This invention relates generally to pixels, and more particularly to high dynamic range pixels which employ a capacitive transimpedance amplifier.
High dynamic range (HDR) imaging is finding growing applications in many areas. For example, infrared (IR) imaging applications may require the ability to capture scenes with large variations in irradiance due to object temperatures, while also having to deal with undesirable scene disturbances, due to, for example, sun reflection or laser jamming. Another application is hyperspectral imaging, in which an image sensor looks at objects using a vast portion of the electromagnetic spectrum. In many imaging applications and particularly in hyperspectral imaging using spatial scanning, it is desirable or critical to maintain spatial and temporal coherence while capturing an HDR image. Spatial coherence refers to using the same point in the image sensor (in practice, the same photodiode) to capture the HDR signal. For example, an HDR image formed by combining the signals from two adjacent pixels (one optimized for low signal levels and the other optimized for high signal levels) is not spatially coherent because the HDR image is obtained from different points in space. Temporal coherence refers to capturing the HDR signal at the same point in time. For example, an HDR image formed by combining two sequential frames taken at different exposures is not temporally coherent because the two exposures are not simultaneous and consequently the scene might have changed between the first and second exposure.
One approach to an HDR pixel with spatial and temporal coherence is the visible monolithic pixel described in Sugawa et al., “A 100 dB dynamic range CMOS sensor using a lateral overflow integration capacitor”, 2005 ISSCC. An overflow capacitor is connected to the floating diffusion node of a standard 4T pixel to collect the overflow charge during integration. However, this pixel requires multiple reads (one before integration and one after integration), and has a reduced fill factor and quantum efficiency (QE) because the photodiode, overflow capacitor and the MOS transistors share the same silicon. Furthermore, this pixel is not suitable for detecting wavelengths greater than 1.1 μm because it uses a silicon photodiode.
With an IR photodetector, a capacitive transimpedance amplifier (CTIA) is often interfaced to the detector and used as an integrator. A small integrating capacitor (known as a high-gain capacitor) can be used to achieve low input-referred noise at the expense of limited well capacity. A large integrating capacitor (known as a low-gain capacitor) can be used to achieve large well capacity at the expense of higher input-referred noise. One known approach to implementing an HDR CTIA pixel with spatial and temporal coherence requires the use of a comparator connected to the CTIA output. The CTIA amplifier has high-gain (HG) and low-gain (LG) capacitors, with the comparator switching the LG capacitor in series with the HG capacitor under specified conditions. However, employing a comparator for every pixel results in extra power consumption and requires a significant amount of layout area.
A novel HDR CTIA pixel is presented which provides automatic gain selection, as well as both spatial and temporal coherence.
The present pixel has an associated pixel frame period comprising a reset phase followed by an integration phase. In a preferred embodiment, the pixel comprises an input node for connection to the photocurrent output Iph of a photodiode, and an output node at which a voltage Vout is provided. The pixel includes a CTIA which comprises a first “high gain” (HG) integration capacitor connected between the input and output nodes, a first reset switch connected between the input and output nodes, a second “low gain” (LG) integration capacitor connected between the input node and a first node, a second reset switch connected between the first node and the output node, and a first FET connected across the second reset switch. In operation, the first FET is off during the reset phase, and is conditionally turned on during or after the integration phase. The first and second reset switches are preferably implemented as FETs of a first polarity (for example, both PMOS), and the first FET is preferably of a second polarity opposite of the first polarity (for example, NMOS). The CTIA preferably also includes an amplifier having at least an inverting input port and an output port, the inverting input port connected to the input node and the output port connected to the output node. A pixel as described herein can be operated in several different ways, including “static low-gain control” and “dynamic low-gain control” modes.
These and other features, aspects, and advantages of the present invention will become better understood with reference to the following drawings, description, and claims.
One possible embodiment of the present HDR CTIA pixel is shown in
The present pixel also includes a first FET Mlgn connected across second reset switch 22. In operation, first FET Mlgn is off during the reset phase, and conditionally turns on during or after the integration phase. First and second reset switches 18, 22 are preferably implemented as FETs of a first polarity, and first FET Mlgn is preferably implemented as a FET of a second polarity opposite that of the first polarity. For example, as shown in
The circuit configuration described above can be operated in several different modes. A “static low-gain control” mode is illustrated in
The following analysis assumes that Iph flows into node 12, Mlgn is an NMOS FET and 0<ΔV<Vt, where Vt is the NMOS threshold voltage:
During the reset phase 32, Mrst and Mlgp are on and Vout and Vlg are reset to a predetermined voltage. In a region 36, Mlgn is off and photocurrent Iph is integrated only on Chg. As a result, Vout decreases with time with a slope −Iph/Chg. When Vout=Vclamp−ΔV, Mlgn turns on in weak inversion and operates in saturation. Now Vout is constant and clamped to Vclamp−ΔV, no current flows through Chg, and Iph is integrated entirely on Clg. Consequently, in this region 40, Vlg decreases with time with a slope −Iph/Clg. Then, when Vlg=Vout=Vclamp−ΔV, Mlgn begins to operate in the linear region as a switch that is closed and Vout is unclamped. In this region 42, Iph is integrated on both Chg and Clg and Vout=Vlg and decreases with time with a slope −Iph/(Chg+Clg).
