WO2008060184A1 - Hétérostructure semi-conductrice d'un transistor à effet de champ - Google Patents
Hétérostructure semi-conductrice d'un transistor à effet de champ Download PDFInfo
- Publication number
- WO2008060184A1 WO2008060184A1 PCT/RU2007/000395 RU2007000395W WO2008060184A1 WO 2008060184 A1 WO2008060184 A1 WO 2008060184A1 RU 2007000395 W RU2007000395 W RU 2007000395W WO 2008060184 A1 WO2008060184 A1 WO 2008060184A1
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- Prior art keywords
- layer
- heterostructure
- field
- channel
- template
- Prior art date
Links
- 239000004065 semiconductor Substances 0.000 title claims abstract description 20
- 230000005669 field effect Effects 0.000 title claims abstract description 15
- 239000000758 substrate Substances 0.000 claims abstract description 14
- 230000004888 barrier function Effects 0.000 claims abstract description 11
- 230000007704 transition Effects 0.000 claims abstract description 5
- 239000013078 crystal Substances 0.000 claims description 7
- 229910052594 sapphire Inorganic materials 0.000 description 6
- 239000010980 sapphire Substances 0.000 description 6
- 150000004767 nitrides Chemical class 0.000 description 5
- 229910002704 AlGaN Inorganic materials 0.000 description 3
- 230000008859 change Effects 0.000 description 3
- 230000007547 defect Effects 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 2
- 230000015572 biosynthetic process Effects 0.000 description 2
- 230000015556 catabolic process Effects 0.000 description 2
- 150000001875 compounds Chemical class 0.000 description 2
- 238000005336 cracking Methods 0.000 description 2
- 238000006731 degradation reaction Methods 0.000 description 2
- 230000006911 nucleation Effects 0.000 description 2
- 238000010899 nucleation Methods 0.000 description 2
- 230000035882 stress Effects 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- FYYHWMGAXLPEAU-UHFFFAOYSA-N Magnesium Chemical compound [Mg] FYYHWMGAXLPEAU-UHFFFAOYSA-N 0.000 description 1
- 230000009471 action Effects 0.000 description 1
- 230000003679 aging effect Effects 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- PMHQVHHXPFUNSP-UHFFFAOYSA-M copper(1+);methylsulfanylmethane;bromide Chemical compound Br[Cu].CSC PMHQVHHXPFUNSP-UHFFFAOYSA-M 0.000 description 1
- 230000006866 deterioration Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 229910052749 magnesium Inorganic materials 0.000 description 1
- 239000011777 magnesium Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000004377 microelectronic Methods 0.000 description 1
- 238000001451 molecular beam epitaxy Methods 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 230000005693 optoelectronics Effects 0.000 description 1
- 230000002265 prevention Effects 0.000 description 1
- 230000008569 process Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a 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
- H01L29/68—Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/778—Field effect transistors with two-dimensional charge carrier gas channel, e.g. HEMT ; with two-dimensional charge-carrier layer formed at a heterojunction interface
- H01L29/7782—Field effect transistors with two-dimensional charge carrier gas channel, e.g. HEMT ; with two-dimensional charge-carrier layer formed at a heterojunction interface with confinement of carriers by at least two heterojunctions, e.g. DHHEMT, quantum well HEMT, DHMODFET
- H01L29/7783—Field effect transistors with two-dimensional charge carrier gas channel, e.g. HEMT ; with two-dimensional charge-carrier layer formed at a heterojunction interface with confinement of carriers by at least two heterojunctions, e.g. DHHEMT, quantum well HEMT, DHMODFET using III-V semiconductor material
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a 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
- H01L29/20—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only AIIIBV compounds
- H01L29/201—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only AIIIBV compounds including two or more compounds, e.g. alloys
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a 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
- H01L29/20—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only AIIIBV compounds
- H01L29/201—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only AIIIBV compounds including two or more compounds, e.g. alloys
- H01L29/205—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only AIIIBV compounds including two or more compounds, e.g. alloys in different semiconductor regions, e.g. heterojunctions
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a 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
- H01L29/20—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only AIIIBV compounds
- H01L29/2003—Nitride compounds
Definitions
- the invention relates to heterostructures of semiconductor devices, mainly field-effect transistors.
- microwave field-effect transistors the power of which is several times greater than the power of such transistors, made on the basis of traditional materials
- nitride-based transistors have unique thermal stability and can operate in continuous operation at a temperature of 300-50O 0 C 5 which was completely unavailable on traditional devices.
