JP6534791B2 - 半導体装置 - Google Patents
半導体装置 Download PDFInfo
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- JP6534791B2 JP6534791B2 JP2013259064A JP2013259064A JP6534791B2 JP 6534791 B2 JP6534791 B2 JP 6534791B2 JP 2013259064 A JP2013259064 A JP 2013259064A JP 2013259064 A JP2013259064 A JP 2013259064A JP 6534791 B2 JP6534791 B2 JP 6534791B2
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- H10D30/47—FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels having 2D charge carrier gas channels, e.g. nanoribbon FETs or high electron mobility transistors [HEMT]
- H10D30/471—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT]
- H10D30/475—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having wider bandgap layer formed on top of lower bandgap active layer, e.g. undoped barrier HEMTs such as i-AlGaN/GaN HEMTs
- H10D30/4755—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having wider bandgap layer formed on top of lower bandgap active layer, e.g. undoped barrier HEMTs such as i-AlGaN/GaN HEMTs having wide bandgap charge-carrier supplying layers, e.g. modulation doped HEMTs such as n-AlGaAs/GaAs HEMTs
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- H10D30/471—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT]
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- H10D30/471—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT]
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- H10D62/815—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials of structures exhibiting quantum-confinement effects, e.g. single quantum wells; of structures having periodic or quasi-periodic potential variation of structures having periodic or quasi-periodic potential variation, e.g. superlattices or multiple quantum wells [MQW]
- H10D62/8161—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials of structures exhibiting quantum-confinement effects, e.g. single quantum wells; of structures having periodic or quasi-periodic potential variation of structures having periodic or quasi-periodic potential variation, e.g. superlattices or multiple quantum wells [MQW] potential variation due to variations in composition or crystallinity, e.g. heterojunction superlattices
- H10D62/8162—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials of structures exhibiting quantum-confinement effects, e.g. single quantum wells; of structures having periodic or quasi-periodic potential variation of structures having periodic or quasi-periodic potential variation, e.g. superlattices or multiple quantum wells [MQW] potential variation due to variations in composition or crystallinity, e.g. heterojunction superlattices having quantum effects only in the vertical direction, i.e. layered structures having quantum effects solely resulting from vertical potential variation
- H10D62/8164—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials of structures exhibiting quantum-confinement effects, e.g. single quantum wells; of structures having periodic or quasi-periodic potential variation of structures having periodic or quasi-periodic potential variation, e.g. superlattices or multiple quantum wells [MQW] potential variation due to variations in composition or crystallinity, e.g. heterojunction superlattices having quantum effects only in the vertical direction, i.e. layered structures having quantum effects solely resulting from vertical potential variation comprising only semiconductor materials
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- H10D64/23—Electrodes carrying the current to be rectified, amplified, oscillated or switched, e.g. sources, drains, anodes or cathodes
- H10D64/251—Source or drain electrodes for field-effect devices
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- H10D64/311—Gate electrodes for field-effect devices
- H10D64/411—Gate electrodes for field-effect devices for FETs
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Description
以下、図面を参照しながら本実施の形態の半導体装置について詳細に説明する。
図1は、本実施の形態の半導体装置の構成を模式的に示す断面図である。図1等に示す本実施の形態の半導体装置(半導体素子)は、窒化物半導体を用いたMIS(Metal Insulator Semiconductor)型の電界効果トランジスタ(FET;Field Effect Transistor)である。この半導体装置は、高電子移動度トランジスタ(HEMT:High Electron Mobility Transistor)型のパワートランジスタとして用いることができる。本実施の形態の半導体装置は、いわゆるリセスゲート型の半導体装置である。
次いで、図5〜図22を参照しながら、本実施の形態の半導体装置の製造方法を説明するとともに、当該半導体装置の構成をより明確にする。図5〜図22は、本実施の形態の半導体装置の製造工程を示す断面図または平面図である。
