Silicon-carbide power device of heterojunction terminal and preparation method of silicon-carbide power device

A power device and heterojunction technology, which is applied in semiconductor/solid-state device manufacturing, semiconductor devices, electrical components, etc., can solve the problems of N-type SiC surface doping characteristics change, affecting low device turn-on voltage, and restricting industrialization development. , to avoid the influence of doping characteristics, high breakdown voltage, and reduce the requirements of high temperature and complex processes

Inactive Publication Date: 2016-11-30
XIAMEN SANAN INTEGRATED CIRCUIT
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  • Abstract
  • Description
  • Claims
  • Application Information

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Problems solved by technology

Among them, epitaxial growth is to directly grow P-type SiC on the entire surface of N-type SiC layer. Since the growth temperature of P-type SiC is often high (>1500°C), some P-type impurities (such as Al) will inevitably diffuse during the growth process. In weak N-type SiC, self-doping is formed on the surface of N-type SiC, and even the area is converted into P-type, which leads to chan

Method used

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  • Silicon-carbide power device of heterojunction terminal and preparation method of silicon-carbide power device
  • Silicon-carbide power device of heterojunction terminal and preparation method of silicon-carbide power device
  • Silicon-carbide power device of heterojunction terminal and preparation method of silicon-carbide power device

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Embodiment 1

[0030] refer to figure 1 , the silicon carbide power device of this embodiment is a silicon carbide Schottky barrier diode (SBD) 100, which includes a cathode electrode 110, a substrate layer 120, an N-type SiC epitaxial layer 130, and an anode electrode 140 from bottom to top, wherein the anode electrode 140 A metal-semiconductor Schottky contact is formed with the N-type SiC epitaxial layer 130 . On the N-type SiC epitaxial layer 130 , there are several P-type structures 150 at intervals on the periphery of the anode electrode 140 to form junction terminals. In areas other than the anode electrode 140 , the exposed N-type SiC epitaxial layer 130 and the P-type structure 150 are covered with a dielectric layer 160 .

[0031] The P-type structure 150 is directly formed on the N-type SiC epitaxial layer 130 by heteroepitaxial growth of a P-type semiconductor material whose growth temperature is lower than that of SiC. Specifically, the growth temperature of the P-type semicon...

Embodiment 2

[0038] refer to figure 2 , the silicon carbide power device of this embodiment is a silicon carbide junction barrier Schottky diode 200, which differs from Embodiment 1 in that the P-type structure is distributed on the N-type SiC epitaxial layer 230 except for the P type structure 251 to form a heterojunction terminal, it also includes several discrete P-type structures 252 arranged between the anode electrode 240 and the N-type SiC epitaxial layer 230 to form a junction barrier. Specifically, the P-type structures 252 can be several parallel The strip structure forms several discretely arranged PN junctions with the N-type SiC epitaxial layer 230, and the exposed N-type SiC epitaxial layer 230 between adjacent P-type structures 252 is in contact with the anode electrode 240 to form a Schottky junction. In the reverse blocking state, the pinch-off effect of the depletion region of the adjacent PN junction is used to obtain blocking characteristics similar to that of the PN d...

Embodiment 3

[0042] refer to image 3 The silicon carbide power device of this embodiment is a silicon carbide PN junction diode 300. The difference between it and Embodiment 2 is that the P-type structure is distributed on the N-type SiC epitaxial layer 330 except for the P-type structure 351 on the periphery of the anode electrode 340. In addition to forming the heterojunction terminal, it also includes a layered P-type structure 352 disposed between the anode electrode 340 and the N-type SiC epitaxial layer 330 and isolating the anode electrode 340 and the N-type SiC epitaxial layer 330 . A PN junction is formed between the P-type structure 352 and the N-type SiC epitaxial layer 330 . For the remaining structures, such as the cathode electrode 310 , the substrate layer 320 and the dielectric layer 360 , refer to Embodiment 1, and refer to Embodiment 2 for the manufacturing method, so no further description is given.

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Abstract

The invention discloses a silicon-carbide power device of a heterojunction terminal. The silicon-carbide power device comprises a cathode electrode, a substrate layer, an N-type SiC epitaxial layer and an anode electrode, and further comprises a plurality of separate and independent P-type structures, wherein the P-type structures are formed by P-type semiconductor materials, the growth temperature of which is lower than that of the SiC, formed on the N-type SiC epitaxial layer through heteroepitaxial growth, and the P-type structures are at least distributed on the periphery of the anode electrode so as to form the heterojunction terminal. Therefore, influence to doping characteristics of the N-type SiC epitaxial layer is effectively avoided, and a silicon-carbide device with high breakdown voltage and low device threshold voltage can be obtained. The invention further discloses a manufacturing method of the silicon-carbide power device of the heterojunction terminal, requirements of the high temperature complex technique are largely reduced, the manufacturing procedure is simple, and the manufacturing costs are reduced.

Description

technical field [0001] The invention relates to a semiconductor device, in particular to a heterojunction-terminated silicon carbide power device and a preparation method thereof. Background technique [0002] Power devices based on wide-bandgap semiconductor materials (such as silicon carbide (SiC), gallium nitride (GaN)) can provide greater breakdown voltage and power density, and are expected to be widely used in next-generation power conversion. In SiC power devices, due to the discontinuity of the junction, the electric force lines tend to concentrate at the edge of the junction, resulting in the existence of a high electric field at the junction edge. The presence of a high field will lead to premature breakdown at the junction edge, which greatly limits the reverse breakdown voltage of the device. Therefore, in the design and manufacture of SiC power devices, various junction termination technologies are often used to alleviate the edge electric field concentration e...

Claims

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Application Information

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IPC IPC(8): H01L21/04H01L29/872H01L21/329
CPCH01L21/04H01L21/0405H01L21/0435H01L29/66212H01L29/872H01L29/0619H01L29/8611H01L29/267H01L29/6606H01L29/1608H01L29/2003H01L21/0495H01L21/02378H01L21/0254H01L21/0262
Inventor 刘成叶念慈黄侯魁
Owner XIAMEN SANAN INTEGRATED CIRCUIT
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