# US 12,224,320 B2 · Silicon carbide semiconductor device and method of manufacturing silicon carbide semiconductor device

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- Number: US 12,224,320 B2
- Document ID: US12224320B2
- Status: Granted
- Kind: B2
- Application number: 17/587,802
- Filed: 2022-01-28
- Published: 2022-09-08
- Granted: 2025-02-11
- Earliest claimed: 2021-03-05
- Assignees: Fuji Electric Co., Ltd.
- Applicants: Fuji Electric Co., Ltd.
- Inventors: Yoshihito Ichikawa
- Web page: https://patentgrep.com/patent/US12224320B2

## CPC

- H10D 62/8325: {Silicon carbide}
- H10D 30/0297: {using recessing of the gate electrodes, e.g. to form trench gate electrodes}
- H10D 30/665: {having edge termination structures}
- H10D 30/668: {having trench gate electrodes, e.g. UMOS transistors}
- H10D 62/107: {Buried supplementary regions, e.g. buried guard rings (multi-RESURF H10D62/111)}
- H10D 62/157: {Impurity concentrations or distributions}
- H10P 34/40: with high-energy radiation
- H10D 62/393: {Body regions of DMOS transistors or IGBTs (cell layout of DMOS H10D62/127)}
- H10D 64/0115: {to silicon carbide}
- H10P 30/2042: {into crystalline silicon carbide}
- H10P 30/218: {characterised by the implantation in a compound semiconductor of both electrically active and inactive species in the same semiconductor region to be doped n-type or p-type}
- H10D: INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10P: GENERIC PROCESSES OR APPARATUS FOR THE MANUFACTURE OR TREATMENT OF DEVICES COVERED BY CLASS H10

## Abstract

At any timing after formation of gate electrodes, particle beam irradiation is performed to a semiconductor wafer having an n−-type drift region constituted by an n−-type epitaxial layer and having an n-type impurity concentration that is higher than a target majority carrier concentration (design value) of the n−-type drift region. Point defects of a defect density corresponding to an irradiation dose of the particle beam are generated in the n−-type drift region by the particle beam irradiation, whereby an effective majority carrier concentration of the n−-type drift region is adjusted and reduced with respect to the n-type impurity concentration of the n−-type drift region, to approach the design value. After formation of the n−-type epitaxial layer, the n-type impurity concentration of the n−-type drift region may be measured, or the n−-type epitaxial layer may be formed to have an n-type impurity concentration higher than the design value.

## Claims

### Claim 1

A silicon carbide semiconductor device, comprising:
a starting substrate containing silicon carbide and having a first surface and a second surface opposite to each other;
a first-conductivity-type epitaxial layer provided on the first surface of the starting substrate;
a second-conductivity-type epitaxial layer provided on the first-conductivity-type epitaxial layer; and
a pn junction through which a main current passes, the pn junction being between the second-conductivity-type epitaxial layer and the first-conductivity-type epitaxial layer, wherein
the first-conductivity-type epitaxial layer contains a plurality of point defects at a defect density corresponding to an irradiation dose of a particle beam, the first-conductivity-type epitaxial layer having an effective majority carrier concentration that is lower than a concentration of a first-conductivity-type impurity of the first-conductivity-type epitaxial layer.

### Claim 2 (depends on 1)

The silicon carbide semiconductor device according to claim 1, wherein
the effective majority carrier concentration of the first-conductivity-type epitaxial layer is at least 70% but less than 100% of the concentration of the first-conductivity-type impurity of the first-conductivity-type epitaxial layer.

### Claim 3 (depends on 1)

The silicon carbide semiconductor device according to claim 1, wherein
the effective majority carrier concentration of the first-conductivity-type epitaxial layer is within 10% lower than the concentration of the first-conductivity-type impurity of the first-conductivity-type epitaxial layer.

### Claim 4 (depends on 1)

The silicon carbide semiconductor device according to claim 1, wherein
the particle beam contains helium, protons or electrons.

### Claim 5 (depends on 1)

The silicon carbide semiconductor device according to claim 1, wherein
an entire area of the first-conductivity-type epitaxial layer and an entire area of the starting substrate contain the point defects.

### Claim 6 (depends on 1)

The silicon carbide semiconductor device according to claim 1, further comprising:
a plurality of first-conductivity-type regions provided in the second-conductivity-type epitaxial layer;
a second-conductivity-type region that is a portion of the second-conductivity-type epitaxial layer free of the first-conductivity-type regions;
a gate insulating film provided in contact with a region of the second-conductivity-type region between one of the first-conductivity-type regions and the first-conductivity-type epitaxial layer;
a gate electrode provided facing the second-conductivity-type region with the gate insulating film intervening therebetween;
a first electrode electrically connected to the first-conductivity-type regions and the second-conductivity-type region; and
a second electrode provided on the second surface of the starting substrate.

