CA2085524A1 - Field effect transistor and method for manufacturing the same - Google Patents
Field effect transistor and method for manufacturing the sameInfo
- Publication number
- CA2085524A1 CA2085524A1 CA002085524A CA2085524A CA2085524A1 CA 2085524 A1 CA2085524 A1 CA 2085524A1 CA 002085524 A CA002085524 A CA 002085524A CA 2085524 A CA2085524 A CA 2085524A CA 2085524 A1 CA2085524 A1 CA 2085524A1
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- Prior art keywords
- impurity region
- highly doped
- doped impurity
- drain
- active layer
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Abandoned
Links
- 238000000034 method Methods 0.000 title claims description 27
- 238000004519 manufacturing process Methods 0.000 title claims description 9
- 230000005669 field effect Effects 0.000 title claims 12
- 239000012535 impurity Substances 0.000 claims abstract description 41
- 239000010410 layer Substances 0.000 claims abstract description 39
- 238000009413 insulation Methods 0.000 claims abstract description 28
- 239000000758 substrate Substances 0.000 claims abstract description 24
- 239000004065 semiconductor Substances 0.000 claims abstract description 23
- 239000002344 surface layer Substances 0.000 claims abstract description 9
- 238000005468 ion implantation Methods 0.000 claims description 7
- 238000005530 etching Methods 0.000 claims description 5
- 238000001020 plasma etching Methods 0.000 claims description 4
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 3
- 238000000151 deposition Methods 0.000 claims description 3
- 238000000137 annealing Methods 0.000 claims description 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 claims 2
- 150000001875 compounds Chemical class 0.000 claims 2
- 229910052760 oxygen Inorganic materials 0.000 claims 2
- 239000001301 oxygen Substances 0.000 claims 2
- 229920002120 photoresistant polymer Polymers 0.000 claims 2
- 238000000992 sputter etching Methods 0.000 claims 1
- 230000015556 catabolic process Effects 0.000 abstract description 14
- 239000000463 material Substances 0.000 description 5
- 239000002184 metal Substances 0.000 description 5
- 241000905957 Channa melasoma Species 0.000 description 4
- 229910052581 Si3N4 Inorganic materials 0.000 description 4
- HQVNEWCFYHHQES-UHFFFAOYSA-N silicon nitride Chemical compound N12[Si]34N5[Si]62N3[Si]51N64 HQVNEWCFYHHQES-UHFFFAOYSA-N 0.000 description 4
- 150000002500 ions Chemical class 0.000 description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 238000000206 photolithography Methods 0.000 description 2
- RBFQJDQYXXHULB-UHFFFAOYSA-N arsane Chemical compound [AsH3] RBFQJDQYXXHULB-UHFFFAOYSA-N 0.000 description 1
- 229910000070 arsenic hydride Inorganic materials 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 238000005229 chemical vapour deposition Methods 0.000 description 1
- 229910052681 coesite Inorganic materials 0.000 description 1
- 239000012141 concentrate Substances 0.000 description 1
- 229910052906 cristobalite Inorganic materials 0.000 description 1
- 238000000227 grinding Methods 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
- 235000012239 silicon dioxide Nutrition 0.000 description 1
- 229910052682 stishovite Inorganic materials 0.000 description 1
- 229910052905 tridymite Inorganic materials 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
- H01L29/40—Electrodes ; Multistep manufacturing processes therefor
- H01L29/41—Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
- H01L29/423—Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions not carrying the current to be rectified, amplified or switched
- H01L29/42312—Gate electrodes for field effect devices
- H01L29/42316—Gate electrodes for field effect devices for field-effect transistors
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- 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)
- Junction Field-Effect Transistors (AREA)
- Electrodes Of Semiconductors (AREA)
Abstract
ABSTRACT OF THE DISCLOSURE
There is disclosed an FET having a high drain breakdown voltage and a short gate length comprising an active layer 2 formed on a surface layer of a semiconductor substrate 1; a source highly doped impurity region 4 and a drain highly doped impurity region 4 formed in the surface layer of the semiconductor substrate 1 to sandwich the active layer 2; an insulation film 5 formed on the source highly doped impurity region 4; a gate electrode 8 formed on the active layer 2 and the insulation film 5 while maintaining a constant distance 1GD from the drain highly doped impurity region 4; and a source electrode 6 and a drain electrode 7 formed on the source highly doped impurity region 4 and the drain highly doped impurity region 4, respectively.
