CN109686810A - Side grid field effect transistor terahertz detector and preparation method thereof - Google Patents
Side grid field effect transistor terahertz detector and preparation method thereof Download PDFInfo
- Publication number
- CN109686810A CN109686810A CN201811559379.4A CN201811559379A CN109686810A CN 109686810 A CN109686810 A CN 109686810A CN 201811559379 A CN201811559379 A CN 201811559379A CN 109686810 A CN109686810 A CN 109686810A
- Authority
- CN
- China
- Prior art keywords
- table top
- effect transistor
- field effect
- grid
- substrate
- 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.)
- Pending
Links
- 230000005669 field effect Effects 0.000 title claims abstract description 52
- 238000002360 preparation method Methods 0.000 title claims description 10
- 239000000758 substrate Substances 0.000 claims abstract description 36
- 238000005530 etching Methods 0.000 claims abstract description 9
- 239000004065 semiconductor Substances 0.000 claims description 8
- 239000000463 material Substances 0.000 claims description 7
- 229910001218 Gallium arsenide Inorganic materials 0.000 claims description 6
- 229910052710 silicon Inorganic materials 0.000 claims description 6
- 239000010703 silicon Substances 0.000 claims description 6
- 229910008599 TiW Inorganic materials 0.000 claims description 5
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 claims description 5
- 229910052782 aluminium Inorganic materials 0.000 claims description 5
- 229910052750 molybdenum Inorganic materials 0.000 claims description 5
- 229910052759 nickel Inorganic materials 0.000 claims description 5
- 229910052763 palladium Inorganic materials 0.000 claims description 5
- 229910052697 platinum Inorganic materials 0.000 claims description 5
- 229910052718 tin Inorganic materials 0.000 claims description 5
- 229910052719 titanium Inorganic materials 0.000 claims description 5
- 229910002601 GaN Inorganic materials 0.000 claims description 4
- JMASRVWKEDWRBT-UHFFFAOYSA-N Gallium nitride Chemical compound [Ga]#N JMASRVWKEDWRBT-UHFFFAOYSA-N 0.000 claims description 4
- 229910003460 diamond Inorganic materials 0.000 claims description 4
- 239000010432 diamond Substances 0.000 claims description 4
- 229910044991 metal oxide Inorganic materials 0.000 claims description 3
- 150000004706 metal oxides Chemical class 0.000 claims description 3
- 229910052594 sapphire Inorganic materials 0.000 claims description 3
- 239000010980 sapphire Substances 0.000 claims description 3
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 claims description 3
- 229910010271 silicon carbide Inorganic materials 0.000 claims description 3
- 230000007480 spreading Effects 0.000 claims description 3
- 238000003892 spreading Methods 0.000 claims description 3
- 229910000831 Steel Inorganic materials 0.000 claims 1
- 239000004020 conductor Substances 0.000 claims 1
- 239000010959 steel Substances 0.000 claims 1
- 230000004044 response Effects 0.000 abstract description 5
- 230000005533 two-dimensional electron gas Effects 0.000 description 21
- 239000000523 sample Substances 0.000 description 14
- 229910052751 metal Inorganic materials 0.000 description 13
- 239000002184 metal Substances 0.000 description 13
- 238000001514 detection method Methods 0.000 description 11
- 238000000034 method Methods 0.000 description 9
- 238000001312 dry etching Methods 0.000 description 6
- 230000005611 electricity Effects 0.000 description 6
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 description 5
- GPXJNWSHGFTCBW-UHFFFAOYSA-N Indium phosphide Chemical compound [In]#P GPXJNWSHGFTCBW-UHFFFAOYSA-N 0.000 description 5
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 5
- 238000013461 design Methods 0.000 description 4
- 230000008901 benefit Effects 0.000 description 3
- 230000006378 damage Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 238000001259 photo etching Methods 0.000 description 3
- 230000008569 process Effects 0.000 description 3
- 230000004043 responsiveness Effects 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 239000007772 electrode material Substances 0.000 description 2
- 238000005566 electron beam evaporation Methods 0.000 description 2
- 238000001017 electron-beam sputter deposition Methods 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 230000003628 erosive effect Effects 0.000 description 2
- 238000003384 imaging method Methods 0.000 description 2
- 238000002347 injection Methods 0.000 description 2
- 239000007924 injection Substances 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000002070 nanowire Substances 0.000 description 2
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 1
- -1 Lan Bao Stone Chemical compound 0.000 description 1
- 208000027418 Wounds and injury Diseases 0.000 description 1
- 229910045601 alloy Inorganic materials 0.000 description 1
- 239000000956 alloy Substances 0.000 description 1
- 238000000137 annealing Methods 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000002146 bilateral effect Effects 0.000 description 1
- 238000003763 carbonization Methods 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 238000012512 characterization method Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 230000007797 corrosion Effects 0.000 description 1
- 238000005260 corrosion Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000003745 diagnosis Methods 0.000 description 1
- 229910052733 gallium Inorganic materials 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 208000014674 injury Diseases 0.000 description 1
- 238000002955 isolation Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 239000000243 solution Substances 0.000 description 1
- 238000004611 spectroscopical analysis Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
- 230000010356 wave oscillation Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/08—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors
