Column-Level CDS Charge Transfer Amplifier for Low-Noise Image Sensors

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Solution Overview

Problem

Conventional CMOS image sensors face challenges in reducing 1/f noise and random telegraph noise due to capacitive coupling between the floating diffusion and transfer gate, limiting the minimum required settling time and increasing readout noise, especially in low-light and photon-counting applications.

Innovation Solution

Incorporating a doped pinning region within or adjacent to the floating diffusion to reduce effective capacitive coupling between the floating diffusion and the transfer gate, and optionally the reset gate, to create a pinned transfer gate and/or reset gate, which isolates the charge transfer path from the surface region, thereby reducing overlap parasitic capacitance and voltage feed-through.

Engineering Contradictions & Design Principles

VSEngineering Contradiction Analysis

1Reliability

If conventional CMOS image sensors are used with standard capacitive coupling between floating diffusion and transfer gate, then the structure is simple and easy to manufacture, but the readout noise is high due to 1/f noise and random telegraph noise

Engineering Contradiction:
Improvereadout noise levelVSAvoidpixel structure complexity
Core Design Contradiction:
ReliabilityVSDevice complexity

Solution Approach 1:

The pixel structure is segmented into distinct regions: a first doped region for charge storage, a second doped region for low-noise amplification, and an isolated floating diffusion region. This segmentation separates the charge transfer path from the surface region, reducing parasitic capacitance and noise coupling between the floating diffusion and transfer gate.

Inventive Principle:
Principle #1Segmentation

Solution Approach 2:

Different doped regions are created with specific doping types and concentrations optimized for their local functions. The first doped region has properties optimized for charge storage, the second for low-noise operation, and the floating diffusion is isolated to minimize noise coupling. Each region has tailored electrical properties to reduce 1/f noise and random telegraph noise locally.

Inventive Principle:
Principle #3Local quality

2Productivity

If the settling time is reduced to improve imaging speed, then the productivity increases, but the noise reduction effectiveness decreases

Engineering Contradiction:
Improveimaging speedVSAvoidnoise reduction effectiveness
Core Design Contradiction:
ProductivityVSReliability

Solution Approach 1:

The harmful parasitic capacitance and noise coupling are extracted from the system by isolating the floating diffusion region from the transfer gate through separate doped regions. This extraction removes the source of 1/f noise and random telegraph noise, allowing fast settling without compromising noise reduction.

Inventive Principle:
Principle #2Taking out (Extraction)

Solution Approach 2:

The first and second doped regions act as intermediary structures between the charge storage node and the floating diffusion. These intermediary regions provide a controlled charge transfer path that is electrically isolated from the floating diffusion, enabling fast charge transfer while preventing noise coupling.

Inventive Principle:
Principle #24Intermediary (Mediator)

3Speed

If the capacitive coupling between floating diffusion and transfer gate is increased to improve charge transfer efficiency, then the charge transfer speed increases, but the voltage feed-through and readout noise increase

Engineering Contradiction:
Improvecharge transfer speedVSAvoidvoltage feed-through
Core Design Contradiction:
SpeedVSObject-generated harmful factors

Solution Approach 1:

The charge transfer is moved from a planar capacitive coupling to a vertical charge transfer path through doped regions. The charge transfers vertically through the first and second doped regions to the isolated floating diffusion, separating the charge transfer dimension from the noise coupling dimension. This dimensional change enables fast transfer without increased parasitic capacitance.

Inventive Principle:
Principle #17Another dimension (Dimensionality change)

Solution Approach 2:

The floating diffusion is electrically isolated and effectively copied or replicated in its electrical characteristics through the doped regions, allowing charge transfer without direct capacitive coupling. The doped regions replicate the charge transfer function while eliminating the harmful parasitic capacitance to the transfer gate.

Inventive Principle:
Principle #26Copying

Applied Scientific Principles

This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.

Function Achieved in This Case

This approach enables shorter correlated double sampling times, lower noise levels, and higher conversion gain by minimizing feed-through voltage, effectively reducing readout noise and enhancing imaging performance in low-light conditions.

Implementation Method 1

reducing 1/f noise and random telegraph noise due to capacitive coupling between the floating diffusion and transfer gate

Methodology Applied
Scientific EffectCapacitive coupling: Capacitance

Implementation Method 2

reducing overlap parasitic capacitance and voltage feed-through

Methodology Applied
Scientific EffectParasitic capacitance: Parasitic Capacitance

Data Source

PatentUS12149847B2Image sensor having column-level correlated-double-sampling charge transfer amplifier
Publication Date: 2024.11.19 GIGAJOT TECHNOLOGY INC
  • US12149847B2 patent drawing
  • US12149847B2 patent drawing
  • US12149847B2 patent drawing

AI summary

Correlated double sampling column-level readout of an image sensor pixel (e.g., a CMOS image sensor) may be provided by a charge transfer amplifier that is configured and operated to itself provide for both correlated-double-sampling and amplification of floating diffusion potentials read out from the pixel onto a column bus after reset of the floating diffusion (i) but before transferring photocharge to the floating diffusion (the reset potential) and (ii) after transferring photocharge to the floating diffusion (the transfer potential). A common capacitor of the charge transfer amplifier may sample both the reset potential and the transfer potential such that a change in potential (and corresponding charge change) on the capacitor represents the difference between the transfer potential and reset potential, and the magnitude of this change is amplified by the charge change being transferred between the common capacitor and a second capacitor selectively coupled to the common capacitor.