There is disclosed an FET having a high drain breakdown voltage and a short gate length comprising an active layer 2 formed on a surface layer of a semiconductor substrate 1; a source highly doped impurity region 4 and a drain highly doped impurity region 4 formed in the surface layer of the semiconductor substrate 1 to sandwich the active layer 2; an insulation film 5 formed on the source highly doped impurity region 4; a gate electrode 8 formed on the active layer 2 and the insulation film 5 while maintaining a constant distance 1GD from the drain highly doped impurity region 4; and a source electrode 6 and a drain electrode 7 formed on the source highly doped impurity region 4 and the drain highly doped impurity region 4, respectively.
Description
2n85~24 .
Field Eifect Transistor and Method ior Manufacturing the Same BACKGROUND OF THE INVENTION
Field o.4 the Invention The present invention relates to a high power ~4ield eil4ect transistor (FET) and method for manuiacturing the same.
Related Background Art Because a high power FET needs a high drain breakdown voltage, an FET having the ~ollowing structure has been proposed. An example is a recessed FET. In such an FET, a recess is l40rmed in a gate region by etching. As a gate electrode is iormed in the recess, a ~
source-gate distance is extended and a drain breakdown ~ -voltage i8 enhanced. In order to enhance the drain breakdown voltage, it has also been proposed to space a reiractry gate electrode irom a drain region ("A New Re4ractory Seli-Alighned Gate Tschnology ior GaAs Microwave Power FET's and MMIC's" IEEE TRANSACTIONS ON
ELECTRON DEVICES, vol. 35, No. 5, May 1~88).
However, in the prior art FET having the recess :~
structure, since the gate region is recessed by etching, it has been diiiicult to attain a highly reproducible device characteristic because oi reproducibility and controllability oi etching.
Field Eifect Transistor and Method ior Manufacturing the Same BACKGROUND OF THE INVENTION
Field o.4 the Invention The present invention relates to a high power ~4ield eil4ect transistor (FET) and method for manuiacturing the same.
Related Background Art Because a high power FET needs a high drain breakdown voltage, an FET having the ~ollowing structure has been proposed. An example is a recessed FET. In such an FET, a recess is l40rmed in a gate region by etching. As a gate electrode is iormed in the recess, a ~
source-gate distance is extended and a drain breakdown ~ -voltage i8 enhanced. In order to enhance the drain breakdown voltage, it has also been proposed to space a reiractry gate electrode irom a drain region ("A New Re4ractory Seli-Alighned Gate Tschnology ior GaAs Microwave Power FET's and MMIC's" IEEE TRANSACTIONS ON
ELECTRON DEVICES, vol. 35, No. 5, May 1~88).
However, in the prior art FET having the recess :~
structure, since the gate region is recessed by etching, it has been diiiicult to attain a highly reproducible device characteristic because oi reproducibility and controllability oi etching.
- 2~8~2~
1 In the FET discolsed in the above re~erence, the gate region is o~ non-etched planar structure but the material o~ the gate electrode must be a re~ractory material having a heat resistance, and a gate resistance is high. Further, it is dif~icult to attain a gate electrode o~ sub hal~ micron such as gate length o~ 0.5 ~m.
SUMMABY OF THE INVENTION ~ :
It is an object o~ the present invention to provide a ~ield e~ect transistor having a high gate breakdown voltage and a short gate length, and method ~or manu~acturing the same.
In order to achieve the above object, the FET o~ the present invention comprises:
an active layer ~ormed in a sur~ace layer o~ a semiconductor substrate;
a source highly doped impurity region and a drain highly doped impurity region iormed in the sur~ace layer o~ the semiconductor substrate to sandwich the active layer;
an insulation ~ilm ~ormed on the source highly doped impurity region;
a gate electrode ~ormed on the active layer and the insulation ~ilm while maintaining a constant distance ~rom the drain highly doped impurity region; and a source electrode and a drain electrode ~ormed on 2~85$2~
1 the source highly doped impurity region and the drain highly doped impurity region respectively.