- H01L31/10—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors characterised by potential barriers, e.g. phototransistors
- H01L31/101—Devices sensitive to infrared, visible or ultraviolet radiation
- H01L31/11—Devices sensitive to infrared, visible or ultraviolet radiation characterised by two potential barriers, e.g. bipolar phototransistors
- H01L31/1105—Devices sensitive to infrared, visible or ultraviolet radiation characterised by two potential barriers, e.g. bipolar phototransistors the device being a bipolar phototransistor
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/02—Details
- H01L31/0224—Electrodes
- H01L31/022408—Electrodes for devices characterised by at least one potential jump barrier or surface barrier
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/08—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors
- H01L31/10—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors characterised by potential barriers, e.g. phototransistors
- H01L31/101—Devices sensitive to infrared, visible or ultraviolet radiation
- H01L31/112—Devices sensitive to infrared, visible or ultraviolet radiation characterised by field-effect operation, e.g. junction field-effect phototransistor
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/08—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors
- H01L31/10—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors characterised by potential barriers, e.g. phototransistors
- H01L31/101—Devices sensitive to infrared, visible or ultraviolet radiation
- H01L31/112—Devices sensitive to infrared, visible or ultraviolet radiation characterised by field-effect operation, e.g. junction field-effect phototransistor
- H01L31/1121—Devices with Schottky gate
- H01L31/1123—Devices with Schottky gate the device being a photo MESFET
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/08—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors
- H01L31/10—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof in which radiation controls flow of current through the device, e.g. photoresistors characterised by potential barriers, e.g. phototransistors
- H01L31/101—Devices sensitive to infrared, visible or ultraviolet radiation
- H01L31/112—Devices sensitive to infrared, visible or ultraviolet radiation characterised by field-effect operation, e.g. junction field-effect phototransistor
- H01L31/113—Devices sensitive to infrared, visible or ultraviolet radiation characterised by field-effect operation, e.g. junction field-effect phototransistor being of the conductor-insulator-semiconductor type, e.g. metal-insulator-semiconductor field-effect transistor
- H01L31/1136—Devices sensitive to infrared, visible or ultraviolet radiation characterised by field-effect operation, e.g. junction field-effect phototransistor being of the conductor-insulator-semiconductor type, e.g. metal-insulator-semiconductor field-effect transistor the device being a metal-insulator-semiconductor field-effect transistor
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/18—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/18—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
- H01L31/1804—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof comprising only elements of Group IV of the Periodic Table
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/18—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
- H01L31/1804—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof comprising only elements of Group IV of the Periodic Table
- H01L31/1812—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof comprising only elements of Group IV of the Periodic Table including only AIVBIV alloys, e.g. SiGe
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/18—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
- H01L31/184—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof the active layers comprising only AIIIBV compounds, e.g. GaAs, InP
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L31/00—Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
- H01L31/18—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof
- H01L31/184—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof the active layers comprising only AIIIBV compounds, e.g. GaAs, InP
- H01L31/1856—Processes or apparatus specially adapted for the manufacture or treatment of these devices or of parts thereof the active layers comprising only AIIIBV compounds, e.g. GaAs, InP comprising nitride compounds, e.g. GaN
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02P—CLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
- Y02P70/00—Climate change mitigation technologies in the production process for final industrial or consumer products
- Y02P70/50—Manufacturing or production processes characterised by the final manufactured product
Landscapes
- Engineering & Computer Science (AREA)
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Electromagnetism (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Manufacturing & Machinery (AREA)
- Junction Field-Effect Transistors (AREA)
Abstract
The invention discloses a kind of side grid field effect transistor terahertz detectors, comprising: substrate;Table top, by by growth on substrate active layer etching after formed, or by growing active layer on substrate after, formed after etched portions substrate and active layer;Grid, setting are located at table top two sides, form Schottky contacts with table top;Source electrode and drain electrode, setting are located at the other two sides of table top, form Ohmic contact with table top.The present invention is designed using side gate transistor device structure, the spurious mode in channel can be greatly reduced, to improve the resonance response characteristic of transistor terahertz detector.
