also include implanted carbon.
According to another aspect, a process is presented for producing at least one deep isolation trench, each deep isolation trench being produced between two photodiodes made from a structure comprising a first doped layer and a second doped layer that have a common face, a free face of the second doped layer being in contact with a conducting layer. The process includes a step during which: a protective layer is formed by implanting a species at the interface between, on one side, a first doped layer and a second doped layer and, on the other side, the deep isolation trench, the implanted species having the property of creating a layer of negative charge in contact with the doped silicon.
The implanted species may be a p-type doping species.
The implanted species may be chosen from boron and indium.
Carbon may also be implanted at the interface during formation of the protective layer.
At least two different species chosen from the implanted species may be co-implanted.
Other objects, features and advantages will become apparent on reading the following description given solely by way of non-limiting example and with reference to the appended drawings in which:
The photodiode 1 thus described is generally intended to be integrated into a matrix sensor. It is therefore necessary to isolate a given photodiode from the neighboring photodiodes. To do this, deep isolation trenches 4 are formed so as to separate two immediately adjacent photodiodes. The deep isolation trenches (DTIs) 4 are made of an insulating material.
Moreover, the external face of the photodiode is protected from the outside by a passivation layer 6, also made of an insulating material.
A space charge zone, in which the incident electromagnetic radiation may be absorbed, is created at the interface between the first layer 2 and the second layer 3. The absorption then gives rise to the creation of electron-hole pairs. The electrons and holes each migrate in opposite directions under the effect of the electric field in the space charge zone. The displacement of the photogenerated electrons and holes thus gives rise to the creation of a photoelectric current.
As described above, the deep isolation trenches 4 are generally made of an insulator of the oxide or nitride type and have the property of generating a positive charge at the interface with a semiconductor. In the case of the photodiode described in
It is proposed to produce a protective layer 7 illustrated in
The protective layer 7 is created by the ion implantation of p-type doping species at the interface between, on one side, the doped silicon of the first layer 2 and of the second layer 3 and, on the other side, the dielectric of the deep isolation trench. The implanted ions must remain localized at the interface so as not to disturb the operation of the active zones. To do this, carbon is also implanted, which has the property of minimizing the diffusion of boron and indium (or other element) into the silicon. Thus, during the thermal annealing steps, the implanted species remain localized at the interface between the silicon and the deep isolation trenches.
The implanted species are p-type dopants and may in particular be boron or indium or other element.
The implantation takes place at an angle α to the normal to the surface of the silicon layers. The angle α may be between 2° and 26°.
The dose is between 1011 and 1013 at.cm˜2.
The implantation energy is between less than 1 keV and 25 keV.
The features of a photodiode that includes deep isolation trenches are improved by implanting a protective layer so that a negative charge zone appears at the interface between the silicon and the deep isolation trench. By preventing the recombination of photogenerated electrons, the protective layer makes it possible to improve the contrast, the dark current and the intensity of the photogenerated current.
| Number | Date | Country | Kind |
|---|---|---|---|
| 0953289 | May 2009 | FR | national |