The method ~or manu~acturing the FET o~ the present invention comprises the step o~:
~ orming an active layer in a surface layer o~ a semiconductor substrate;
~ orming a dummy gate on the active layer;
~ orming a source highly doped impurity region and a drain highly doped impurity region in the sur~ace layer o~ the semiconductor substrate by ion implantation using -the dummy gate as a mask;
depositing an insulation ~ilm on the sur~ace o~ the semiconductor substrate and liiting of~ the insulation ~ilm oi the dummy gate area by using the dummy gate;
removing the insulation ~ilms on the source highly doped impurity region which are spaced ~rom the active :
layer and ~orming a source electrode and a drain elctrode in the exposed areas; and : -~orming on the active layer a gate electrode having . .
one end thereor spaced ~rom the drain highly doped impurity region and the other end thereo~ overlapped on ~ .
; the imsulation ~ilm on the source highly doped impurity region. .
In accordance with the FET oi the present invention, since a portion o~ the gate elctrode is ~ormed on an insulation ~ilm adjacent to the source electrode in an 20~24 ~ 1 overlapped and or~set fashion, a certain distance is ; secured between the gate elctrode and the drain electrode. As a result, a high drain breakdown voltage is attained. An essential gate length is a portion Or ~ the gate electrode which contacts to an active layer, and s it is shorter than the length Or the gate electrode ~^ itselr.
The present invention will become more ~ully understood rrom the detailed description given hereinbelow and the accompanying drawings which are given by way o~ illustration only, and thus are not to be considered as limiting the present invention.
Further scope Or applicability Or the present invention will become apparent rrOm the detailed description given hereinarter. However, it should be understood that the detailed description and speciric ~ examples, while indicating prererred embodiments Or the i invention, are given by way Or illustration only, since ~ various changes and modirications within the spirit and ¦~ 20 scope Or the invention will become apparent to those skilled in the art iorm this detailed description.
BRIEF DESCRIPTION OF THE DRAWINGS
Figs. lA-lG show process sectional views Or one embodiment Or the method rOr manuracturing FET Or the ¦ present invention, I Fig. 2 shows a graph Or experimental data on a 2~8~24 1 relation between a distance lGD and a gate-drain breakdown voltage, and Fig. 3 shows a graph o+~ IdS-Vds characteristics of an FET having distance 1~ o~ 1.5 ~m and an FET having distance 16Dof 7.0 ~m. ~-DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
.
Figs. lA-lG show sectional views in a manuiacturing process to complete a Schottky barrier type FET (MESFET) in one embodiment oi the present invention. The manu~acturing process is explained below.
First, an active layer 2 is ~ormed in a suriace -~ -layer oi a semi-insulative GaAs semiconductor substrate 1. Then, a silicon nitride film 10 is deposited on the suriace oi the semiconductor substrate 1 to a thichness oi approximately lOOOA (see Fig. lA). The active layer 2 may be iormed by an ion implantation method in which Si+
ions having dose oi 3 x 1012/cm2 are accelerated under an elctric iield oi 30KeV. The silicon nitride iilm 10 may be iormed by a CVD method. The silicon nitride iilm 10 is used as a protection iilm ior a annealing process, which will be taken place later, ior the active layer 2.
Then, a dummy gate 3 in iormed by a opticallithography technique. A material oi the dummy gate 3 is a resist material, and a dimension ld oi the dummy gate 3 corresponding to the gate length is, ior example, 2 ~m. Then, a highly doped n+layer (n+ region) 2~552~
1 4 having a high impurity concentration is formed by an ion implantation method using the dummy gate 3 as a mask (see Fig. lB). The ion implantation is carried out while Si+ ions having dose o~ 4 x 10l3/cm2 are accelerated under application Or an electric rield Or 120 KeV. In Fig. lB, a lefthand n+ region 4 is a source highly doped impurity region, and a righthand n+ region 4 is a drain highly doped impurity region.
Then, the gate length Or the dummy gate 3 is slightly reduced. It is done by slightly and isotropically grinding the entire ~urrace (top surrace and side surrace) Or the dummy gate 3 by 2 plasma etching (see Fig. lC).
Then, an insulation rilm 5 made oi SiO2 is formed on the entire æurrace Or the substrate including the reduced dummy gate 3 (see Fig. lD). The dummy gate 3 is then lirted o~i to rOrm an insulation iilm 5 having a inversion pattern to the dummy gate 3 (see Fig. lE).
Then, in order to activate the Si+ ions implanted into the semiconductor substrate 1, it is annealed at 800 C
ror ~0 minutes. Then, ohmic electrode rormation areas in the insulation rilm 5 and the anneal protection rilm 10 are selectively removed by using a opticallithographic technique and an RIE method. A source electrode B and a drain electrode 2 which are made or AuGe/Ni metal are ~ormed on the n+ region 4 exposed by the removal (see 20~52~
- 1 Fig. lF).
