KR20130049916A - Silicon carbide schottky barrier diode and manufacturing method for the same - Google Patents
Silicon carbide schottky barrier diode and manufacturing method for the same Download PDFInfo
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- KR20130049916A KR20130049916A KR1020110114968A KR20110114968A KR20130049916A KR 20130049916 A KR20130049916 A KR 20130049916A KR 1020110114968 A KR1020110114968 A KR 1020110114968A KR 20110114968 A KR20110114968 A KR 20110114968A KR 20130049916 A KR20130049916 A KR 20130049916A
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- Prior art keywords
- epi
- silicon carbide
- layer
- schottky barrier
- metal
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- 230000004888 barrier function Effects 0.000 title claims abstract description 27
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 title claims abstract description 21
- 229910010271 silicon carbide Inorganic materials 0.000 title claims abstract description 21
- 238000004519 manufacturing process Methods 0.000 title claims abstract description 17
- 239000002184 metal Substances 0.000 claims abstract description 38
- 229910052751 metal Inorganic materials 0.000 claims abstract description 38
- 239000000758 substrate Substances 0.000 claims abstract description 12
- 238000005530 etching Methods 0.000 claims description 9
- 238000000034 method Methods 0.000 claims description 9
- 230000000903 blocking effect Effects 0.000 claims description 6
- 238000000151 deposition Methods 0.000 claims description 4
- 230000035939 shock Effects 0.000 claims description 2
- 230000015556 catabolic process Effects 0.000 abstract description 7
- 230000005684 electric field Effects 0.000 abstract description 2
- 238000005468 ion implantation Methods 0.000 description 11
- 150000002500 ions Chemical class 0.000 description 6
- 238000010438 heat treatment Methods 0.000 description 5
- 230000008569 process Effects 0.000 description 5
- 238000011084 recovery Methods 0.000 description 3
- 230000009467 reduction Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000006872 improvement Effects 0.000 description 2
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 1
- 239000000969 carrier Substances 0.000 description 1
- 230000000779 depleting effect Effects 0.000 description 1
- 239000006185 dispersion Substances 0.000 description 1
- 238000001312 dry etching Methods 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 230000020169 heat generation Effects 0.000 description 1
- 239000001257 hydrogen Substances 0.000 description 1
- 229910052739 hydrogen Inorganic materials 0.000 description 1
- 229920002120 photoresistant polymer Polymers 0.000 description 1
- 238000005036 potential barrier Methods 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/02—Semiconductor bodies ; Multistep manufacturing processes therefor
- H01L29/12—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
- H01L29/16—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only elements of Group IV of the Periodic System
- H01L29/1608—Silicon carbide
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/66007—Multistep manufacturing processes
- H01L29/66053—Multistep manufacturing processes of devices having a semiconductor body comprising crystalline silicon carbide
- H01L29/6606—Multistep manufacturing processes of devices having a semiconductor body comprising crystalline silicon carbide the devices being controllable only by variation of the electric current supplied or the electric potential applied, to one or more of the electrodes carrying the current to be rectified, amplified, oscillated or switched, e.g. two-terminal devices
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/86—Types of semiconductor device ; Multistep manufacturing processes therefor controllable only by variation of the electric current supplied, or only the electric potential applied, to one or more of the electrodes carrying the current to be rectified, amplified, oscillated or switched
- H01L29/861—Diodes
- H01L29/872—Schottky diodes
Abstract
Description
The present invention relates to a silicon carbide schottky barrier diode and a method for manufacturing the same, and more particularly, to a silicon carbide schottky barrier diode and a method for manufacturing the same.
The Schottky diode is a diode made by bonding an N-type semiconductor and a metal, and it is called a Schottky diode made using a Schottky barrier discovered by a German person named Walter H. Schottky.
Schottky diodes have a low forward drop of 0.2V to 0.4V and a 10x faster switching speed than conventional diodes.
The low forward voltage drop means low heat generation and good efficiency in terms of power, and low voltage drop (= distortion) of the input signal when acting as a signal rectifier or switch.
Faster switching speed means shorter recovery time. Recovery time is how fast a signal can be sent in the forward direction when the reverse bias is applied and the forward bias is applied again.
Thus, Schottky diodes can be used to increase efficiency, so they are often used where power supply circuits or fast switches / rectifiers are required for high frequency signal processing.
However, there are disadvantages such as low maximum reverse voltage (maximum voltage that can withstand when reverse bias is applied) and high reverse leakage current.
Meanwhile, most of the silicon carbide schottky barrier diodes (SBDs) currently in mass production have a junction barrier schottky formed with p + in the form of ion implantation at the bottom of the Schottky junction in order to reduce the reverse leakage current. By applying barrier schottky (JBS) structure, leakage current is blocked and breakdown voltage is improved by overlapping of pn diode depletion layer diffused when reverse voltage is applied.