Note that the CTIA can be single-ended or differential (as shown in
If Iph flows out of node 12, Mlgn is a PMOS FET and 0<ΔV<|Vt|, where Vt is the PMOS threshold voltage, the pixel operation is similar to the one described above except that:
A plot of the sampled value of Vout at the end of integration phase 34 versus Iph for the “static low-gain control” mode is shown in
where tint is the integration time.
Vout is in logarithmic region 52 when Iph is greater than
but less than
where ΔVout=Vrst−Vclamp+ΔV. In logarithmic region 52 Vout is essentially independent of the values of Chg and Clg, and decreases logarithmically with Iph:
where k is Boltzmann's constant, T is absolute temperature, q is the charge of the electron, n is a non-ideality factor, and I0 is current proportional to W/L of Mlgn.
When Iph is greater than Iph,2, Vout is in LG linear region 54, in which Vout decreases linearly with photocurrent and is inversely proportional to the sum of Chg and Clg:
As Iph increases further, Vout (Iph) approaches zero and the CTIA pixel saturates. This occurs for approximately 400 pA in
For reference, the following parameters were used in creating the plot shown in
trst=30 μs
tframe=500 μs
tint=470 μs
If Iph flows out of node 12 and Mlgn is a PMOS FET, the behavior of Vout as a function of photocurrent Iph and the associated equations are similar, except that Vout increases with Iph during first linear region 50, logarithmic region 52 and second linear region 54.
Another possible operating mode, referred to herein as “dynamic low-gain control”, is illustrated in
Pixel frame period 62 further comprises a charge redistribution phase 64 following the reset phase 66 and integration phase 68. The pixel frame period 62 is arranged such that:
The pixel operation during the reset and integration phases (66, 68) in “dynamic low-gain control” mode is essentially identical to the one in “static low-gain control” mode. The following analysis assumes that Iph flows into node 12, Mlgn is an NMOS FET and 0<ΔV<Vt, where Vt is the NMOS threshold voltage. During reset phase 66, Mrst and Mlgp are on and Vout and Vlg are reset to a predetermined voltage. Δt the onset of integration phase 68, Mlgn is off and photocurrent Iph is integrated only on Chg. As a result, Vout decreases with time with a slope −Iph/Chg. When Vout=Vclamp−ΔV, Mlgn turns on in weak inversion and clamps Vout to Vclamp−ΔV. The HG CTIA output is the value of Vout sampled just before the end of integration phase 68. During the charge redistribution phase 64, Mlgn is driven with a full-rail gate voltage (Vdd), so that it turns on in strong inversion and operates as a switch that is closed. Consequently, Vlg and Vout become equal and the integrated charge on Chg and Clg is redistributed. For the duration Δt of the charge redistribution phase, Vout=Vlg and decreases with time with a slope −Iph/(Chg+Clg). The value of Vout just before the end of the charge redistribution phase 64 is sampled as the LG CTIA output.
When the CTIA is differential (as shown in
If Iph flows out of node 12, Mlgn is a PMOS FET and 0<ΔV<|Vt|, where Vt is the PMOS threshold voltage, the pixel operation is similar to the one described above except that:
A plot of Vout,hg (the HG CTIA output) and Vout,lg (the LG CTIA output) versus Iph in “dynamic low-gain control” mode is shown in
where ΔVout=Vrst−Vclamp+ΔV. Signal Vout,lg is given by:
As Iph increases further, Vout,lg approaches ground and the CTIA pixel saturates. This occurs for approximately 400 pA in
For reference, the following parameters were used in creating the plot shown in
trst=30 μs
Δt=30 μs
tframe=500 μs
tint=440 μs
The pixels described herein would typically be coupled to additional circuitry to provide a desired functionality. One possible example is shown in
The relative advantages and disadvantages of static and dynamic low-gain control will be discussed next. The primary advantage of static low-gain control is that there is a single pixel output (the sampled value of Vout at the end of integration) which is an HDR signal containing three different regions (as shown in
A HDR CTIA pixel as described herein selectively enables an overflow capacitor (Clg in
In contrast with a visible monolithic pixel, for the present pixel the photodiode can be on a separate layer and can be made of different semiconductor materials (e.g., Si, HgCdTe, InGaAs). With a suitable selection of photodiode material, the HDR CTIA pixel can work over various spectral bands of interest from UV to long-wave IR. An HDR CTIA pixel with a Si photodiode achieves higher optical fill factor and quantum efficiency (QE) than a visible monolithic pixel, especially in the near-IR spectrum. Pixel crosstalk is also lower, because the CTIA amplifier maintains the CTIA input at a virtual ground and therefore the interpixel capacitance does not matter.
The pixel implementations depicted in
The embodiments of the invention described herein are exemplary and numerous modifications, variations and rearrangements can be readily envisioned to achieve substantially equivalent results, all of which are intended to be embraced within the spirit and scope of the invention as defined in the appended claims.