-- A~ter the ~ormation o~ the ohmic electrodes, a gate electrode pattern is formed on the substate by the opticallithography technique. The pattern is ~ormed to be of~set toward the source electrode 6, that is, the center o~ the gate is o~set toward the source electrode ff. A low resistance metal made of Ti/Pt/Au is vapor-deposited on the gate electrode pattern, and the metal o~
unnecessary areas is removed by the li~t-o~ method to ~
~orm a gate electrode 8. As a result, an MESFET having a ;~-structure shown in Fig. lG is completed. A portion o~
the gate electrode 8 contacts to the active layer 2 and the remaining portion overlaps on the insulation ~ilm 5 which is adjacent to the source electrode 6.
Prior to the ~ormation o~ the gate electrode 8, the anneal protection ~ilm 10 in the gate electrode ~ormation -area on the active layer 2 is removed. Where the anneal protection ~ilm 10 is the silicon nitride ~ilm as it i9 in the present embodiment, it may be removed by the RIE
' 20 method using CF4. I~ the active layer 2 is annealed in ! an atmosphere o~ AsH3, anneal protection ~ilm 10 is not necessary.
In accordance with the present embodiment, since a I portion o~ the gate electrode 8 is ~ormed on the f insulation iilm 5 on the side o~ the source electrode 6 in the overlapped and oriset ~ashion, a constant distance ' ~.' 2~8~2~
lGD (1.5 ~m in the present embodiment) is secured between the gate electrode 8 and the n+ region 4 on the drain side. As a result, the drain breakdown voltage o~ the ' FET may be enhanced. Further, since only the portion of Z the gate electrode 8 is ~ormed on the active layer 2, the essential gate length lg is determined by the portion o~
the gate electrode 8 which contacts to the active layer 2. Namely, assuming that the metal length lM o~ the gate electrode 8 is 1.0 ~m and the overlap o~ the source electrode 6 on the insulation film 5 is 0.5 ~m, the actual gate length lg is 0.5 ~m.
Fig. 2 shows a graph o~ an experimental result on a relationship between the distance l~ and the gate-drain breakdown voltage (drain breakdown voltage). According to the experimental result, when the distance lOEZexceeds 1 ~m, the gate-drain breakdown voltage starts to saturate and it substantially saturates over 1.5 ~m.
On the other hand, ii the distance lOEZis too long, a device area increases and an electric ~ield concentrates towards the drain electrode so that a channel may be broken between the source and the drain. Fig. 3 shows a graph o~ IdS-Vds characteristics ~or the FET o~ the present embodiment having the distance lOE o~ 1.5 ~m and an FET having the distance l~ of 7.0 ~m. As seen ~rom the graph, when the distance l~ is 7.0 ~m, the breakdown occurs when the source-drain voltage Vds exceeds 10 2~8~5~4 1 volts. On the other hand, when the distance lGD is 1.5 ~m, the breakdown does not occur even if a higher voltage -is applied. In practice, it is pre~erable that the distance lGD is smaller than 5 ~m.
In accordance with the FET o~ the present invention, ~i a high drain breakdown voltage is attained by controlling the distance 1~.
Further, since the gate electrode 8 overlaps on the insulation ~ilm 5, the real gate length lg by which the gate electrode 8 contacts to the active layer 2 can be readily shortened, and it is possible to readily manu~acture the gate length o~ substantially sub-half-micron.
In accordance with the manufacturing method o~ the present invention, since the n~ region 4 is ~ormed by the ion implantation method using the dummy gate 3 as the mask, it is not necesæary to use a re~ractory material ior the gate eletrode 8. Aceordingly, a gate metal having a low resistanee may be used and the increase o~
the gate resistance is avoided. On the side o~ the source eleetrode 6, the n~ region 4 is sel~-aligned to the gate eleetrode 8 whieh is formed at the plaee oi the dummy gate 3. As a result, the resistanee between the Schottoky eontaet to the souree eleetrode 6 is redueed -~
and a source parasitie capacitance is reduced.
The FET o~ the present invention may be e~ectively -2a~5~2~
1 utilized as a high power device in a high ~requency band.
From the invention thus described, it will be obvious that the invention may be varied in many ways.
Such variations are not to be regarded as a departure ~rom the spirit and scope o~ the invention, and all such modi~ications as would be obvious to one skilled in the art are intended to be included within the scope o~ the ~ollowing claims.
