GB1585376A - Field effect transistor having an interdigital structure - Google Patents
Field effect transistor having an interdigital structure Download PDFInfo
- Publication number
- GB1585376A GB1585376A GB3442577A GB3442577A GB1585376A GB 1585376 A GB1585376 A GB 1585376A GB 3442577 A GB3442577 A GB 3442577A GB 3442577 A GB3442577 A GB 3442577A GB 1585376 A GB1585376 A GB 1585376A
- Authority
- GB
- United Kingdom
- Prior art keywords
- electrodes
- substrate
- gate
- source
- drain
- 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.)
- Expired
Links
- 230000005669 field effect Effects 0.000 title claims description 13
- 239000000758 substrate Substances 0.000 claims description 23
- 239000004065 semiconductor Substances 0.000 claims description 10
- 238000001465 metallisation Methods 0.000 claims description 9
- 238000000034 method Methods 0.000 claims description 4
- 239000000463 material Substances 0.000 claims description 3
- 230000003071 parasitic effect Effects 0.000 claims description 3
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 claims description 2
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 2
- 230000001629 suppression Effects 0.000 claims description 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- 239000010703 silicon Substances 0.000 description 2
- 239000008186 active pharmaceutical agent Substances 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 230000000135 prohibitive effect Effects 0.000 description 1
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
- H01L29/40—Electrodes ; Multistep manufacturing processes therefor
- H01L29/41—Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
- H01L29/417—Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions carrying the current to be rectified, amplified or switched
- H01L29/41725—Source or drain electrodes for field effect devices
- H01L29/4175—Source or drain electrodes for field effect devices for lateral devices where the connection to the source or drain region is done through at least one part of the semiconductor substrate thickness, e.g. with connecting sink or with via-hole
-
- 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
- H01L29/40—Electrodes ; Multistep manufacturing processes therefor
- H01L29/41—Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
- H01L29/417—Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions carrying the current to be rectified, amplified or switched
- H01L29/41725—Source or drain electrodes for field effect devices
- H01L29/41758—Source or drain electrodes for field effect devices for lateral devices with structured layout for source or drain region, i.e. the source or drain region having cellular, interdigitated or ring structure or being curved or angular
-
- 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
- H01L29/40—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
-
- 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
- H01L29/68—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
- H01L29/80—Field effect transistors with field effect produced by a PN or other rectifying junction gate, i.e. potential-jump barrier
- H01L29/812—Field effect transistors with field effect produced by a PN or other rectifying junction gate, i.e. potential-jump barrier with a Schottky gate
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)
- Junction Field-Effect Transistors (AREA)
Description
(54) A FIELD EFFECT TRANSISTOR HAVING AN
INTERDIGITAL STRUCTURE
(71) We, THOMSON-C SF, a French Body
Corporate, of 173, Boulevard Haussmann 75008 Paris - France - do hereby declare the invention, for which we pray that a patent may be granted to us, and the method by which it is to be performed, to be particularly described in and by the following statement:
This invention relates to field-effect transistors having an interdigital structure and to processes for producing these transistors. More particularly, the invention relates to fieldeffect transistors having their three electrodes (source, gate and drain) situated on the same surface of a semiconductor device and intended to operate at very high frequencies and relatively high power levels.
It is known that power transistors for very high frequency applications can only be produced in the form of interdigital structures.
Now, in the case of devices having their three electrodes distributed over the same surface of the substrate, the input or output connections of the electrodes necessarily cross in the common distribution plane. Although it is known how to produce crossings such as these by the interposition of insulating layers, the outcome is an increase in the complexity of construction, in addition to which troublesome parasitic capacitances are created between connections which is harmful and, in some cases, prohibitive in very high frequency applications.
It is also known how to construct interdigital structures having only two electrodes on one
surface of the substrate with a common gate on
the opposite surface. However, the control of
a gate such as this lacks rapidity and, for this
reason, is not always suitable in very high
frequency applications.
The present invention obviates these various
disadvantages.