- An AlN nucleation layer is placed on the sapphire substrate, then a GaN buffer layer and an AlGaN barrier layer.
- This heterostructure requires compensating doping of the buffer layer with magnesium (or carbon, iron, etc.) to reduce current leakage.
- magnesium or carbon, iron, etc.
- cracking of the barrier layer occurs even at relatively low tensile stresses, since the crystal lattice constant of sapphire differs significantly (by 17%) from the crystal lattice constant of GaN.
- the presence of a very thin AlN nucleation layer between the substrate and the GaN layer practically does not affect the aforementioned mismatch.
- heterostructures on a sapphire substrate are known, in particular, a heterostructure of a field effect transistor, RU 2222845 Cl; the heterostructure consistently includes a substrate, an insulating layer made of Al y Ga 1-y N, a channel layer and a barrier layer made of Al z Gai -z N, the channel layer is made of Al x Ga] _ X N, where 0.12>x> 0.03, while on the border of the channel and insulating layers l ⁇ y ⁇ x + 0.1, on the border of the channel and barrier layers l>z> x + 0, l, and the thickness of the channel layer is in the range from 3 to 20 nm, with x, y, z being the molar fractions of Al in the composition of the AlGaN compound.
- This heterostructure is characterized by the disadvantages of
- GaN is about 3%, which eliminates a number of drawbacks of the analogues described above, reduces the density of intrinsic defects, and virtually eliminates cracking of the barrier layer.
- a semiconductor heterostructure of a field-effect transistor including a single-crystal substrate of AlN, an epitaxial template layer of AlN, a channel layer of GaN, and a barrier layer of Al x Ga 1 _ X N, see X.
- Hu atal Trisistors Arsel Letsters, heterofigured filed a on sipgl-crustal bulk AlN "vol. 82, N8, 2003, R.P. 1299-1301, AMERICAP IPSITO OF PHYSICS, USA (a copy of the link is attached).
- the disadvantage of the prototype is the following circumstance.
- the GaN channel layer is grown directly on the AlN template layer in the first stage of this process, at a small channel layer thickness, significant compressive stresses of the channel layer arise.
- the channel layer relaxes with the formation of a large number of defects, which is unacceptable.
- Limiting the thickness of the GaN layer significantly limits the conductivity of the channel layer and, accordingly, limits the operating currents and power of the device. Disclosure of invention
- the objective of the present invention is to increase the conductivity of the channel layer of a semiconductor heterostructure and, therefore, increase the operating currents and power of field-effect transistors.
- this problem is solved due to the fact that in a semiconductor heterostructure of a field-effect transistor including a single crystal AlN substrate, an AlN template layer, a GaN channel layer and an Al x Ga 1 -X N barrier layer, are located one above the other between the template and channel layers, accordingly, the transition layer is Al y Ga ⁇ y N, the buffer layer is Al z Gai -z N, the value of y at the boundary with the template layer is 1, and at the boundary with the buffer layer it is equal to the value z of the buffer layer, with 0.3 ⁇ x ⁇ 0 5, a 0, l ⁇ z ⁇ 0.5;
- the buffer layer at the interface with the channel layer can be doped with Si to a depth of 50–15 ⁇ A.
- the semiconductor heterostructure of the field-effect transistor created in accordance with the claimed features makes it possible to grow a channel layer of a given thickness in accordance with the required operating currents and the installed power of the device; this is due to the fact that high conductivity of the channel layer of GaN is ensured due to the prevention of the formation of reducing mobility electron defects with an increase in its thickness above a critical value.
- the presence of doped Si in the upper sublayer of the buffer layer provides an additional increase in the conductivity of the channel layer by increasing the concentration of electrons in it.
- the single crystal substrate 1 is made of aluminum nitride and has a thickness of 500 ⁇ m, crystallographic orientation (0001). On the substrate 1 is a template layer 2
- AlN thickness in a specific example, 2100 A.
- transition layer 3 Al y Gai -y N with a thickness of 1400 A.
- the value of y varies in thickness of the transition layer from 1 at the border with the template layer to the z value of the buffer layer 4.
- the z value is constantly the entire buffer layer and is 0, l ⁇ z ⁇ 0.5.
- the thickness of the buffer layer 4 in this example is 4200 A, the value of z is 0.3.
- the channel layer 5 GaN has a thickness of 1400 A.