1 In the FET discolsed in the above re~erence, the gate region is o~ non-etched planar structure but the material o~ the gate electrode must be a re~ractory material having a heat resistance, and a gate resistance is high. Further, it is dif~icult to attain a gate electrode o~ sub hal~ micron such as gate length o~ 0.5 ~m.
SUMMABY OF THE INVENTION ~ :
It is an object o~ the present invention to provide a ~ield e~ect transistor having a high gate breakdown voltage and a short gate length, and method ~or manu~acturing the same.
In order to achieve the above object, the FET o~ the present invention comprises:
an active layer ~ormed in a sur~ace layer o~ a semiconductor substrate;
a source highly doped impurity region and a drain highly doped impurity region iormed in the sur~ace layer o~ the semiconductor substrate to sandwich the active layer;
an insulation ~ilm ~ormed on the source highly doped impurity region;
a gate electrode ~ormed on the active layer and the insulation ~ilm while maintaining a constant distance ~rom the drain highly doped impurity region; and a source electrode and a drain electrode ~ormed on 2~85$2~
1 the source highly doped impurity region and the drain highly doped impurity region respectively.
The method ~or manu~acturing the FET o~ the present invention comprises the step o~:
~ orming an active layer in a surface layer o~ a semiconductor substrate;
~ orming a dummy gate on the active layer;
~ orming a source highly doped impurity region and a drain highly doped impurity region in the sur~ace layer o~ the semiconductor substrate by ion implantation using -the dummy gate as a mask;
depositing an insulation ~ilm on the sur~ace o~ the semiconductor substrate and liiting of~ the insulation ~ilm oi the dummy gate area by using the dummy gate;
removing the insulation ~ilms on the source highly doped impurity region which are spaced ~rom the active :
layer and ~orming a source electrode and a drain elctrode in the exposed areas; and : -~orming on the active layer a gate electrode having . .
one end thereor spaced ~rom the drain highly doped impurity region and the other end thereo~ overlapped on ~ .
; the imsulation ~ilm on the source highly doped impurity region. .
In accordance with the FET oi the present invention, since a portion o~ the gate elctrode is ~ormed on an insulation ~ilm adjacent to the source electrode in an 20~24 ~ 1 overlapped and or~set fashion, a certain distance is ; secured between the gate elctrode and the drain electrode. As a result, a high drain breakdown voltage is attained. An essential gate length is a portion Or ~ the gate electrode which contacts to an active layer, and s it is shorter than the length Or the gate electrode ~^ itselr.
The present invention will become more ~ully understood rrom the detailed description given hereinbelow and the accompanying drawings which are given by way o~ illustration only, and thus are not to be considered as limiting the present invention.
Further scope Or applicability Or the present invention will become apparent rrOm the detailed description given hereinarter. However, it should be understood that the detailed description and speciric ~ examples, while indicating prererred embodiments Or the i invention, are given by way Or illustration only, since ~ various changes and modirications within the spirit and ¦~ 20 scope Or the invention will become apparent to those skilled in the art iorm this detailed description.
BRIEF DESCRIPTION OF THE DRAWINGS
Figs. lA-lG show process sectional views Or one embodiment Or the method rOr manuracturing FET Or the ¦ present invention, I Fig. 2 shows a graph Or experimental data on a 2~8~24 1 relation between a distance lGD and a gate-drain breakdown voltage, and Fig. 3 shows a graph o+~ IdS-Vds characteristics of an FET having distance 1~ o~ 1.5 ~m and an FET having distance 16Dof 7.0 ~m. ~-DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
.
Figs. lA-lG show sectional views in a manuiacturing process to complete a Schottky barrier type FET (MESFET) in one embodiment oi the present invention. The manu~acturing process is explained below.
First, an active layer 2 is ~ormed in a suriace -~ -layer oi a semi-insulative GaAs semiconductor substrate 1. Then, a silicon nitride film 10 is deposited on the suriace oi the semiconductor substrate 1 to a thichness oi approximately lOOOA (see Fig. lA). The active layer 2 may be iormed by an ion implantation method in which Si+
ions having dose oi 3 x 1012/cm2 are accelerated under an elctric iield oi 30KeV. The silicon nitride iilm 10 may be iormed by a CVD method. The silicon nitride iilm 10 is used as a protection iilm ior a annealing process, which will be taken place later, ior the active layer 2.