According to the present invention there is
provided a field effect transistor comprising a
heavily doped semiconductor substrate carrying
a first high resistivity semiconductor layer and
an overlying semiconductor layer, a series of
parallel grooves being etched in the surface of
said layers to a depth sufficient to cut into said
substrate, a first set of electrodes destined to be
source or drain electrodes being deposited in
the shape of metallizations in said grooves and on the margins of the same, a second and a third set of electrodes parallel to said grooves being deposited so as to form an interdigitated structure with said grooves, the electrodes of said second and third sets being interconnected by two metallizations each of them forming the spine of a comb having respectively the electrodes of one set as teeth, and the electrodes of said first set being interconnected by the substrate itself.
The invention will be better understood and other features thereof will become apparent from the following description in conjunction with the accompanying drawings wherein:
Figure 1 is a sectional view illustrating a first embodiment of the invention.
Figures 2 and 3 are explanatory diagrams.
In the embodiment of Figure 1 there is formed on a silicon substrate 41 with P+ (or N+) - type doping layer of very high resistivity (F.R.) 42 (obtained for example by epitaxial growth without any doping in the case of silicon) and then an N-doped layer 43 (for example by a second epitaxial growth). Grooves 44 pe+netratirsg into the layers 42 and 43 up to the P (or ma material of the substrate 41 are then physically or chemically etched at the place intended for the drain (or source) electrode. A metallisation 45 covering the groove and overlapping the two sides is deposited at the same time as the deposition of other electrodes S, G. In the example selected, gate electrodes have been interposed both in the intervals SD and also in the intervals DS. An arrangement such as this enables the efficiency of the interdigital structure to be increased whilst doubling the current output of each electrode. This is because, in a series of transistors such as that illustrated in Figure 2, the roles of the source and drain may be reversed in alternate devices. This reversal is effected by connecting the electrodes selected as source to the so-called "source" feed terminal, i.e. the feed terminal giving the lowest d.c. voltage, and the electrodes selected as drains to the opposite feed terminal. Under these conditions, it is possible to simplify the structure shown in
Figure 2 by merging the intermediate electrodes into pairs which gives the block diagram shown in Figure 3 which is no different from that shown in Figure 1 apart from the particular profile of the electrodes D in this latter case.
In this embodiment, all the drains have common conducive path formed by the P substrate. The P -substrate is provided with a metallisation 46 which is intended to facilitate the connection to the feed drain and to the load circuits.
In addition to the above-mentioned advantage of reducing the parasitic capacitance between electrode connections, the embodiment of Figure 1 has the following advantages:
1 - the almost complete suppression of the inherent inductance of the electrode interconnected by the substrate rendered conductive by doping, which is a particularly important advantage when the electrode in question is the source (contrary to the illustration in Figures 1); 2 - the reduction in the thermal resistance, particularly in the case of a substrate of gallium arsenide, the doping of this material reducing its resistivity;
3 - compatibility with methods of thinning down the substrate for reducing its thermal resistance.
WHAT WE CLAIM IS:
1. A field effect transistor comprising a heavily doped semiconductor substrate carrying a first high resistivity semiconductor layer and an overlying semiconductor layer, a series of parallel grooves being etched in the surface of said layers to a depth sufficient to cut into said substrate, a first set of electrodes destined to be source or drain electrodes being deposited in the shape of metallizations in said grooves and on the margins of the same, a second and a third set of electrodes parallel to said grooves being deposited so as to form an interdigital structure with said grooves, the electrodes of said second and third sets being interconnected by two metallizations each of them forming the spine of a comb having respectively the electrodes of one set as teeth, and the elctrodes of said first set being interconnected by the substrate itself.
2. A field effect transistor as claimed in claim 1, wherein the sequence of interdigitated electrodes is as follows:
source, gate, drain, gate, source, gate, drain.
3. A field effect transistor as claimed in claim 1, wherein: the sequence of interdigitated electrodes is as follows:
drain, gate, source, gate, drain, gate, source.
