This application claims the priority benefit of French Application for Patent No. 1451651, filed on Feb. 28, 2014, the contents of which is hereby incorporated by reference in its entirety to the maximum extent allowable by law.
The present disclosure relates to photodetectors formed in a semiconductor layer formed of one or a plurality of conductive materials, the semiconductor layer being of SOI (semiconductor-on-insulator) type.
For certain applications, particularly in photonics, it is desirable to have a photodetector formed in an SOI-type semiconductor layer with a transverse illumination.
An embodiment provides a photodetector formed in an SOI-type semiconductor layer, the photodetector comprising a first region and a second region of a first conductivity type separated from each other by a central region of the second conductivity type, and a transverse surface submitted to an illumination extending orthogonally to the upper surface of the central region.
According to an embodiment, the first conductivity type is type N and the second conductivity type is type P.
Another embodiment provides a method of using the photodetector, wherein a ground voltage is applied to the first region and a positive voltage is applied to the second region, the central region being left floating.
According to an embodiment, a contact is arranged on the upper surface of the central region.
According to an embodiment, a contact is arranged astride the first region and the central region.
According to an embodiment, the first region is interrupted by an extension of the central region and a contact is arranged on the upper surface of the extension.
According to an embodiment, the first region and the second region are interrupted by extensions of the central region and a contact is arranged on the upper surface of each extension.
Another embodiment provides a method of using the photodetector, wherein a positive voltage is applied to the second region and a ground voltage is applied to the first region and to the central region.
The foregoing and other features and advantages will be discussed in detail in the following non-limiting description of specific embodiments in connection with the accompanying drawings, wherein:
For clarity, the same elements have been designated with the same reference numerals in the various drawings and the various drawings are not to scale.
The photodiode comprises a heavily-doped P-type semiconductor layer 9 (P+) and a heavily-doped N-type semiconductor layer 11 (N+) longitudinally extending on either side of a lightly-doped P-type central region 12 (P−).
When the photodiode is reverse-biased and light rays reach its upper surface, electron-hole pairs are created in regions 12 and 13 and a current is generated.
In the photodiode of
The phototransistor comprises two heavily-doped N-type semiconductor regions 21 and 23 (N+) longitudinally extending on either side of a lightly-doped P-type central region 25 (P−). Metal contacts 27 and 29 rest on the upper surfaces, respectively, of region 21 and of region 23. Regions 21, 25, and 23 respectively form the phototransistor emitter, base, and collector.
In operation, light rays originating from a source 31 (waveguide or optical fiber) illuminate a transverse surface of region 25 of the phototransistor. The photo-transistor is biased by the application, for example, of a ground voltage to contact 27 and of a positive voltage, for example, 1 V, to contact 29. The base is left floating (that is, is not connected). When light rays reach the transverse surface of base region 25, electron-hole pairs are created and a current is generated.
In such a phototransistor, all the light rays reaching the transverse surface of base region 25 are capable of creating electron-hole pairs taking part in the generation of a current, conversely to the case of a photodiode of the type in
Curve 33 illustrates the dependence between current I generated by a photodiode of the type in
For bias voltages V in the range from 0.1 to 1 V, current I generated in the phototransistor (curve 35) is greater than the current generated in the photodiode (curve 33).
In the variation of
In the variation of
In the variation of
In the variation of
In operation, base region 25 of each of the phototransistors of
Referring again to
Current I of the floating-base phototransistor of
Although current I of curves 37 and 39 is lower than that of curve 35, the biasing to the same voltage of the base and of the emitter of the phototransistors of curves 37 and 39 results in a cut-off frequency of these phototransistors much higher than that of a floating-base transistor of the type in
Further, current I of curve 39 is almost constant whatever bias voltage V while current I of curves 35 and 37 increases along with bias voltage V. Thus, a phototransistor of the type in
In the phototransistors of
A dimension of a region or of a portion will be considered as being its width if this dimension is parallel to the illuminated transverse surface, and to the upper surface of the SOI-type semiconductor layer, and will be considered as its length if this dimension is orthogonal to the illuminated transverse surface. As an example of dimensions, the width of region 25 is in the range from 0.3 to 0.5 μm, for example, 0.4 μm. The width of regions 21 and 23 may be in the range from 0.2 to 0.4 μm, for example, 0.3 μm. The length of regions 21, 23, and 25 may be in the range from 2 to 30 μm, for example, 15 μm. The length of extension 61 and of an extension 71 may be in the range from 0.5 to 3 μm, for example, 1.5 μm. The thickness of the semiconductor layer may be in the range from 0.2 to 0.5 μm, for example, 0.3 μm.
In an optoelectronic technological process, the forming of layers, regions, or portions having different doping levels is usually provided, the available doping concentrations will for example be:
Specific embodiments have been described. Various alterations and modifications will occur to those skilled in the art. In particular, the conductivity types of emitter, base, and collector regions 21, 25, and 23 indicated as an example in relation with the above embodiments may all be reversed, the bias voltages being reversed. The doping levels of the regions and of the areas indicated as an example may be adapted according, for example, to the various technological processes used.
The dimensions of the regions, of the extensions of regions, and of the areas indicated as an example may be adapted according, for example, to the wavelength of the received light rays.
More generally, the topography of the regions, of the extensions of regions, of the overdoped areas, and of the phototransistors described hereabove may be modified by those skilled in the art. In particular, it will be within the abilities of those skilled in the art to adapt the number of contacting areas and the number of metal contacts according to the length of the base region.
Such alterations, modifications, and improvements are intended to be part of this disclosure, and are intended to be within the spirit and the scope of the present invention. Accordingly, the foregoing description is by way of example only and is not intended to be limiting. The present invention is limited only as defined in the following claims and the equivalents thereto.
Number | Date | Country | Kind |
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1451651 | Feb 2014 | FR | national |