Then, a dummy gate 3 in iormed by a opticallithography technique. A material oi the dummy gate 3 is a resist material, and a dimension ld oi the dummy gate 3 corresponding to the gate length is, ior example, 2 ~m. Then, a highly doped n+layer (n+ region) 2~552~
1 4 having a high impurity concentration is formed by an ion implantation method using the dummy gate 3 as a mask (see Fig. lB). The ion implantation is carried out while Si+ ions having dose o~ 4 x 10l3/cm2 are accelerated under application Or an electric rield Or 120 KeV. In Fig. lB, a lefthand n+ region 4 is a source highly doped impurity region, and a righthand n+ region 4 is a drain highly doped impurity region.
Then, the gate length Or the dummy gate 3 is slightly reduced. It is done by slightly and isotropically grinding the entire ~urrace (top surrace and side surrace) Or the dummy gate 3 by 2 plasma etching (see Fig. lC).
Then, an insulation rilm 5 made oi SiO2 is formed on the entire æurrace Or the substrate including the reduced dummy gate 3 (see Fig. lD). The dummy gate 3 is then lirted o~i to rOrm an insulation iilm 5 having a inversion pattern to the dummy gate 3 (see Fig. lE).
Then, in order to activate the Si+ ions implanted into the semiconductor substrate 1, it is annealed at 800 C
ror ~0 minutes. Then, ohmic electrode rormation areas in the insulation rilm 5 and the anneal protection rilm 10 are selectively removed by using a opticallithographic technique and an RIE method. A source electrode B and a drain electrode 2 which are made or AuGe/Ni metal are ~ormed on the n+ region 4 exposed by the removal (see 20~52~
- 1 Fig. lF).
-- A~ter the ~ormation o~ the ohmic electrodes, a gate electrode pattern is formed on the substate by the opticallithography technique. The pattern is ~ormed to be of~set toward the source electrode 6, that is, the center o~ the gate is o~set toward the source electrode ff. A low resistance metal made of Ti/Pt/Au is vapor-deposited on the gate electrode pattern, and the metal o~
unnecessary areas is removed by the li~t-o~ method to ~
~orm a gate electrode 8. As a result, an MESFET having a ;~-structure shown in Fig. lG is completed. A portion o~
the gate electrode 8 contacts to the active layer 2 and the remaining portion overlaps on the insulation ~ilm 5 which is adjacent to the source electrode 6.
Prior to the ~ormation o~ the gate electrode 8, the anneal protection ~ilm 10 in the gate electrode ~ormation -area on the active layer 2 is removed. Where the anneal protection ~ilm 10 is the silicon nitride ~ilm as it i9 in the present embodiment, it may be removed by the RIE
' 20 method using CF4. I~ the active layer 2 is annealed in ! an atmosphere o~ AsH3, anneal protection ~ilm 10 is not necessary.
In accordance with the present embodiment, since a I portion o~ the gate electrode 8 is ~ormed on the f insulation iilm 5 on the side o~ the source electrode 6 in the overlapped and oriset ~ashion, a constant distance ' ~.' 2~8~2~
lGD (1.5 ~m in the present embodiment) is secured between the gate electrode 8 and the n+ region 4 on the drain side. As a result, the drain breakdown voltage o~ the ' FET may be enhanced. Further, since only the portion of Z the gate electrode 8 is ~ormed on the active layer 2, the essential gate length lg is determined by the portion o~
the gate electrode 8 which contacts to the active layer 2. Namely, assuming that the metal length lM o~ the gate electrode 8 is 1.0 ~m and the overlap o~ the source electrode 6 on the insulation film 5 is 0.5 ~m, the actual gate length lg is 0.5 ~m.
Fig. 2 shows a graph o~ an experimental result on a relationship between the distance l~ and the gate-drain breakdown voltage (drain breakdown voltage). According to the experimental result, when the distance lOEZexceeds 1 ~m, the gate-drain breakdown voltage starts to saturate and it substantially saturates over 1.5 ~m.
On the other hand, ii the distance lOEZis too long, a device area increases and an electric ~ield concentrates towards the drain electrode so that a channel may be broken between the source and the drain. Fig. 3 shows a graph o~ IdS-Vds characteristics ~or the FET o~ the present embodiment having the distance lOE o~ 1.5 ~m and an FET having the distance l~ of 7.0 ~m. As seen ~rom the graph, when the distance l~ is 7.0 ~m, the breakdown occurs when the source-drain voltage Vds exceeds 10 2~8~5~4 1 volts. On the other hand, when the distance lGD is 1.5 ~m, the breakdown does not occur even if a higher voltage -is applied. In practice, it is pre~erable that the distance lGD is smaller than 5 ~m.
