CN113611741A - GaN HMET device with fin-shaped structure - Google Patents

GaN HMET device with fin-shaped structure Download PDF

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Publication number
CN113611741A
CN113611741A CN202110879949.3A CN202110879949A CN113611741A CN 113611741 A CN113611741 A CN 113611741A CN 202110879949 A CN202110879949 A CN 202110879949A CN 113611741 A CN113611741 A CN 113611741A
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gan
conductive material
fin
along
barrier layer
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CN113611741B (en
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罗小蓉
邓思宇
廖德尊
魏杰
贾艳江
张�成
孙涛
郗路凡
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University of Electronic Science and Technology of China
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University of Electronic Science and Technology of China
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor 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
    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types 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
    • H01L29/76Unipolar devices, e.g. field effect transistors
    • H01L29/772Field effect transistors
    • H01L29/778Field effect transistors with two-dimensional charge carrier gas channel, e.g. HEMT ; with two-dimensional charge-carrier layer formed at a heterojunction interface
    • H01L29/7786Field effect transistors with two-dimensional charge carrier gas channel, e.g. HEMT ; with two-dimensional charge-carrier layer formed at a heterojunction interface with direct single heterostructure, i.e. with wide bandgap layer formed on top of active layer, e.g. direct single heterostructure MIS-like HEMT
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor 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
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/402Field plates
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor 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
    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/41Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
    • H01L29/423Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions not carrying the current to be rectified, amplified or switched
    • H01L29/42312Gate electrodes for field effect devices
    • H01L29/42316Gate electrodes for field effect devices for field-effect transistors
    • H01L29/4232Gate electrodes for field effect devices for field-effect transistors with insulated gate
    • H01L29/42372Gate electrodes for field effect devices for field-effect transistors with insulated gate characterised by the conducting layer, e.g. the length, the sectional shape or the lay-out
    • H01L29/4238Gate electrodes for field effect devices for field-effect transistors with insulated gate characterised by the conducting layer, e.g. the length, the sectional shape or the lay-out characterised by the surface lay-out

Abstract

The invention belongs to the technical field of power semiconductors, and relates to a GaN HMET (high electron mobility transistor) device with a multi-fin structure. The invention is mainly characterized in that: when the device is conducted, the electron accumulation layers are arranged on the periphery of the fin-shaped GaN layers which are distributed discontinuously along the vertical direction of the device, and two-dimensional electron gas (2DEG) with high concentration and high mobility exists on the heterogeneous interface of the GaN channel layer and the barrier layer along the transverse direction of the device, so that the conduction current of the device can be improved, and the conduction resistance can be reduced; two-dimensional hole gas (2DHG) is introduced through a heterostructure formed by the fin-shaped GaN layer and the barrier layer, a conducting path between the source electrode and the two-dimensional electron gas in the vertical direction is cut off, and the enhancement type GaN HMET device is realized; compared with the large transverse distance between the gate sources in the traditional GaN HMET, the source electrode is positioned on the top of the fin-shaped GaN, so that the area of the device is reduced; the terminal region positioned on one side of the source gate structure can reduce the peak of the electric field at the edge of the gate and introduce a new peak of the electric field, thus being beneficial to improving the withstand voltage of the device.