Description
Technical field
The present invention relates to terahertz detections and field of manufacturing semiconductor devices, and in particular to a kind of side grid field effect transistor
Structure of terahertz detector and preparation method thereof.
Background technique
THz wave due to its band characteristic, be suitable for material characterization, high-resolution imaging, medical diagnosis, safety check,
The various fields such as information communication, radar detection, atmosphere and environment measuring, national economy and in terms of all have
Important application prospect.Traditional terahertz detector needs work in low temperature mostly, and volume is larger, inconvenient to use, and responds
Speed is slower.FET sensor is a kind of continuously adjustable terahertz detection of look-in frequency developed in recent years
Device.Its basic detection principle is formed under specific boundary conditions using the two-dimensional electron gas in field-effect transistor structure
Plasma wave oscillation effect couples or resonates with incident THz wave, and then converts in the output end of transistor
For photoelectric current or photovoltage.High electron mobility transistor detector based on two-dimensional electron gas has high speed, highly sensitive, low
The advantages such as noise, high-frequency distinguishing, working and room temperature.In addition, the detector be also equipped with structure it is simple, it is simple for production, be easy to plus
The features such as work integrates obtains the great attention of people at present.
THz wave detection, which is carried out, using field effect transistor is divided into off-resonance detection mode and resonant probe mould
Formula.People have carried out a large amount of research to the off-resonance detection of field effect transistor and resonant probe, and use GaAs, nitrogen
The FET device of the change multiple materials such as gallium and indium phosphide has been observed in low temperature and at room temperature to THz wave
Resonance response.But the progress in field effect transistor Terahertz resonant probe field is slow.The resonance reported a little at present
The experimental result of detection is far below theory expectation.This is mainly reflected in two o'clock: first point be resonant probe responsiveness it is very low, very
To lower than the responsiveness under off-resonance detection mode;Second point is that the bandwidth of resonant probe response peak is very big, does not meet resonance and visits
The theoretical model of survey.Two above phenomenon also limits resonant probe mode the answering in practical field of field effect transistor
With.
The reason of generating the above phenomenon is since the grid width (W) of the transistor of conventional structure can all be much larger than the grid of transistor
Long (L), causes the plasma wave in transistor channel other than natural oscillation mode, there is also other spurious modes,
So that the resonant probe peak stretching of transistor, responsiveness decline.As shown in Figure 9 and Figure 10.There is study group to attempt using dry
The method of method etching reduces the grid width of transistor, but this method is limited to the result promotion of resonant probe.Though because firstly,
Right dry etching can be such that the roomy amplitude of transistor gate reduces, but because technological ability limits, the transistor grid width after etching
Still long in same order with transistor gate;Secondly, the plasma bombardment in dry etching is brought to the side wall of table top
Etching injury, increases sidewall surfaces roughness, and then increase the surface scattering of two-dimensional electron gas, reduces Two-dimensional electron
The mobility of gas.It can thus be seen that relying solely on dry etch process physically to reduce the grid width of transistor, it is difficult to reach
To the requirement theoretically to terahertz detector resonant probe.