In accordance with the FET o~ the present invention, ~i a high drain breakdown voltage is attained by controlling the distance 1~.
Further, since the gate electrode 8 overlaps on the insulation ~ilm 5, the real gate length lg by which the gate electrode 8 contacts to the active layer 2 can be readily shortened, and it is possible to readily manu~acture the gate length o~ substantially sub-half-micron.
In accordance with the manufacturing method o~ the present invention, since the n~ region 4 is ~ormed by the ion implantation method using the dummy gate 3 as the mask, it is not necesæary to use a re~ractory material ior the gate eletrode 8. Aceordingly, a gate metal having a low resistanee may be used and the increase o~
the gate resistance is avoided. On the side o~ the source eleetrode 6, the n~ region 4 is sel~-aligned to the gate eleetrode 8 whieh is formed at the plaee oi the dummy gate 3. As a result, the resistanee between the Schottoky eontaet to the souree eleetrode 6 is redueed -~
and a source parasitie capacitance is reduced.
The FET o~ the present invention may be e~ectively -2a~5~2~
1 utilized as a high power device in a high ~requency band.
From the invention thus described, it will be obvious that the invention may be varied in many ways.
Such variations are not to be regarded as a departure ~rom the spirit and scope o~ the invention, and all such modi~ications as would be obvious to one skilled in the art are intended to be included within the scope o~ the ~ollowing claims.
Claims (11)
1. A field effect transistor comprising:
an active layer formed in a surface layer of a semiconductor substrate;
a source highly doped impurity region and a drain highly doped impurity region and a drain highly doped impurity region formed in the surface layer of the semiconductor substrate to sandwich the active layer;
an insulation film formed on the source highly doped impurity region;
a gate electrode formed on the active layer and the insulation film which maintaining a constant distance from the drain highly doped impurity region; and a source electrode and a drain electrode formed on the source highly doped impurity region and the drain highly doped impurity region, respectively.
an active layer formed in a surface layer of a semiconductor substrate;
a source highly doped impurity region and a drain highly doped impurity region and a drain highly doped impurity region formed in the surface layer of the semiconductor substrate to sandwich the active layer;
an insulation film formed on the source highly doped impurity region;
a gate electrode formed on the active layer and the insulation film which maintaining a constant distance from the drain highly doped impurity region; and a source electrode and a drain electrode formed on the source highly doped impurity region and the drain highly doped impurity region, respectively.
2. A field effect transistor according to Claim 1 wherein the distance between the gate electrode and the drain highly doped impurity region is between 1 µm and 5 µm, inclusive.
3. A field effect transistor according to Claim 2 wherein the insulation film formed on the source highly doped impurity region slightly overlaps on the active layer.
4. A field effect transistor according to Claim 3 wherein the semiconductor substrate is a compound semiconductor substrate.
5. A field effect transistor according to Claim 4 wherein the compound semiconductor substrate is a GaAs semiconductor substrate.
6. A method for manufacturing a field effect transistor comprising the steps of:
forming an active layer in a surface layer of a semiconductor substrate;
forming a dummy gate on the active layer;
forming a source highly doped impurity region and a drain highly doped impurity region in the surface layer of the semiconductor substrate by ion implantation using the dummy gate as a mask;
depositing an insulation film on the surface of the semiconductor substrate and lifting off the insulation film of the dummy gate area by using the dummy gate;
removing the insulation films on the source highly doped impurity region and the drain highly doped impurity region which are spaced from the active layer and forming a source electrode and a drain electrode in the exposed areas; and forming on the active layer a gate electrode having one end thereof spaced from the drain highly doped impurity region and the other end thereof overlapped on the insulation film on the source highly doped impurity region.
forming an active layer in a surface layer of a semiconductor substrate;
forming a dummy gate on the active layer;
forming a source highly doped impurity region and a drain highly doped impurity region in the surface layer of the semiconductor substrate by ion implantation using the dummy gate as a mask;
depositing an insulation film on the surface of the semiconductor substrate and lifting off the insulation film of the dummy gate area by using the dummy gate;
removing the insulation films on the source highly doped impurity region and the drain highly doped impurity region which are spaced from the active layer and forming a source electrode and a drain electrode in the exposed areas; and forming on the active layer a gate electrode having one end thereof spaced from the drain highly doped impurity region and the other end thereof overlapped on the insulation film on the source highly doped impurity region.