Description

GaN HMET device with fin-shaped structure
Technical Field
The invention belongs to the technical field of power semiconductors, and relates to a GaN HMET device with a fin-shaped structure.
Background
Compared with the first-generation semiconductor material Si, the third-generation wide bandgap semiconductor material GaN has more excellent material physical characteristics, and the physical parameters such as the forbidden band width, the electron mobility, the electron saturation rate, the critical breakdown electric field, the thermal conductivity and the high/low frequency Baliga excellent value are far higher than those of the Si material. The GaN HEMT (high electron mobility transistor) device has wide application prospect in the application field of high-current, low-power consumption and high-voltage switching devices.
The conventional GaN HEMT is a depletion mode device because the AlGaN/GaN heterojunction has strong spontaneous polarization and piezoelectric polarization effects, and a heterojunction interface spontaneously forms high-concentration two-dimensional electron gas (2 DEG). However, in practical circuit applications, the depletion mode device needs a negative voltage power supply to turn off the device, which not only increases the risk of false turn-on of the circuit, but also increases the power consumption of the whole circuit and the design difficulty of the driving circuit. Therefore, the enhancement mode GaN HEMT device is more suitable for power electronic circuits. Typical ways to implement enhancements today include: groove gate technology, P-GaN technology, Cascode cascade technology, fluorine ion implantation technology, thin barrier technology and the like.
In addition, although the GaN material has the advantage of high critical breakdown electric field, for the AlGaN/GaN HEMT device, the device breaks down in advance due to the existence of electric field sharp edges at the edge of the gate, excessive leakage current and the like, and the withstand voltage of the device is far from the theoretical limit of the GaN material. For this reason, various technical means are used to improve the breakdown voltage of the device, mainly including: the method comprises the following steps of field plate technology, fluorine ion implantation, terminal technology, polarized super junction technology, compensation doping technology and the like.
Disclosure of Invention
The invention provides a GaN HMET device with a fin-shaped structure based on the application requirement of a HEMT device.
The technical scheme of the invention is as follows:
a GaN HMET device with a fin-shaped structure comprises a substrate layer 1, a GaN buffer layer 2, a GaN channel layer 3, a barrier layer 4 and a passivation layer 5 which are sequentially stacked from bottom to top along the vertical direction of the device; along the transverse direction of the device, one end of the device is a source gate structure which penetrates through the passivation layer 5 along the vertical direction of the device, and the other end of the device is a first conductive material 6 which penetrates through the passivation layer 5 along the vertical direction of the device;
the first conductive material 6 is in contact with the upper surface of the barrier layer 4 along the vertical direction of the device, the contact is ohmic contact, and a drain electrode is led out from the upper surface;
the source gate structure is characterized by comprising a plurality of fin-shaped GaN layers 7 which are discontinuously distributed along the longitudinal direction of the device, a source electrode and an insulated gate structure; the fin-shaped GaN layer 7 is positioned above the barrier layer 4 along the vertical direction of the device and is in contact with the upper surface of the barrier layer 4; the source electrode is made of a second conductive material 8, is in contact with the upper surface of the fin-shaped GaN layer 7, and is in ohmic contact; the insulated gate structure is composed of an insulated gate dielectric 9 and a third conductive material 10, wherein the insulated gate dielectric 9 is positioned above the barrier layer 4 along the vertical direction of the device, is in contact with the upper surface of the barrier layer 4, and covers the side walls of the fin-shaped GaN layer 7 and the second conductive material 8; the side wall and the bottom of the third conductive material 10 are in contact with the upper surface of the insulated gate dielectric 9 and are not in contact with the second conductive material 8; a grid is led out of the upper surface of the third conductive material 10;
further, the barrier layer 4 is made of one or a combination of AlN, AlGaN, InGaN, and InAlN.
According to the GaN HMET device with the multi-fin structure, when the device is conducted, the electron accumulation layers are arranged on the periphery of the fin-shaped GaN layers which are distributed discontinuously along the vertical direction of the device, and two-dimensional electron gas (2DEG) with high concentration and high mobility exists on the heterogeneous interface of the GaN channel layer and the barrier layer along the transverse direction of the device, so that the conduction current of the device can be improved, and the conduction resistance can be reduced; two-dimensional hole gas (2DHG) is introduced through a heterostructure formed by the fin-shaped GaN layer and the barrier layer, a conducting path between the source electrode and the two-dimensional electron gas in the vertical direction is cut off, and the enhancement type GaN HMET device is realized; compared with the large transverse distance between the gate sources in the traditional GaN HMET, the source electrode is positioned on the top of the fin-shaped GaN, so that the area of the device is reduced; the terminal region positioned on one side of the source gate structure can reduce the peak of the electric field at the edge of the gate and introduce a new peak of the electric field, thus being beneficial to improving the withstand voltage of the device.