### Claim 7 (depends on 1)

A method of manufacturing the silicon carbide semiconductor device according to claim 1, the method comprising:
preparing, as a first process, the starting substrate containing silicon carbide and epitaxially growing the first-conductivity-type epitaxial layer on the first surface of the starting substrate;
epitaxially growing the second-conductivity-type epitaxial layer on the first-conductivity-type epitaxial layer as a second process;
forming, as a third process, a plurality of first-conductivity-type regions in the second-conductivity-type epitaxial layer, a portion of the second-conductivity-type epitaxial layer free of the first-conductivity-type regions constituting a second-conductivity-type region;
forming a gate insulating film in contact with a region of the second-conductivity-type region as a fourth process, the region being between one of the first-conductivity-type regions and the first-conductivity-type epitaxial layer;
forming a gate electrode facing the second-conductivity-type region with the gate insulating film intervening therebetween as a fifth process;
forming a first electrode electrically connected to the first-conductivity-type regions and the second-conductivity-type region as a sixth process;
forming a second electrode on the second surface of the starting substrate as a seventh process;
measuring a concentration of a first-conductivity-type impurity of the first-conductivity-type epitaxial layer as a measurement process, the measurement process being performed after the first process but before the second process; and
when the concentration of the first-conductivity-type impurity of the first-conductivity-type epitaxial layer measured by the measurement process is higher than a design value, irradiating, as an adjustment process, the first-conductivity-type epitaxial layer with a particle beam, and reducing an effective majority carrier concentration of the first-conductivity-type epitaxial layer with respect to the concentration of the first-conductivity-type impurity of the first-conductivity-type epitaxial layer, to approach the design value.

### Claim 8 (depends on 7)

The method according to claim 7, wherein
in the adjustment process, the effective majority carrier concentration of the first-conductivity-type epitaxial layer is set to be at least 70% but less than 100% of the concentration of the first-conductivity-type impurity of the first-conductivity-type epitaxial layer.

### Claim 9 (depends on 7)

The method according to claim 7, wherein
in the adjustment process, the effective majority carrier concentration of the first-conductivity-type epitaxial layer is within 10% lower than the concentration of the first-conductivity-type impurity of the first-conductivity-type epitaxial layer.

### Claim 10 (depends on 7)

The method according to claim 7, wherein
in the adjustment process, the particle beam contains helium, protons or electrons.

### Claim 11 (depends on 7)

The method according to claim 7, wherein
the adjustment process includes performing a heat treatment at a temperature in a range from 350 degrees C. to 400 degrees C. after irradiating the first-conductivity-type epitaxial layer with the particle beam.

### Claim 12 (depends on 11)

The method according to claim 11, wherein
in the adjustment process, the heat treatment is performed for a length of time in a range from 30 minutes to 60 minutes.

### Claim 13 (depends on 11)

The method according to claim 11, wherein
the method is free of another heat treatment of a temperature of at least 400 degrees C. after the heat treatment of the adjustment process.

### Claim 14 (depends on 1)

A method of manufacturing the silicon carbide semiconductor device according to claim 1, the method comprising:
preparing, as a first process, the starting substrate containing silicon carbide and epitaxially growing the first-conductivity-type epitaxial layer on the first surface of the starting substrate, the first-conductivity-type epitaxial layer having a concentration of a first-conductivity-type impurity higher than a design value;
epitaxially growing the second-conductivity-type epitaxial layer on the first-conductivity-type epitaxial layer as a second process;
forming, as a third process, a plurality of first-conductivity-type regions in the second-conductivity-type epitaxial layer, a portion of the second-conductivity-type epitaxial layer free of the first-conductivity-type regions constituting a second-conductivity-type region;
forming a gate insulating film in contact with a region of the second-conductivity-type region as a fourth process, the region being between one of the first-conductivity-type regions and the first-conductivity-type epitaxial layer;
forming a gate electrode facing the second-conductivity-type region with the gate insulating film intervening therebetween as a fifth process;
forming a first electrode electrically connected to the first-conductivity-type regions and the second-conductivity-type region as a sixth process;
forming a second electrode on the second surface of the starting substrate as a seventh process; and
irradiating, as an adjustment process, the first-conductivity-type epitaxial layer with a particle beam, and reducing an effective majority carrier concentration of the first-conductivity-type epitaxial layer with respect to the concentration of the first-conductivity-type impurity of the first-conductivity-type epitaxial layer, to approach the design value.

### Claim 15 (depends on 14)

The method according to claim 14 wherein
in the adjustment process, the effective majority carrier concentration of the first-conductivity-type epitaxial layer is set to be at least 70% but less than 100% of the concentration of the first-conductivity-type impurity of the first-conductivity-type epitaxial layer.

### Claim 16 (depends on 14)

The method according to claim 14, wherein
in the adjustment process, the effective majority carrier concentration of the first-conductivity-type epitaxial layer is within 10% lower than the concentration of the first-conductivity-type impurity of the first-conductivity-type epitaxial layer.

### Claim 17 (depends on 14)

The method according to claim 14, wherein
in the adjustment process, the particle beam contains helium, protons or electrons.

### Claim 18 (depends on 14)

The method according to claim 14, wherein
the adjustment process includes performing a heat treatment at a temperature in a range from 350 degrees C. to 400 degrees C. after irradiating the first-conductivity-type epitaxial layer with the particle beam.

### Claim 19 (depends on 18)

The method according to claim 18, wherein
in the adjustment process, the heat treatment is performed for a length of time in a range from 30 minutes to 60 minutes.

### Claim 20 (depends on 18)

The method according to claim 18, wherein
the method is free of another heat treatment of a temperature of at least 400 degrees C. after the heat treatment of the adjustment process.