However, in order to achieve such an effect, an expensive ion implanter capable of applying a wafer held at a high temperature to high voltage ions and an apparatus capable of high temperature heat treatment to recover a damaged wafer surface after ion implantation are required. There is a disadvantage in that cost increases when manufacturing SBD.
The present invention has been invented to improve the above disadvantages, Schottky by applying a method of etching a substrate on which a p + epitaxial layer (hereinafter, abbreviated as epi) is grown instead of the conventional ion implantation process. By forming a p + epi (junction barrier Schottky structure) under the region, silicon carbide Schottky barrier diodes and their cost can be saved not only by blocking leakage current but also by eliminating ion implantation process and heat treatment process for wafer surface recovery. The purpose is to provide a manufacturing method.
In order to achieve the above object, the silicon carbide Schottky barrier diode according to the present invention comprises: an n− epilayer stacked in a planar shape on an n + substrate; P + epi protruding at intervals in the horizontal direction on the n- epi layer; A Schottky metal stacked on the p + epi and n- epi layers; a conductive region through which a current flows between p + epi when forward voltage is applied, and a depletion layer formed under the p + epi when reverse voltage is applied. It is characterized by blocking the leakage current.
The p + epi is formed in a straight line, a square shape and a hexagonal shape when viewed from the bottom of the shock key metal, so as to ensure the maximum conduction area.
In addition, the method of manufacturing a silicon carbide Schottky barrier diode according to the present invention comprises the steps of depositing an n + substrate, n-epi layer, p + epi layer in order; Etching the p + epi layer in a predetermined pattern to form p + epi at an interval in the horizontal direction from the n− epi layer; And depositing a schottky metal on the p + epi and n− epi layers.
The advantages of the silicon carbide Schottky barrier diode and its manufacturing method according to the present invention are as follows.
First, p + epi is formed between the Schottky metal and n- epi by etching the substrate on which the p + epi layer is grown, so that when a reverse voltage is applied, a depletion layer is formed under the p + epi to block leakage current, Dispersion can also be improved to improve yield characteristics.
Secondly, since the present invention does not need to use a conventional ion implanter to improve leakage current blocking and breakdown voltage characteristics, it is possible to reduce the cost of an expensive ion implanter and to recover a damaged wafer surface after ion implantation. Since no high temperature heat treatment equipment is required, the cost of SiC SBD can be lowered.
Third, by applying a closed cross-sectional structure of a straight, square, or hexagonal shape to the p + epi region, it is possible to ensure the maximum conduction region between the p + epi to smooth the flow of current when forward voltage is applied.
1 is a cross-sectional view showing the structure of a Schottky barrier diode according to an embodiment of the present invention.
2 is an operating state diagram of the Schottky diode in FIG.
3 is a plan view illustrating a p + epi region and an energization region in FIG. 1;
4 to 6 are cross-sectional views showing a method of manufacturing a schottky barrier diode according to an embodiment of the present invention.
Hereinafter, exemplary embodiments of the present invention will be described in detail with reference to the accompanying drawings so that those skilled in the art may easily implement the present invention.
1 is a cross-sectional view illustrating a structure of a schottky barrier diode according to an embodiment of the present invention, and FIG. 2 is a diagram illustrating an operating state of the schottky diode in FIG. 1.
In the present invention, a silicon carbide Schottky barrier diode (SiC SBD) is formed by applying an etching process instead of a conventional ion implantation process to form a p + formed junction barrier Schottky structure, thereby obtaining the same effect as conventional ion implantation. In addition, the present invention relates to a silicon carbide Schottky barrier diode and a method of manufacturing the same, which can improve existing problems.
The silicon carbide Schottky barrier diode device according to the present invention has a structure stacked from below with an ohmic metal, an n +
The p +
The
Although the leakage characteristics and the degree of improvement of the breakdown voltage are different according to the interval between the p +
When the p +
Referring to FIG. 2, when the forward voltage is applied to the Schottky diode terminal, since there is no
At this time, the
3 is a plan view showing a p +
Here, the present invention provides a predetermined width of the etched and remaining p +
At this time, in the case where the shape of the p +
As such, when optimizing the distance and the number of p +
Hereinafter, a method of manufacturing a schottky barrier diode according to the present invention will be described.
4 is a cross-sectional view showing a wafer prior to fabrication of the device, FIG. 5 is a cross-sectional view showing the etching of the p +
As shown in FIG. 4, in the wafer prior to fabrication of the device, n- and p +
At this time, the doping concentration of n − is 10 15 to 10 16 / cm 3, and the doping concentration of p +
As shown in FIG. 5, the p +
In this case, the mask for etching may use a PR (photoresist) or a metal, etc., to form a pattern using dry etching.