Drawings
FIG. 1 is a schematic three-dimensional structure of example 1;
FIG. 2 is a cross-sectional view along AA' of the structure of example 1;
FIG. 3 is a schematic three-dimensional structure of example 2;
FIG. 4 is a schematic three-dimensional structure of example 3;
FIG. 5 is a schematic three-dimensional structure of example 4;
Detailed Description
The technical scheme of the invention is described in detail in the following with reference to the accompanying drawings and embodiments:
example 1
As shown in fig. 1, the HEMT device of this example includes a substrate layer 1, a GaN buffer layer 2, a GaN channel layer 3, a barrier layer 4, and a passivation layer 5, which are sequentially stacked from bottom to top in the vertical direction of the device; along the transverse direction of the device, one end of the device is a source gate structure which penetrates through the passivation layer 5 along the vertical direction of the device, and the other end of the device is a first conductive material 6 which penetrates through the passivation layer 5 along the vertical direction of the device;
the first conductive material 6 is in contact with the upper surface of the barrier layer 4 along the vertical direction of the device, the contact is ohmic contact, and a drain electrode is led out from the upper surface;
the source gate structure is characterized by comprising a plurality of fin-shaped GaN layers 7 which are discontinuously distributed along the longitudinal direction of the device, a source electrode and an insulated gate structure; the fin-shaped GaN layer 7 is positioned above the barrier layer 4 along the vertical direction of the device and is in contact with the upper surface of the barrier layer 4; the source electrode is made of a second conductive material 8, is in contact with the upper surface of the fin-shaped GaN layer 7, and is in ohmic contact; the insulated gate structure is composed of an insulated gate dielectric 9 and a third conductive material 10, wherein the insulated gate dielectric 9 is positioned above the barrier layer 4 along the vertical direction of the device, is in contact with the upper surface of the barrier layer 4, and covers the side walls of the fin-shaped GaN layer 7 and the second conductive material 8; the side wall and the bottom of the third conductive material 10 are in contact with the upper surface of the insulated gate dielectric 9 and are not in contact with the second conductive material 8; a grid is led out of the upper surface of the third conductive material 10;
compared with the traditional GaN HMET device, the GaN HMET device has the advantages of large conduction current, high breakdown voltage, smaller device area under the same voltage withstanding level and the like.
Example 2
The difference between this example and embodiment 1 is that, in this example, the third conductive material 10 extends toward one side of the first conductive material 6 along the lateral direction of the device and covers the passivation layer 5 to form a gate field plate 11, and the gate field plate 11 has a gap from the first conductive material 6; compared with embodiment 1, the advantage of this example is that the gate field plate 11 further optimizes the electric field distribution of the device in the withstand voltage, and improves the breakdown voltage of the device.
Example 3
The difference between this example and example 1 is that in this example, a fluorine ion implantation terminal 12 is embedded in the passivation layer 5, and the fluorine ion implantation terminal 12 is not in contact with the barrier layer 4 in the device vertical direction; in the device lateral direction, with a spacing from the first conductive material 6; compared with embodiment 2, the advantage of this example is that the fluorine ion implantation terminal 12 can improve the device withstand voltage, and does not introduce additional parasitic capacitance, which leads to the degradation of the dynamic performance of the device.
Example 4
The difference between this example and embodiment 1 is that, in this example, along the lateral direction of the device, the barrier layer 4 located between the source-gate structure and the first conductive material 6 has a groove, and does not contact with the lower surface of the barrier layer 4, and the passivation layer 5 covering the barrier layer 4 also has a groove to form a groove terminal, and the groove terminal has a distance from the first conductive material 6 and the source-gate structure along the lateral direction of the device; compared with embodiment 3, the advantage of this example is that the groove terminal 13 is simple in implementation process, low in cost and free of any high temperature process.