Summary of the invention
The purpose of the present invention is to provide a kind of side grid field effect transistor terahertz detectors and preparation method thereof, so that
Field effect transistor Terahertz device is in terahertz light spectroscopy, terahertz imaging, the application performance in the fields such as safety check and biomedicine
It effectively improves.
In view of this, the present invention provides a kind of side grid field effect transistor terahertz detectors, wherein applied field
Effect transistor includes: Metal-Oxide Semiconductor field effect transistor, and metal-semiconductor field effect transistor, metal-is absolutely
Edge semiconductor field effect transistor, modulation-doped FET, junction field effect transistor and high electron mobility field effect
Answer transistor.
Grid field effect transistor terahertz detector in side provided by the invention includes:
Substrate;
Further, substrate material are as follows: gallium nitride, GaAs, indium phosphide, diamond, sapphire, silicon carbide or silicon.
Table top, by by growth on substrate active layer etching after formed, or by growing active layer on substrate after, carve
It is formed after erosion section substrate and active layer;
Further, table top is relative to substrate protrusion, and table surface height is more than or equal to active layer thickness.
Grid, setting are located at table top two sides, form Schottky contacts with table top;
Further, the number of grid is 2 or 2 or more, wherein at least has 2 grids to be located at the two of table top
Side, and be only in contact with the side surface of table top.
Source electrode and drain electrode, setting are located at the other two sides of table top, form Ohmic contact with table top.
Further, source electrode and drain electrode forms Ohm contact electrode, which connects with the side surface of table top
Touching, or be in contact with the upper surface of table top, or be in contact simultaneously with the side surface of table top and upper surface.
Further, above-mentioned grid, source electrode and drain electrode material comprise at least one of the following: Ti, Al, Ni, Mo,
Pt, Pd, Au, W, TiW and TiN.
Based on above-mentioned side grid field effect transistor terahertz detector, the present invention also provides a kind of above-mentioned side gate field-effects
The preparation method of transistor terahertz detector, comprising:
On substrate by injecting, spreading or be epitaxially-formed active layer;
It etches active layer or active layer and section substrate to form table top, the height of table top is more than or equal to the thickness for having edge layer
Degree;
Ohm contact electrode is prepared at the both ends of table top;
Gate electrode is prepared at the other both ends of table top.
The advantage of the invention is that designing using side gate transistor device structure, (grid can be parallel in the horizontal direction
Pole and substrate direction) it is modulated by the electricity of side grid to control the width of FET device two-dimensional electron gas channel, together
When two-dimensional electron gas is not caused to exhaust (perpendicular to grid and substrate direction) in vertical direction and (keeps two-dimensional electron gas
Concentration and mobility are constant).So it so that transistor device is formed nano wire Two-dimensional electron gas channel, but also can make
Two-dimensional electron gas is not influenced by dry etching damage, keeps the high mobility of two-dimensional electron gas.Using side gate transistor structure,
The spurious mode in channel can be greatly reduced, to improve the resonance response characteristic of transistor terahertz detector.
Detailed description of the invention
To further illustrate the contents of the present invention and feature, it is detailed that one is made to the present invention with reference to the accompanying drawings and embodiments
Description, in which:
Fig. 1-Fig. 7 is the process flow chart of the embodiment of the present invention;
Fig. 8 is the structural schematic diagram of grid field effect transistor terahertz detector in side provided in an embodiment of the present invention;
Fig. 9-Figure 10 is propagation schematic diagram of the plasma wave in the transistor of different grid width;
Figure 11-Figure 12 is the schematic illustration that grid field effect transistor electricity in side modulates two-dimensional electron gas channel width.
Specific embodiment
To make the objectives, technical solutions, and advantages of the present invention clearer, below in conjunction with specific embodiment, and reference
Attached drawing, the present invention is described in further detail.
