The invention relates to photodiode arrays, and more particularly to photodiode arrays based on indium-gallium arsenide (InGaAs) and indium phosphide (InP), as well as to their manufacturing process.
One of the methods for manufacturing photodiodes in semiconductor materials with a small band gap (often for infrared light detection) consists of inserting the detection active small band gap layer between two large gap semiconductor materials. Both large band gap semiconductor layers are an efficient protection/passivation while remaining transparent to the wavelength of the radiation intended to be detected by the photodiode.
Further, with suitable dopings, both heterojunctions between the active layer and the two protection/passivation layers confine photoelectric charges in the active detection layer and improve the quantum yield of the thereby built photodiode.
An InGaAs photodiode is a typical example of this critical structure. The detection active layer consisting of InGaAs material may have an adjustable band gap depending on the indium, and gallium composition in InGaAs, ideal for operating in the SWIR (Short Wave Infra-Red) band of the order of 1.4 to 3 μm.
Indium phosphide and indium-gallium arsenide have the same face centered cubic crystalline structure. The most used composition is In0.53Ga0.47As. The crystalline lattice size is then comparable with that of the InP substrate, notably the lattice parameters. This crystalline compatibility allows growth by epitaxy of an active InGaAs layer of excellent quality on an InP substrate. The band gap of In0.53Ga0.47As is of about 0.73 eV, capable of detecting up to a wavelength of 1.68 μm in the SWIR band. It has a growing benefit in fields of applications such as spectrometry, night vision, sorting of used plastics, etc.
Both protection/passivation layers are generally made in InP. Especially as the composition In0.53Ga0.47As, has the same crystalline lattice size as InP, this allows a very low darkness current from room temperature onwards.
The individual anodes 3 are formed by local diffusion of zinc (Zn). The dopant Zn crosses the thin passivation InP layer 6 and penetrates into the active InGaAs layer 5.
With a detector operating in an integration mode, an output signal is obtained proportional to the product of the flux and of the exposure time. However, the output signal is limited by the maximum integration capability of the sensor. For scenes with high contrast, it is often impossible to obtain good rendering of dark areas and at the same time to keep bright areas without any saturation. This problem is all the more serious for night vision for which an array sensor with InGaAs photodiodes is often intended.
Another way of reading the photoelectric signals from photodiodes, in a general way, is proposed by document EP 1 354 360 and illustrated in its principle by
In this operating mode, the photodiode 51 does not receive any external bias and it is forward-biased by the photoelectric charges generated in its junction. The direct bias voltage observed on the photodiode is proportional to the logarithm of the incident light flux.
This logarithmic response gives the possibility of covering without any electrical and optical adjustment, an operating dynamic range of more than 120 dB, indispensable for using a SWIR InGaAs sensor under natural conditions outdoors. Document EP 1 354 360 also proposes association of a switching readout circuit 55 with the photodiode.
The principle of use of the image sensor array illustrated in
By means of the second readout, zero voltage corresponding to the darkness condition is generated. This electronic darkness signal gives the possibility of suppressing signal offsets in the readout chain in an array detector.
The principle proposed by EP 1 354 360 was applied in an InGaAs sensor and operates perfectly. But a blooming phenomenon is observed for daylight scenes. This phenomenon may simply be described as a loss of spatial resolution in an image. The detector nevertheless continues to be sensitive to variation of light according to the logarithmic law. This phenomenon is not observed in other types of photodiodes such as those based on silicon, InSb or MCT.
The present invention proposes a simple and efficient solution to this blooming phenomenon in an array of InGaAs photodiodes. The solution proposed by the present invention also allows an improvement in image quality in a conventional detector in an integration mode.
For this purpose, according to a first aspect, a method for manufacturing an array of photodiodes is proposed, comprising:
The invention according to the present aspect is advantageously completed by the following features, taken alone or in any one of their technically possible combinations:
Preferably the doping depth N is comprised between 0.5 μm and 2 μm.
According to a second aspect, the invention also relates to an array of photodiodes comprising:
The invention according to the second aspect is advantageously completed by the following features, taken alone or in any of their technically possible combinations:
The invention also relates according to a third aspect to an image sensor incorporating a readout circuit and an array of photodiodes according to a second aspect. Preferably, the readout circuit is a logarithmic circuit.
