The invention relates to a time-of-flight pixel with a charge storage below the modulation gates and a time-of-flight sensor comprising corresponding pixels.
The time-of-flight sensor according to the invention is used in particular in time-of-flight camera systems which obtain distances from the phase shift of emitted and received radiation. As time-of-flight or 3D cameras in particular PMD cameras with photomixing detectors (PMD), such as those described in DE 197 04 496 A1 are suitable.
It is an object of the invention to reduce the space requirement of a time-of-flight pixel in the time-of-flight sensor.
The time-of-flight pixel according to the invention solves this object and enables the demodulation and storage of the photogenerated charge carriers under a single photogate to be carried out. This results in a significant reduction of the space requirement.
The figures schematically show:
The idea according to the invention, as sketched in
In addition, a drain gate GD with attached drain diode DD allows the defined suppression of the integration below the storage regions MA, MB.
On a semiconductor substrate, which has a suitable doping of p- or n-type, two photogates GA, GB form a photoactive area FAB disposed centrally in a time-of-flight pixel. Below the photogates GA, GB and bounding the photoactive area FAB storage regions MA and MB are arranged in the semiconductor substrate, wherein the photogates GA, GB only partially cover the storage regions MA, MB.
Adjacent to the memory regions MA, MB the respective transfer gates TXA and TXB are disposed, which in turn are adjacent to the readout diodes DA and DB. In a vertical or perpendicular direction to photogate GA, GB, transfer gate TXA, TXB and diodes DA, DB, a drain gate (GD) is arranged, which connects the mixer area or the photoactive area FAB of the photogates GA, GB with a drain diode DD (discard node) in a switchable manner.
The storage regions MA, MB are preferably produced partially below the photogates GA, GB with the aid of an enhanced n-type implantation. These implantations lead to a local increase of the electrostatic potential below the photogates GA, GB. These areas can be used as storage region MA, MB for intermediate storage of the demodulated photoelectrons.
Thus, a double functionality is achieved with the photogates GA, GB: On the one hand the demodulation of the photogenerated charge carriers and on the other hand the intermediate storage of these charge carriers, in order to achieve a functionality according to the principle of correlated double sampling with simultaneous global electronic aperture (global shutter). The structure can be used both for a front side illumination FSI as well as for a back side illumination BSI of the pixel.
During integration the transfer gates TXA and TXB are kept at low potential, thus separating the storage regions MA and MB from the readout diodes DA and DB. Drain gate GD is also at low potential and separates the drain contact from the mixer area or the photoactive area FAB. The photogates GA and GB form the sufficiently known charge carrier swing. The correspondingly demodulated photogenerated charge carriers enter the storage regions MA and MB, respectively. In the further course of the integration phase, the charge carriers stored there can escape neither in the direction of the readout diode DA, DB nor in the direction of the photoactive area FAB. The storage capability of the storage regions MA, MB is thus independent of the voltage applied to the photogates GA, GB. Thus, there is a continuous integration of charge carriers in the storage regions MA, MB during the integration phase.
In the hold mode both photogates GA, GB are kept at low potential and the transfer gates TXA, TXB decouple the storage regions MA, MB from the readout diodes DA, DB. In order to prevent further integration of charge carriers in the storage regions, the drain gate GD is now switched to a high potential, resulting in a direct connection of the mixer region GA, GB with the drain diode DD. The photogenerated charge carriers are now discharged in the direction of the drain diode DD, i.e. they are no longer available for further integration in the storage regions MA, MB.
The readout mode is used to transfer the charge carriers integrated below the storage regions MA, MB in the direction of the readout diodes DA and DB. For this purpose, photogates GA and GB are kept at low potential. The drain gate GD is also kept at high potential and discharges all charge carriers photogenerated during the readout mode towards the drain diode DD.
The transfer gates TXA and TXB are now switched to a high potential, resulting in a formation of a potential gradient in the direction of the readout diodes DA, DB. This causes the charges stored in the storage regions MA, MB to flow towards the readout diodes DA, DB. With an appropriate timing, the readout can be performed as a noise-reduced correlated double sampling, CDS.
In principle, designs with more than two diode nodes are also conceivable.
The scattering elements SR can be combined with optical isolation elements ISO, as shown in
Number | Date | Country | Kind |
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10 2020 132 868.0 | Dec 2020 | DE | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2021/080373 | 11/2/2021 | WO |