IMAGE SENSOR
20190230305 ยท 2019-07-25
Assignee
Inventors
Cpc classification
H04N25/713
ELECTRICITY
International classification
Abstract
A CCD image sensor of the type for providing charge multiplication by impact ionisation has an image area and a plurality of pixels. A separate multiplication register has a plurality of multiplication elements arranged to receive charge from the pixels of the image area. Each multiplication element comprises a sequence of electrodes operable to cause multiplication, the electrodes of each multiplication element being adjacent one another and non-overlapping. The non-overlapping arrangement may be manufactured by a CMOS process thereby providing a CCD image sensor with the advantages of CCD multiplication but using a CMOS manufacturing process.
Claims
1. A CCD image sensor of the type for providing charge multiplication by impact ionisation, comprising an image area having a plurality of pixels and a separate multiplication register having a plurality of multiplication elements arranged to receive charge from the pixels of the image area, each multiplication element comprising a sequence of electrodes operable to cause charge multiplication, wherein the electrodes of each multiplication element are adjacent one another and non-overlapping.
2. The CCD image sensor according to claim 1, wherein the electrodes are derived from a single layer.
3. The CCD image sensor according to claim 1, wherein the electrodes are formed by etching.
4. The CCD image sensor according to claim 1, wherein the electrodes and manufactured using a CMOS process.
5. The CCD images sensor according to claim 1, wherein the electrodes are derived from a single layer of polysilicon.
6. The CCD image sensor according to claim 1, wherein each multiplication element comprises a sequence of electrodes on a gate dielectric, wherein the gate dielectric is thinner than 20 nm.
7. The CCD image sensor according to claim 1, wherein the electrodes of each multiplication element have inter-electrode gaps that are narrower than 100 nm.
8. The CCD image sensor according to claim 1, wherein the pixels of the image area are arranged in rows and columns and comprising a single multiplication register arranged to receive charge from the pixels of the image area.
9. The CCD image sensor according to claim 1, wherein the pixels of the image area are arranged in rows and columns and comprising a plurality of multiplication registers, each multiplication register arranged to receive charge from a subset of the pixels of the image area.
10. The CCD image sensor according to claim 9, wherein each multiplication register is arranged to receive charge from a corresponding column of the image area.
11. The CCD image sensor according to claim 9, comprising charge to signal converters arranged to produce a signal from each multiplication register and an output multiplexer arranged to receive the signals and implemented to reduce the number of output connections.
12. The CCD image sensor according to claim 1, wherein the electrodes are on a front face of a substrate and the CCD image sensor is arranged for illumination on the back face thereof.
13. An apparatus comprising a CCD image sensor according to claim 1.
14. (canceled)
15. A camera comprising the CCD image sensor according to claim 1.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0016] Some ways in which the invention may be performed are described in more detail by way of example with reference to the accompanying drawings, in which:
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DETAILED DESCRIPTION
[0029] An embodiment may be an image sensor, a semiconductor-based imaging device, a method of manufacturing a semiconductor-based image sensor or imager device, semiconductor image sensor modules, cameras and other optical devices including semiconductor image sensor modules.
[0030] The present disclosure describes an arrangement that significantly reduces the voltage required to achieve EM gain values compared to traditional EM CCDs. By using low voltage CMOS arrangements for EM elements the voltage level at the HV Gate can be reduced by a factor of at least 2, leading to the added advantage of a reduction of the power dissipation by a factor of at least 4.
[0031] In addition, the electron multiplication is realised outside the photosensitive area of the device, giving higher fill factor and improved quantum efficiency. This allows the photosensitive area to be optimised for only electro-optical performance and in particular for lower dark current. The electron multiplication provides a gain from input to output. Gain uniformity may also be improved in an embodiment due to the use of common gain elements per column or for the whole device. The number of EM elements is reduced in comparison with devices using EM per pixel, resulting in reduced power dissipation.
[0032] In a low voltage CMOS fabrication process, as used in an embodiment, the gate dielectric is much thinner than in traditional CCD technology; typically the CMOS gate dielectric is less than 20 nm thick while in EMCCDs it is usually more than 100 nm thick. For example, the dielectric thickness used may be 12.5 nm in a 5V CMOS process, but the dielectric breakdown voltage may be much higher than 5V. In 3.3V devices the dielectric may be 7 nm thick. In general, the thickness of dielectric in an embodiment is less than 20 nm.
[0033] In such a CMOS fabrication process normally a single polysilicon layer is used to manufacture the gates of the charge transfer structure, and the gaps between electrodes are obtained using deep-submicron etching. This process could achieve inter-electrode gaps below 100 nm. In contrast, traditional CCD technology uses multiple layers of polysilicon as gate electrodes. After each layer of polysilicon is deposited and patterned, its surface is thermally oxidised until a thin layer of silicon dioxide is grown. This oxide insulates any polysilicon layer from any subsequent polysilicon layers deposited on top of it, and forms the inter-electrode gap with the polysilicon serving as various electrodes. Usually, the inter-electrode gap created by polysilicon oxidation has thickness in the range 200 to 300 nm.
[0034] The effects of the thinner gate dielectric and narrower inter-electrode gaps combine to allow the generation of higher electric field at the same applied voltage (or generating higher electric field than possible in traditional designs), thus increasing the EM gain for the same applied voltage. Simulations indicate that the voltage applied to the HV Gate can be reduced by at least a factor of 2 while achieving the same EM gain.
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[0036] Typically CCD processes do not have capability for integrating logic and amplifiers using complementary MOS devices.
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[0041] As can be seen from the steps shown in
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[0043] As discussed above, the embodiment is a CCD image sensor because charge is shifted from one element to another element to achieve transfer from an image area and subsequent multiplication prior to conversion to a signal. However, the techniques for creating the device are typically used to manufacture CMOS devices of the type having signal charge to voltage conversion within each image element.
[0044] An apparatus such as a camera or scientific apparatus embodying the invention is shown schematically in