Other aspects, objects and advantages of the present invention will become better apparent upon reading the detailed description which follows. The invention will also be better understood with reference to this description considered together with the appended drawings, given as non-limiting examples and wherein:
In a structure of the state of the art as illustrated by
The lateral parasitic PN junctions 32 between the anodes 3 and the passivation layer 6 form a possible electric flow path between the neighboring photodiodes via the passivation layer.
A conventional readout circuit integrates, in a capacitor, the reverse current in the photodiode by applying a reverse bias to the latter. In this configuration, the lateral parasitic junctions 32 in the photodiodes are reverse-biased at the same time with the effect of adding an additional parasitic current in the integration capacitor. This parasitic current degrades the image quality, but does not quasi-generate any cross-talk between the neighboring photodiodes. These parasitic currents may be partly compensated for by complex image processing operations on the raw image coming from the readout circuit.
When a photodiode operates in the solar cell mode, the junction is forward-biased by the incident light. In this case, the lateral parasitic junction 32 are also forward biased and they form a passage for electric current between neighbouring photodiodes. This forward-biasing becomes all the more significant since the incident light intensity increases, thereby generating a blooming phenomenon which considerably degrades the spatial resolution of the sensor.
The present invention proposes a structure allowing suppression of lateral conductivity in an array of InGaAs photodiodes. An array of photodiodes manufactured according to the present invention may be used in a solar cell mode as described in document EP 1 354 360, without any loss of spatial resolution, even in the presence of very strong light intensity. Such an array also provides improvement in the image quality with a conventional readout circuit in an integration mode, such as for example the different readout circuits CMOS ISC9705 and ISC9809 marketed by Indigo/FLIR in the USA. The circuit ISC9705 integrates the photoelectric current from a photodiode directly on a capacitor (direct injection mode) and circuit ISC9809 integrates the photoelectric current through an operational amplifier (CTIA mode). The CTIA mode allows a more significant charge-voltage conversion gain which promotes detection sensitivity.
first selective etching is applied (step S4) in order to suppress on the whole of its thickness an area 10 of the passivation layer 6 surrounding each anode 3. This first selective etching selectively suppresses the passivation layer 6 as far as the active layer 5.
The InP layers are of type N, doped with silicon. The active layer 5 of InGaAs may be slightly N-doped or may remain quasi-intrinsic. Therefore the two lower/upper InP layers and the active InGaAs layer 5 form the common cathode of the photodiodes in this array.
Suppressing by the first etching, at each anode 3, an area 10 of the passivation layer 6 surrounding each of said anodes 3 gives the possibility of suppressing the lateral electric passage between neighboring anodes 3 formed by neighboring Zn dopings.
This first etching is preferably chemical etching, achieved by means of a first selective chemical etching agent, preferably a solution of hydrochloric acid and of phosphoric acid, of formula HCl:H3PO5.
The HCl:H3PO5 solution allows selective dissolution of the passivation layer 6 consisting of indium phosphide InP and etching to be stopped upon reaching the active layer 5 consisting of indium-gallium arsenide InGaAs. By this etching selectivity, suppression of the passivation layer 6 may be obtained in a simple way.
The area 10 of the passivation layer 6 surrounding each of the anodes 3, to be suppressed, does not have to be large and may be limited to the accuracy of the lithography. Therefore, this area 10 may be kept quite far away from the Zn diffusion forming an anode 3, in which is found the region for capturing photoelectric charges. Thus, preferably, the first selective etching suppresses an area 10 sufficiently far away from the anodes 3 so that this first selective etching does not reach the PN junction between the anode 3 of type P and the passivation layer 6 of type N.
This first etching is preferably chemical etching but it may optionally be dry etching, for example plasma etching. Chemical etching is however preferred since it does not cause any physical damages in the etching area. In every case, the defects generated by this first etching only have a small impact on the darkness current of the photodiode, since they are sufficiently distant from the diffusion areas of the zinc.
Passivation based on an insulator such as silicon nitride SiNx or silicon dioxide SiO2 may be applied following this etching. However, passivation based on an insulator does not allow sufficient reduction in the number of interface defects.