One embodiment of the invention provides a kind of side grid field effect transistor terahertz detector, and applied field-effect is brilliant
Body pipe includes but is not limited to: Metal-Oxide Semiconductor field effect transistor, metal-semiconductor field effect transistor, metal-
Insulator-semiconductor field effect transistor, modulation-doped FET, junction field effect transistor and high electron mobility field
Effect transistor.
Fig. 8 is please referred to, is the concrete structure schematic diagram of the present embodiment, it can be seen that the detector includes:
Substrate;
In the present embodiment, substrate 100, material includes but is not limited to gallium nitride, GaAs, indium phosphide, diamond, Lan Bao
Stone, silicon carbide and silicon.
Table top, by by growth on substrate active layer etching after formed, or by growing active layer on substrate after, carve
It is formed after erosion section substrate and active layer;
In some embodiments, table top is relative to substrate protrusion, and table surface height is more than or equal to active layer thickness.
In the present embodiment, please refer to Fig. 1-Fig. 3, on substrate 100 in the way of injection, doping or epitaxial growth etc. shape
At active layer 200, the active layer 200 and section substrate are etched, obtains a table top 210, which is in a square relative to substrate
Shape protrusion, there are four side surface 211,212,213,214 and a upper surfaces 215 for tool.
The detector further comprises:
Source electrode and drain electrode, setting are located at table top two sides, form Ohmic contact with table top.
In some embodiments, source electrode and drain electrode forms Ohm contact electrode, the side surface of the Ohm contact electrode and table top
It is in contact, or is in contact with the upper surface of table top, or be in contact simultaneously with the side surface of table top and upper surface.
In the present embodiment, referring to figure 4. and Fig. 5, Ohm contact electrode 301,302, the both side surface with rectangular mesa
211, it 213 is in contact.
In another embodiment, Ohm contact electrode 301,302 is in contact (in figure not with the upper surface 215 of rectangular mesa
Show).
In another embodiment, a side surface 211 and upper surface 215 for an Ohm contact electrode 301 and rectangular mesa is simultaneously
It is in contact, the same phase in another corresponding side surface 213 and upper surface 215 of another Ohm contact electrode 302 and rectangular mesa
Contact (not shown).
The detector further include:
Grid, setting are located at the other two sides of table top, form Schottky contacts with table top;
In some embodiments, the number of grid is 2 or 2 or more, wherein at least has 2 grids to be located at table top
Two sides, and be only in contact with the side surface of table top.
In the present embodiment, Fig. 6 and Fig. 7 are please referred to, there are two grids 401,402 for tool, are located at rectangular mesa in addition
Two sides form Schottky contacts with the other both side surface 212,214 of rectangular mesa.
In some embodiments, above-mentioned grid, source electrode and drain electrode material comprise at least one of the following or several: Ti, Al,
Ni, Mo, Pt, Pd, Au, W, TiW and TiN.
Based on above-mentioned side grid field effect transistor terahertz detector, another embodiment of the present invention provides a kind of side grid fields
The preparation method of effect transistor terahertz detector, includes the following steps:
Step 1: on substrate by injecting, spreading or be epitaxially-formed active layer;
In the present embodiment, then Fig. 1 is please referred to, the sides such as injection, doping or epitaxial growth are utilized on sample 100 to be prepared
Formula forms active layer 200.The material of the sample 100 can be gallium nitride, GaAs, indium phosphide, diamond, sapphire, carbonization
Silicon or silicon.
Step 2: etching active layer or active layer and section substrate to form table top, the height of table top, which is more than or equal to, has chance with
The thickness of layer;
In the present embodiment, then referring to figure 2. and Fig. 3, on sample 100 to be prepared using photoetching combination dry etching or
Wet etch techniques form table top figure 210.Wherein: the shape of table top figure 210 can be square or rectangle or for its
His shape;Table top figure 210 possesses 4 side surfaces, and respectively 211,212,213,214;Table top figure 210 possesses 1 upper table
Face is 215;The height of the table top figure 210 is greater than the thickness of active layer 200.In this way, to the active area of device into
Row isolation.
