SiC UV Photodetector Structure for Low Dark Current Breakdown Control
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Solution Overview
Problem
Silicon carbide ultraviolet light photodetectors face challenges with high dark current and soft breakdown due to surface implantation processes and leakage currents, affecting their performance in single photon detection conditions.
Innovation Solution
A silicon carbide ultraviolet light photodetector with a non-planar structure featuring a buried region and edge region with insulating material, which enhances electrical field confinement and breakdown voltage, reducing dark current and optimizing detection efficiency.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Productivity
If surface implantation processes are used to create the active area and edge ring, then the detection efficiency is improved, but the dark current increases due to leakage current from the device periphery
Solution Approach 1:
The patent applies curvature by forming a sloped lateral surface on the semiconductor body and creating a recessed peripheral area that follows this curvature. This curved geometry naturally confines the electrical field within the active area and prevents field extension toward the periphery, thereby reducing leakage current and dark current while maintaining detection efficiency through proper active area configuration.
Solution Approach 2:
The patent transitions from a planar two-dimensional structure to a three-dimensional structure by creating a recessed peripheral area and sloped lateral surface. This dimensional change allows the active area to be confined within a specific depth range, enabling better electrical field confinement and reduced peripheral leakage while maintaining high detection efficiency through optimized vertical and lateral geometry.
2Productivity
If the electrical field is extended laterally to increase the active area, then the detection efficiency is improved, but the breakdown voltage decreases due to soft breakdown from peripheral leakage current
Solution Approach 1:
The sloped lateral surface and recessed peripheral area create a curved geometry that confines the electrical field vertically within the active area while preventing lateral field extension. This allows the active area to be sufficiently large for high detection efficiency without causing peripheral leakage that would reduce breakdown voltage and cause soft breakdown.
Solution Approach 2:
The patent applies different geometric properties to different regions: the active area maintains a planar top surface for optimal light detection, while the peripheral area is recessed with a sloped lateral surface for field confinement. This local differentiation allows the active area to be large for high efficiency while the periphery geometry prevents leakage current that would reduce breakdown voltage.
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
The solution results in a photodetector with low dark current, high fill factor, and controlled breakdown voltage, enabling reliable operation in high-density arrays and improved detection of ultraviolet light with reduced noise.
Implementation Method 1
silicon carbide ultraviolet light photodetector... enabling detection of ultraviolet (UV) light with a high sensitivity
Implementation Method 2
avalanche photodiode (SPAD) or Geiger mode-avalanche photodiode (GM-APD) operating condition... considered a gain (of the order of 102 to 105) measured in the avalanche multiplication condition
Data Source
AI summary
The photodetector is formed in a silicon carbide body formed by a first epitaxial layer of an N type and a second epitaxial layer of a P type. The first and second epitaxial layers are arranged on each other and form a body surface including a projecting portion, a sloped lateral portion, and an edge portion. An insulating edge region extends over the sloped lateral portion and the edge portion. An anode region is formed by the second epitaxial layer and is delimited by the projecting portion and by the sloped lateral portion. The first epitaxial layer forms a cathode region underneath the anode region. A buried region of an N type, with a higher doping level than the first epitaxial layer, extends between the anode and cathode regions, underneath the projecting portion, at a distance from the sloped lateral portion as well as from the edge region.