実施の形態1においては、素子分離領域ISOに接続部VIAを設けたが、活性領域ACに接続部VIAを設けてもよい。例えば、本実施の形態においては、ソース電極SEの下に接続部VIAを設ける。
図26は、本実施の形態の半導体装置の構成を模式的に示す断面図である。本実施の形態の半導体装置(半導体素子)は、窒化物半導体を用いたMIS型の電界効果トランジスタである。この半導体装置は、高電子移動度トランジスタ(HEMT)型のパワートランジスタとして用いることができる。本実施の形態の半導体装置は、いわゆるリセスゲート型の半導体装置である。
次いで、図29〜図34を参照しながら、本実施の形態の半導体装置の製造方法を説明するとともに、当該半導体装置の構成をより明確にする。図29〜図34は、本実施の形態の半導体装置の製造工程を示す断面図または平面図である。
実施の形態1および2においては、リセスゲート型の半導体装置を例示したが、他の構成の半導体装置としてもよい。例えば、本実施の形態のように、ゲート電極の下にゲート接合層を配置した接合型の半導体装置を用いてもよい。
図35は、本実施の形態の半導体装置の構成を模式的に示す断面図である。本実施の形態の半導体装置(半導体素子)は、窒化物半導体を用いたトランジスタである。この半導体装置は、高電子移動度トランジスタ(HEMT)型のパワートランジスタとして用いることができる。
次いで、図36〜図40を参照しながら、本実施の形態の半導体装置の製造方法を説明するとともに、当該半導体装置の構成をより明確にする。
実施の形態3においては、素子分離領域ISOに接続部VIAを設けたが、活性領域ACに接続部VIAを設けてもよい。例えば、本実施の形態においては、ソース電極SEの下に接続部VIAを設ける。
図41は、本実施の形態の半導体装置の構成を模式的に示す断面図である。本実施の形態の半導体装置(半導体素子)は、窒化物半導体を用いたトランジスタである。この半導体装置は、高電子移動度トランジスタ(HEMT)型のパワートランジスタとして用いることができる。
次いで、図42を参照しながら、本実施の形態の半導体装置の製造方法を説明するとともに、当該半導体装置の構成をより明確にする。
BA 障壁層
BU バッファ層
C1D コンタクトホール
C1S コンタクトホール
CH チャネル層
CP キャップ層
DE ドレイン電極
DP ドレインパッド
GE ゲート電極
GI ゲート絶縁膜
GL ゲート線
GLT 溝
IF1 絶縁膜
IL1 層間絶縁膜
ISO 素子分離領域
JL ゲート接合層
NUC 核生成層
PR1 フォトレジスト膜
PR2 フォトレジスト膜
PRO 保護膜
S 基板
SE ソース電極
SP ソースパッド
T 溝
TH 貫通孔
UC チャネル下地層
VC 電位固定層
VIA 接続部
Claims (2)
- 基板の上方に形成された第1窒化物半導体層と、
前記第1窒化物半導体層上に形成された第2窒化物半導体層と、
前記第2窒化物半導体層上に形成された第3窒化物半導体層と、
前記第3窒化物半導体層上に形成された第4窒化物半導体層と、
前記第4窒化物半導体層を貫通し、前記第3窒化物半導体層の途中まで到達する溝と、
前記溝内にゲート絶縁膜を介して配置されたゲート電極と、
前記ゲート電極の両側の前記第4窒化物半導体層の上方にそれぞれ形成された第1電極および第2電極と、
前記第1電極と第1窒化物半導体層との間を接続する接続部と、
を有し、
前記第3窒化物半導体層の電子親和力は、前記第2窒化物半導体層の電子親和力より大きく、
前記第4窒化物半導体層の電子親和力は、前記第2窒化物半導体層の電子親和力より小さく、
前記第1窒化物半導体層は、p型の不純物を含有し、活性化した前記p型の不純物濃度は、5×1016cm−3以上で、かつ、1×1017cm−3未満である、半導体装置。 - 請求項1記載の半導体装置において、
前記p型の不純物濃度は、0.5×10 17 cm −3 以下である、半導体装置。
Priority Applications (7)
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JP2013259064A JP6534791B2 (ja) | 2013-12-16 | 2013-12-16 | 半導体装置 |
KR1020140163391A KR20150070001A (ko) | 2013-12-16 | 2014-11-21 | 반도체 장치 |
TW103140804A TW201528503A (zh) | 2013-12-16 | 2014-11-25 | 半導體裝置 |
EP14197151.5A EP2884539A1 (en) | 2013-12-16 | 2014-12-10 | Semiconductor device |
US14/569,492 US9601609B2 (en) | 2013-12-16 | 2014-12-12 | Semiconductor device |
CN201410784150.6A CN104716176B (zh) | 2013-12-16 | 2014-12-16 | 半导体器件 |
US15/437,559 US10014403B2 (en) | 2013-12-16 | 2017-02-21 | Semiconductor device |
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JP2013259064A JP6534791B2 (ja) | 2013-12-16 | 2013-12-16 | 半導体装置 |
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EP (1) | EP2884539A1 (ja) |
JP (1) | JP6534791B2 (ja) |
KR (1) | KR20150070001A (ja) |
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JP6534791B2 (ja) * | 2013-12-16 | 2019-06-26 | ルネサスエレクトロニクス株式会社 | 半導体装置 |
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JP6442800B2 (ja) * | 2014-12-25 | 2018-12-26 | 住友電工デバイス・イノベーション株式会社 | 半導体装置及び半導体装置を製造する方法 |
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JP6527423B2 (ja) * | 2015-08-11 | 2019-06-05 | ルネサスエレクトロニクス株式会社 | 半導体装置およびその製造方法 |
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CN111048576B (zh) * | 2018-10-15 | 2024-02-02 | 苏州捷芯威半导体有限公司 | 一种半导体器件及其制备方法 |
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JP7258735B2 (ja) * | 2019-12-13 | 2023-04-17 | 株式会社東芝 | 半導体装置 |
TWI767425B (zh) * | 2020-11-27 | 2022-06-11 | 合晶科技股份有限公司 | 氮化物磊晶片及其製造方法 |
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JP6251071B2 (ja) * | 2014-02-05 | 2017-12-20 | ルネサスエレクトロニクス株式会社 | 半導体装置 |
JP6341679B2 (ja) * | 2014-02-06 | 2018-06-13 | ルネサスエレクトロニクス株式会社 | 半導体装置 |
-
2013
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2014
- 2014-11-21 KR KR1020140163391A patent/KR20150070001A/ko not_active Application Discontinuation
- 2014-11-25 TW TW103140804A patent/TW201528503A/zh unknown
- 2014-12-10 EP EP14197151.5A patent/EP2884539A1/en not_active Ceased
- 2014-12-12 US US14/569,492 patent/US9601609B2/en not_active Expired - Fee Related
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US20170162683A1 (en) | 2017-06-08 |
EP2884539A1 (en) | 2015-06-17 |
US10014403B2 (en) | 2018-07-03 |
CN104716176A (zh) | 2015-06-17 |
CN104716176B (zh) | 2019-06-14 |
TW201528503A (zh) | 2015-07-16 |
JP2015115582A (ja) | 2015-06-22 |
KR20150070001A (ko) | 2015-06-24 |
US20150171204A1 (en) | 2015-06-18 |
US9601609B2 (en) | 2017-03-21 |
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