Step 3: preparing Ohm contact electrode at the both ends of table top;
In the present embodiment, then referring to figure 4. and Fig. 5, using photoetching, electron beam evaporation or sputtering technology, in table top figure
The both ends of shape 210 prepare metal electrode 301 and 302.Metal electrode 301 and 302 must be contacted with generating between active layer 200.Tool
For body: metal electrode 301 and 302 both can be contacted only with the side surface of table top figure 210 211 and 213, can also only with platform
The upper surface 215 of face figure 210 contacts, it might even be possible at the same with the side surface of table top figure 210 211 and 213 and table top figure
The upper surface 215 of shape 210 is in contact.Be shown as in figure, the side surface 211 of metal electrode 301 and 302 and table top figure 210 and
213 are in contact, and Ohmic contact is formed between metal electrode 301 and 302 and active layer 200, in order to achieve this goal, must having
In the case where wanting, high temperature alloy annealing must be carried out to sample.The metal of metal electrode 301 and 302 can for Ti, Al, Ni, Mo,
Pt, Pd, Au, W, TiW, TiN and any combination between them.
Step 4: preparing gate electrode at the other both ends of table top;
In the present embodiment, then Fig. 6 and Fig. 7 are please referred to, using photoetching, electron beam evaporation or sputtering technology, in table top figure
The other both ends of shape 210 prepare metal electrode 401 and 402.It generates and contacts between metal electrode 401 and 402 and active layer 200.
Specifically: metal electrode 401 and 402, which only allows to generate with the side surface 212 and 214 of table top figure 210, to be contacted, it is not possible to
The upper surface 215 of table top figure 210 generates contact.Palpiform is at schottky junctions between metal electrode 401 and 402 and active layer 200
Touching.The metal of metal electrode 401 and 402 can be Ti, Al, Ni, Mo, Pt, Pd, Au, W, TiW, TiN and any between them
Combination.
So far, the structure design of side grid field effect transistor terahertz detection device is completed.
Based on side grid field effect transistor terahertz detection device structure provided by the invention, at this to its excellent
Gesture is described in further detail, and please refers to Fig. 9 to Figure 12, shows grid field effect transistor electricity tune in side provided by the present invention
The basic principle of Two-dimensional electron gas channel processed.
Figure 11 is please referred to, first to apply negative electricity when two side grid of side gate transistor with high electron mobility terahertz detector
When pressure, two side grid can start to exhaust the two-dimensional electron gas in high electron mobility transistor channel, Two-dimensional electron gas channel
Channel width starts to narrow.But because the negative voltage of side grid at this time is big not enough, the width of Two-dimensional electron gas channel still compared with
Greatly, at this moment if detecting to incident THz wave, the plasma wave in channel still can have as shown in Figure 9 miscellaneous
Dissipate mode.And as the minus gate voltage of our side grid is gradually increased (as shown in figure 12), Two-dimensional electron gas channel will continue to narrow, most
One-dimensional electric channel is formed afterwards, and at this moment the plasma wave in channel is just only left eigen mode as shown in Figure 10, spuious mould
Formula will be eliminated, so that us be facilitated to carry out resonant probe to incident THz wave.
A kind of design of side grid field effect transistor disclosed by the invention, be widely used in include silicon substrate, GaAs base and
The field effect transistor terahertz detector of indium phosphide.Field-effect crystalline substance is prepared by dry etching or wet corrosion technique
The table top of body pipe;And at least two be located at transistor mesa two sides form Xiao Te with the side surface of transistor mesa
The grid of base contact completes device structure design.By this device structure design, (grid can be parallel in the horizontal direction
With substrate direction) it is modulated by the electricity of side grid to control the width of transistor device Two-dimensional electron gas channel, while vertical
Two-dimensional electron gas is not caused to exhaust (perpendicular to grid and substrate direction) on direction and (keeps the concentration of two-dimensional electron gas and move
Shifting rate is constant).So the limitation of energy breakthrough process working ability is modulated by the electricity of bilateral grid, can both be made
Transistor device forms nano wire Two-dimensional electron gas channel, and two-dimensional electron gas can be made not influenced by dry etching damage,
Keep the high mobility of two-dimensional electron gas.Using side gate transistor structure, it will be able to the spurious mode in channel is greatly reduced,
To improve the resonance response characteristic of transistor terahertz detector.