Therefore, passivation is preferably applied (step S6) by N-type doping of the etching areas 11 of the passivation layer 6 and of the active layer 5 exposed by the first etching. The structure after this N doping is illustrated by
The N-doping depth of said regions 11 may be controlled between 0.5 μm and 2 μm, notably depending on the type of etching, either chemical or dry etching, and on the size of the photodiode. The surface generation is rapidly recombined in the N doping region. The heterojunction formed by this N doping inside the active InGaAs layer 5 repels the photoelectric charges towards the Zn diffusion area, i.e. the capture area. Therefore the quantum yield is thereby improved.
A doping of type P on the surfaces exposed by the etching forms a parasitic junction which drains the photoelectric charges towards the exposed surface. If the surface generation of electron/hole pairs is confined, the quantum yield suffers from this drainage towards the surface through this parasitic junction. Thus, passivation is advantageously carried out by means of N-type doping rather than P-type doping.
Preferably, prior to this passivation by N-type doping, second selective etching is applied, suppressing over the whole of its thickness an area 20 of the active layer 5 surrounding each anode (step S5), being aware that after the first etching of the passivation layer 6, the active layer 5 is exposed at areas 10 surrounding each of the anodes, as illustrated by
Indeed, selective suppression of areas of the passivation layer 6 around each anode 3 of a photodiode suppresses lateral conductivity between neighboring photodiodes. But lateral propagation of the photoelectric charges in the active indium-gallium arsenide InGaAs layer 5 may also degrade the spatial resolution of a sensor incorporating such a photodiode array. Partial suppression of the InGaAs active layer 5 around the Zn diffusion may be highly beneficial for the spatial resolution of the InGaAs sensor.
This second etching, which suppresses over the whole of its thickness a crown 20 of the active layer 5 in indium-gallium arsenide InGaAs around the Zn diffusion, is also preferably chemical etching and applied by means of a second selective chemical etching agent. For this second etching, an aqueous solution comprising sulfuric acid and hydrogen peroxide of formula H2SO4:H2O2:H2O is preferably used. Such a solution selectively etches only the active layer 5 consisting of indium-gallium arsenide InGaAs but preserves indium phosphide making up the passivation layer 6 and the substrate 4.
Thus, each photodiode may be completely insulated from the others.
Further, this second etching by means of H2SO4:H2O2:H2O is beneficial for forming a thin layer protecting the structure against ambient oxidation.
Similarly to the foregoing, if this second etching is preferably chemical etching, it may optionally be dry etching, for example plasma etching. Chemical etching is however preferred since it does not cause any physical damages in the etching area. In every case, the defects generated by the second etching have little impact on the darkness current of the photodiode, since they are sufficiently distant from the zinc diffusion areas.
Passivation based on an insulator such as silicon nitride SiNx or silicon dioxide SiO2 may be applied following this etching. However passivation based on an insulator does not allow sufficient reduction in the number of interface defects.
Thus, similarly to the one discussed above, passivation by N-doping of the etched areas of the passivation layer 6 and of the active layer 5 exposed by the first and second etchings is then applied (step S6).
A photodiode array structure 101 of the type illustrated by
Thus, an array 101 of photodiodes is obtained, each comprising:
with further an indium phosphide passivation layer 6 of type N in which are at least partly formed the anodes 3 by diffusion of a dopant of type P, including areas 10 surrounding each anode in which said passivation layer 6 is absent over the whole of its thickness.
Preferably, the array 101 has areas 20 surrounding each anode 3 in which said active layer 5 in indium-gallium arsenide is absent over the whole of its thickness.
Once the array of photodiodes is without any lateral conduction, the same manufacturing method for metallization and mounting as a chip turned upside down (flip-chip) with a readout circuit of a silicon substrate, may be found again.
Preferably, the readout circuit 2 is a logarithmic readout circuit as described above and discussed in
Number | Date | Country | Kind |
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11 56290 | Jul 2011 | FR | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/EP2012/063596 | 7/11/2012 | WO | 00 | 4/17/2014 |
Publishing Document | Publishing Date | Country | Kind |
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WO2013/007753 | 1/17/2013 | WO | A |
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