- the buffer layer 4 at the interface with the channel layer is doped with Si to a depth of 100 A with a concentration of l xl ⁇ 19 cm "3 .
- the first embodiment corresponds to claim 1 of the claims
- the buffer layer at the interface with the channel layer is Si doped.
- the characteristics of both variants of the heterostructures are shown in table 1.
- Tests showed a significant improvement in the parameters of heterostructures in comparison with the prototype.
- the resulting heterostructures are the basis of high power field effect transistors.
Landscapes
- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Ceramic Engineering (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Chemical & Material Sciences (AREA)
- Materials Engineering (AREA)
- Junction Field-Effect Transistors (AREA)
Abstract
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE112007002782T DE112007002782T5 (de) | 2006-11-14 | 2007-07-12 | Halbleiterheterostruktur für einen Feldeffekttransistor |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
RU2006140699/28A RU2316076C1 (ru) | 2006-11-14 | 2006-11-14 | Полупроводниковая гетероструктура полевого транзистора |
RU2006140699 | 2006-11-14 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2008060184A1 true WO2008060184A1 (fr) | 2008-05-22 |
Family
ID=39110139
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/RU2007/000395 WO2008060184A1 (fr) | 2006-11-14 | 2007-07-12 | Hétérostructure semi-conductrice d'un transistor à effet de champ |
Country Status (3)
Country | Link |
---|---|
DE (1) | DE112007002782T5 (fr) |
RU (1) | RU2316076C1 (fr) |
WO (1) | WO2008060184A1 (fr) |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU2517788C1 (ru) * | 2012-12-25 | 2014-05-27 | Федеральное Государственное Унитарное Предприятие "Научно-Производственное Предприятие "Пульсар" | Биполярный транзистор свч |
RU2534002C1 (ru) * | 2013-06-18 | 2014-11-27 | федеральное государственное автономное образовательное учреждение высшего профессионального образования "Национальный исследовательский ядерный университет МИФИ" (НИЯУ МИФИ) | Высоковольтный нитрид-галлиевый транзистор с высокой подвижностью электронов |
CN110501773B (zh) * | 2019-08-29 | 2020-06-02 | 南京大学 | 应用于日盲光电探测器的AlN/AlGaN多周期一维光子晶体滤波器及日盲光电探测器 |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
RU2222845C1 (ru) * | 2003-04-01 | 2004-01-27 | Закрытое акционерное общество "Научное и технологическое оборудование" | Полевой транзистор |
US20050133816A1 (en) * | 2003-12-19 | 2005-06-23 | Zhaoyang Fan | III-nitride quantum-well field effect transistors |
US20060049426A1 (en) * | 2004-09-08 | 2006-03-09 | Samsung Electro-Mechanics Co., Ltd. | Nitride based hetero-junction field effect transistor |
US7030428B2 (en) * | 2001-12-03 | 2006-04-18 | Cree, Inc. | Strain balanced nitride heterojunction transistors |
-
2006
- 2006-11-14 RU RU2006140699/28A patent/RU2316076C1/ru active
-
2007
- 2007-07-12 DE DE112007002782T patent/DE112007002782T5/de not_active Ceased
- 2007-07-12 WO PCT/RU2007/000395 patent/WO2008060184A1/fr active Application Filing
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7030428B2 (en) * | 2001-12-03 | 2006-04-18 | Cree, Inc. | Strain balanced nitride heterojunction transistors |
RU2222845C1 (ru) * | 2003-04-01 | 2004-01-27 | Закрытое акционерное общество "Научное и технологическое оборудование" | Полевой транзистор |
US20050133816A1 (en) * | 2003-12-19 | 2005-06-23 | Zhaoyang Fan | III-nitride quantum-well field effect transistors |
US20060049426A1 (en) * | 2004-09-08 | 2006-03-09 | Samsung Electro-Mechanics Co., Ltd. | Nitride based hetero-junction field effect transistor |
Non-Patent Citations (1)
Title |
---|
HU X. ET AL.: "AlGaN/GaN heterostructure field-effect transistors on single-crystal bulk AlN", vol. 82, no. 8, 2003, pages 1299 - 1301, XP012034877, DOI: doi:10.1063/1.1555282 * |
Also Published As
Publication number | Publication date |
---|---|
RU2316076C1 (ru) | 2008-01-27 |
DE112007002782T5 (de) | 2009-09-10 |
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