4. A field effect transistor substantially as herein before described with reference to the accompanying drawings.
**WARNING** end of DESC field may overlap start of CLMS **.
Claims (4)
1 - the almost complete suppression of the inherent inductance of the electrode interconnected by the substrate rendered conductive by doping, which is a particularly important advantage when the electrode in question is the source (contrary to the illustration in Figures 1);
2 - the reduction in the thermal resistance, particularly in the case of a substrate of gallium arsenide, the doping of this material reducing its resistivity;
3 - compatibility with methods of thinning down the substrate for reducing its thermal resistance.
WHAT WE CLAIM IS:
1. A field effect transistor comprising a heavily doped semiconductor substrate carrying a first high resistivity semiconductor layer and an overlying semiconductor layer, a series of parallel grooves being etched in the surface of said layers to a depth sufficient to cut into said substrate, a first set of electrodes destined to be source or drain electrodes being deposited in the shape of metallizations in said grooves and on the margins of the same, a second and a third set of electrodes parallel to said grooves being deposited so as to form an interdigital structure with said grooves, the electrodes of said second and third sets being interconnected by two metallizations each of them forming the spine of a comb having respectively the electrodes of one set as teeth, and the elctrodes of said first set being interconnected by the substrate itself.
2. A field effect transistor as claimed in claim 1, wherein the sequence of interdigitated electrodes is as follows:
source, gate, drain, gate, source, gate, drain.
3. A field effect transistor as claimed in claim 1, wherein: the sequence of interdigitated electrodes is as follows:
drain, gate, source, gate, drain, gate, source.
4. A field effect transistor substantially as herein before described with reference to the accompanying drawings.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR7625230A FR2362492A1 (en) | 1976-08-19 | 1976-08-19 | FIELD EFFECT TRANSISTOR WITH PROHIBITED STRUCTURE AND METHODS FOR MANUFACTURING THE SAID TRANSISTOR |
Publications (1)
Publication Number | Publication Date |
---|---|
GB1585376A true GB1585376A (en) | 1981-03-04 |
Family
ID=9177008
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB3442577A Expired GB1585376A (en) | 1976-08-19 | 1977-08-16 | Field effect transistor having an interdigital structure |
Country Status (4)
Country | Link |
---|---|
JP (1) | JPS5324788A (en) |
DE (1) | DE2737503A1 (en) |
FR (1) | FR2362492A1 (en) |
GB (1) | GB1585376A (en) |
Families Citing this family (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5448574U (en) * | 1977-08-19 | 1979-04-04 | ||
GB2049273B (en) * | 1979-05-02 | 1983-05-25 | Philips Electronic Associated | Method for short-circuting igfet source regions to a substrate |
DE3245457A1 (en) * | 1982-12-08 | 1984-06-14 | Siemens AG, 1000 Berlin und 8000 München | SEMICONDUCTOR ELEMENT WITH CONTACT HOLE |
FR2545295B1 (en) * | 1983-04-29 | 1985-07-12 | Thomson Csf | POWER MICROWAVE AMPLIFIER |
FR2637737A1 (en) * | 1988-10-07 | 1990-04-13 | Thomson Hybrides Microondes | III-V material power transistor on a silicon substrate, and its method of manufacture |
JP5985282B2 (en) * | 2012-07-12 | 2016-09-06 | ルネサスエレクトロニクス株式会社 | Semiconductor device |
-
1976
- 1976-08-19 FR FR7625230A patent/FR2362492A1/en active Granted
-
1977
- 1977-08-16 GB GB3442577A patent/GB1585376A/en not_active Expired
- 1977-08-19 JP JP9939177A patent/JPS5324788A/en active Pending
- 1977-08-19 DE DE19772737503 patent/DE2737503A1/en not_active Withdrawn
Also Published As
Publication number | Publication date |
---|---|
FR2362492A1 (en) | 1978-03-17 |
FR2362492B1 (en) | 1982-06-18 |
JPS5324788A (en) | 1978-03-07 |
DE2737503A1 (en) | 1978-02-23 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PS | Patent sealed | ||
PCNP | Patent ceased through non-payment of renewal fee |