In addition, after etching, the sacrificial oxide layer may be formed to stabilize the surface, and the oxide layer may be etched or annealed in a gas atmosphere such as hydrogen.
As shown in FIG. 6, the
The upper
As shown in FIG. 1,
As the
Therefore, according to the present invention, the p +
In addition, since the present invention does not need to use a conventional ion implanter to improve leakage current blocking and breakdown voltage, the cost of expensive ion implanters is reduced, and a separate surface for recovering the damaged wafer surface after ion implantation is required. No high temperature heat treatment equipment is required, which reduces the cost of SiC SBD.
In addition, by applying a closed cross-sectional structure of a straight, square, or hexagonal shape to the p + epi area, it is possible to secure the maximum conduction area between the p +
10: n + substrate 11: n- epi layer
12: p + epi (layer) 13: Schottky metal
14: ohmic metal 15: pad metal
16: depletion layer
Claims (3)
an n− epi layer 11 stacked in a planar shape on the n + substrate 10;
P + epi (12) protruding at intervals in the horizontal direction on the upper surface of the n- epi layer (11);
A Schottky metal 13 stacked on the p + epi 12 and n- epi layer;
And a conductive region through which a current flows between the p + epi 12 when a forward voltage is applied, and blocking a leakage current by the depletion layer 16 formed under the p + epi 12 when a reverse voltage is applied. Silicon carbide schottky barrier diodes.
The p + epi (12) is a silicon carbide Schottky barrier diode, characterized in that formed in a straight, square and hexagonal shape when viewed under the shock key metal to ensure the maximum conduction area.
depositing an n + substrate 10, an n− epi layer 11, and a p + epi layer 12 in order;
Etching the p + epi layer 12 in a predetermined pattern to form a p + epi 12 at an interval n in the horizontal direction from the n− epi layer 11;
Depositing a Schottky metal (13) on the p + epi (12) and n− epi layers (11);
Method of manufacturing a silicon carbide Schottky barrier diode, comprising a.
Priority Applications (1)
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KR1020110114968A KR20130049916A (en) | 2011-11-07 | 2011-11-07 | Silicon carbide schottky barrier diode and manufacturing method for the same |
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KR1020110114968A KR20130049916A (en) | 2011-11-07 | 2011-11-07 | Silicon carbide schottky barrier diode and manufacturing method for the same |
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Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR101490937B1 (en) * | 2013-09-13 | 2015-02-06 | 현대자동차 주식회사 | Schottky barrier diode and method for manufacturing the same |
US20150179826A1 (en) * | 2013-12-23 | 2015-06-25 | Samsung Electro-Mechanics Co., Ltd. | Diode device and method of manufacturing the same |
CN108538925A (en) * | 2018-06-15 | 2018-09-14 | 深圳基本半导体有限公司 | A kind of silicon carbide junction barrier schottky diodes |
CN110571262A (en) * | 2019-09-09 | 2019-12-13 | 电子科技大学 | Silicon carbide junction barrier Schottky diode with groove structure |
CN111261723A (en) * | 2018-11-30 | 2020-06-09 | 全球能源互联网研究院有限公司 | SiC JBS device |
US10930797B2 (en) | 2016-07-05 | 2021-02-23 | Hyundai Motor Company, Ltd. | Schottky barrier diode and method of manufacturing the same |
KR102320367B1 (en) * | 2020-05-29 | 2021-11-02 | 전북대학교산학협력단 | Method for manufacturing schottky barrier diode with improved breakdown voltage through field plate layer deposition |
-
2011
- 2011-11-07 KR KR1020110114968A patent/KR20130049916A/en not_active Application Discontinuation
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR101490937B1 (en) * | 2013-09-13 | 2015-02-06 | 현대자동차 주식회사 | Schottky barrier diode and method for manufacturing the same |
US20150179826A1 (en) * | 2013-12-23 | 2015-06-25 | Samsung Electro-Mechanics Co., Ltd. | Diode device and method of manufacturing the same |
US10930797B2 (en) | 2016-07-05 | 2021-02-23 | Hyundai Motor Company, Ltd. | Schottky barrier diode and method of manufacturing the same |
CN108538925A (en) * | 2018-06-15 | 2018-09-14 | 深圳基本半导体有限公司 | A kind of silicon carbide junction barrier schottky diodes |
CN111261723A (en) * | 2018-11-30 | 2020-06-09 | 全球能源互联网研究院有限公司 | SiC JBS device |
CN110571262A (en) * | 2019-09-09 | 2019-12-13 | 电子科技大学 | Silicon carbide junction barrier Schottky diode with groove structure |
KR102320367B1 (en) * | 2020-05-29 | 2021-11-02 | 전북대학교산학협력단 | Method for manufacturing schottky barrier diode with improved breakdown voltage through field plate layer deposition |
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