7. A method for manufacturing a field effect transistor acording to Claim 6 further comprising a step of reducing a gate length of the dummy gate prior to the lift-of step of the insulation film.
8. A method for manufacturing a field effect transistor according to Claim 7 wherein the dummy gate is a photoresist pattern and the step of reducing the gate length of the dummy gate is effected by slight etching of the surface of the dummy gate by an oxygen ion etching method.
9. A method for manufacturing a field effect transistor comprising the steps of:
forming an active layer in a surface layer of a semiconductor substrate;
forming an anneal protection film on the surface of the semiconductor substrate;
forming a dummy gate on the anneal protection film on the active layer;
forming a source highly doped impurity region and a drain highly doped impurity region in the surface layer of the semiconductor substrate by ion implantation using the dummy gate as a mask;
depositing an insulation film on the surface of the semiconductor substrate and lifting of the insulation film in the dummy gate area by using the dummy gate;
annealing the active layer;
removing the insulation film and the anneal protection film in the areas spaced from the active layer on the source highly doped impurity region and the drain highly doped impurity region and forming a source electorode and a drain electrode in the exposed areas;
and removing the anneal protection film on the active layer and forming on the active layer a gate electrode having one end thereof spaced from the drain highly doped impurity region and the other end thereof overlapped on the insulation film on the source highly doped impurity region.
forming an active layer in a surface layer of a semiconductor substrate;
forming an anneal protection film on the surface of the semiconductor substrate;
forming a dummy gate on the anneal protection film on the active layer;
forming a source highly doped impurity region and a drain highly doped impurity region in the surface layer of the semiconductor substrate by ion implantation using the dummy gate as a mask;
depositing an insulation film on the surface of the semiconductor substrate and lifting of the insulation film in the dummy gate area by using the dummy gate;
annealing the active layer;
removing the insulation film and the anneal protection film in the areas spaced from the active layer on the source highly doped impurity region and the drain highly doped impurity region and forming a source electorode and a drain electrode in the exposed areas;
and removing the anneal protection film on the active layer and forming on the active layer a gate electrode having one end thereof spaced from the drain highly doped impurity region and the other end thereof overlapped on the insulation film on the source highly doped impurity region.
10. A method for manufacturing a field effect transistor according to Claim 9 further comprising a step of reducing a gate length of the dummy gate prior to the lift-off step of the insulation film.
11. A method for manufacturing a field effect transistor according to Claim 10 wherein the dummy gate is a photoresist pattern and the step of reducing the gate length of the dummy gate is effected by slight etching of the surface of the dummy gate by an oxygen plasma etching method.
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2239699A JPH04119636A (en) | 1990-09-10 | 1990-09-10 | Field effect transistor and manufacture thereof |
US07/988,258 US5382821A (en) | 1992-12-14 | 1992-12-14 | High power field effect transistor |
CA002085524A CA2085524A1 (en) | 1990-09-10 | 1992-12-16 | Field effect transistor and method for manufacturing the same |
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2239699A JPH04119636A (en) | 1990-09-10 | 1990-09-10 | Field effect transistor and manufacture thereof |
US07/988,258 US5382821A (en) | 1992-12-14 | 1992-12-14 | High power field effect transistor |
CA002085524A CA2085524A1 (en) | 1990-09-10 | 1992-12-16 | Field effect transistor and method for manufacturing the same |
Publications (1)
Publication Number | Publication Date |
---|---|
CA2085524A1 true CA2085524A1 (en) | 1994-06-17 |
Family
ID=27169286
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CA002085524A Abandoned CA2085524A1 (en) | 1990-09-10 | 1992-12-16 | Field effect transistor and method for manufacturing the same |
Country Status (2)
Country | Link |
---|---|
JP (1) | JPH04119636A (en) |
CA (1) | CA2085524A1 (en) |
-
1990
- 1990-09-10 JP JP2239699A patent/JPH04119636A/en active Pending
-
1992
- 1992-12-16 CA CA002085524A patent/CA2085524A1/en not_active Abandoned
Also Published As
Publication number | Publication date |
---|---|
JPH04119636A (en) | 1992-04-21 |
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EEER | Examination request | ||
FZDE | Discontinued |