Claims (5)

1. A GaN HMET device with a fin-shaped structure comprises a substrate layer (1), a GaN buffer layer (2), a GaN channel layer (3), a barrier layer (4) and a passivation layer (5) which are sequentially stacked from bottom to top along the vertical direction of the device; along the transverse direction of the device, one end of the device is a source gate structure which penetrates through the passivation layer (5) along the vertical direction of the device, and the other end of the device is a first conductive material (6) which penetrates through the passivation layer (5) along the vertical direction of the device;
the first conductive material (6) is in contact with the upper surface of the barrier layer (4) along the vertical direction of the device, the contact is ohmic contact, and a drain electrode is led out from the upper surface;
the source gate structure is characterized by comprising a plurality of fin-shaped GaN layers (7) which are discontinuously distributed along the longitudinal direction of the device, a source electrode and an insulated gate structure; the fin-shaped GaN layer (7) is positioned above the barrier layer (4) along the vertical direction of the device and is in contact with the upper surface of the barrier layer (4); the source electrode is made of a second conductive material (8), is in contact with the upper surface of the fin-shaped GaN layer (7), and is in ohmic contact; the insulated gate structure is composed of an insulated gate dielectric (9) and a third conductive material (10), wherein the insulated gate dielectric (9) is positioned above the barrier layer (4) along the vertical direction of the device, is in contact with the upper surface of the barrier layer (4), and covers the side walls of the fin-shaped GaN layer (7) and the second conductive material (8); the side wall and the bottom of the third conductive material (10) are in contact with the upper surface of the insulated gate dielectric (9) and are not in contact with the second conductive material (8); a grid is led out of the upper surface of the third conductive material (10);
the device longitudinal direction is a third dimension direction which is simultaneously vertical to both the device transverse direction and the device vertical direction.
2. The GaN HMET device with a fin structure as claimed in claim 1, wherein the third conductive material (10) extends along the lateral direction of the device to one side of the first conductive material (6) and covers the passivation layer (5) to form a gate field plate (11), and the gate field plate (11) is spaced apart from the first conductive material (6).
3. The GaN HMET device with fin structure as claimed in claim 1, wherein the passivation layer (5) is embedded with fluorine ion implantation terminal (12), and the fluorine ion implantation terminal (12) is not in contact with the barrier layer (4) along the vertical direction of the device; in the device lateral direction, a spacing is provided with the first conductive material (6).
4. A GaN HMET device with fin structure according to claim 1, wherein the barrier layer (4) between the source gate structure and the first conductive material (6) is recessed along the lateral direction of the device and does not contact the lower surface of the barrier layer (4), and the passivation layer (5) covering the barrier layer (4) is also recessed to form a recess termination, the recess termination being spaced from the first conductive material (6) and the source gate structure along the lateral direction of the device.
5. The GaN HMET device with a fin structure according to any of claims 1-4, wherein the barrier layer (4) is made of one or more of AlN, AlGaN, InGaN and InAlN.
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Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006253559A (en) * 2005-03-14 2006-09-21 Nichia Chem Ind Ltd Field-effect transistor and its manufacturing method
CN102403347A (en) * 2010-09-14 2012-04-04 三星Led株式会社 Gallium nitride based semiconductor devices and methods of manufacturing the same
US20130099283A1 (en) * 2011-10-21 2013-04-25 Taiwan Semiconductor Manufacturing Company, Ltd. III-V Multi-Channel FinFETs
CN103681836A (en) * 2012-09-21 2014-03-26 罗伯特·博世有限公司 Vertical microelectronic component and corresponding production method
CN105810728A (en) * 2016-05-06 2016-07-27 西安电子科技大学 Enhanced fin-type insulated gate high-electronic mobility transistor
CN106611781A (en) * 2015-10-27 2017-05-03 上海新昇半导体科技有限公司 Quantum well device and forming method therefor
WO2019139624A1 (en) * 2018-01-12 2019-07-18 Intel Corporation Vertical field effect transistors having extended drain regions and methods of manufacturing the same

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006253559A (en) * 2005-03-14 2006-09-21 Nichia Chem Ind Ltd Field-effect transistor and its manufacturing method
CN102403347A (en) * 2010-09-14 2012-04-04 三星Led株式会社 Gallium nitride based semiconductor devices and methods of manufacturing the same
US20130099283A1 (en) * 2011-10-21 2013-04-25 Taiwan Semiconductor Manufacturing Company, Ltd. III-V Multi-Channel FinFETs
CN103681836A (en) * 2012-09-21 2014-03-26 罗伯特·博世有限公司 Vertical microelectronic component and corresponding production method
CN106611781A (en) * 2015-10-27 2017-05-03 上海新昇半导体科技有限公司 Quantum well device and forming method therefor
CN105810728A (en) * 2016-05-06 2016-07-27 西安电子科技大学 Enhanced fin-type insulated gate high-electronic mobility transistor
WO2019139624A1 (en) * 2018-01-12 2019-07-18 Intel Corporation Vertical field effect transistors having extended drain regions and methods of manufacturing the same

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