Particular embodiments described above has carried out further in detail the purpose of the present invention, technical scheme and beneficial effects
Describe in detail bright, it should be understood that the above is only a specific embodiment of the present invention, is not intended to restrict the invention, it is all
Within the spirit and principles in the present invention, any modification, equivalent substitution, improvement and etc. done should be included in protection of the invention
Within the scope of.
Claims (10)
1. a kind of side grid field effect transistor terahertz detector characterized by comprising
Substrate;
Table top, by by growth on substrate active layer etching after formed, or by growing active layer on substrate after, etching portion
It is formed after dividing substrate and active layer;
Grid, setting are located at table top two sides, form Schottky contacts with the table top;
Source electrode and drain electrode, setting are located at the other two sides of table top, form Ohmic contact with the table top.
2. grid field effect transistor terahertz detector in side according to claim 1, it is characterised in that:
The field effect transistor comprises at least one of the following: Metal-Oxide Semiconductor field effect transistor, metal-half
Conductor field effect transistor, metal-insulatorsemiconductor field effect transistor, modulation-doped FET, junction field
Transistor and high electron mobility field-effect transistor.
3. grid field effect transistor terahertz detector in side according to claim 1, it is characterised in that:
The substrate material are as follows: gallium nitride, GaAs, phosphatization steel, diamond, sapphire, silicon carbide or silicon.
4. grid field effect transistor terahertz detector in side according to claim 1, it is characterised in that:
The table top is relative to substrate protrusion, and the table surface height is more than or equal to active layer thickness.
5. grid field effect transistor terahertz detector in side according to claim 1, it is characterised in that:
The number of the grid is 2 or 2 or more, wherein at least has 2 grids to be located at the two sides of table top.
6. the preparation method of grid field effect transistor terahertz detector in side according to claim 1, it is characterised in that:
The source electrode and drain electrode forms Ohm contact electrode, and the Ohm contact electrode connects with the side surface of the table top
Touching, or be in contact with the upper surface of the table top, or be in contact simultaneously with the side surface of the table top and upper surface.
7. the preparation method of side grid field effect transistor terahertz detector, feature exist according to claim 1 or 5
In:
The gate electrode is only in contact with the side surface of table top.
8. grid field effect transistor terahertz detector in side according to claim 1, it is characterised in that:
The material of the grid, source electrode and drain electrode comprises at least one of the following: Ti, Al, Ni, Mo, Pt, Pd, Au, W, TiW and
TiN。
9. a kind of preparation method of side grid field effect transistor terahertz detector, comprising:
On substrate by injecting, spreading or be epitaxially-formed active layer;
It etches active layer or active layer and section substrate to form table top;
Ohm contact electrode is prepared at the both ends of table top;
Gate electrode is prepared at the other both ends of table top.
10. the preparation method of grid field effect transistor terahertz detector in side according to claim 9, it is characterised in that:
The height of the table top is more than or equal to the thickness of active layer.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201811559379.4A CN109686810A (en) | 2018-12-19 | 2018-12-19 | Side grid field effect transistor terahertz detector and preparation method thereof |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201811559379.4A CN109686810A (en) | 2018-12-19 | 2018-12-19 | Side grid field effect transistor terahertz detector and preparation method thereof |
Publications (1)
Publication Number | Publication Date |
---|---|
CN109686810A true CN109686810A (en) | 2019-04-26 |
Family
ID=66186929
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201811559379.4A Pending CN109686810A (en) | 2018-12-19 | 2018-12-19 | Side grid field effect transistor terahertz detector and preparation method thereof |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN109686810A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109991766A (en) * | 2019-04-29 | 2019-07-09 | 电子科技大学 | A kind of high electron mobility transistor terahertz wave modulator loaded in waveguide |
CN112670371A (en) * | 2020-12-25 | 2021-04-16 | 中国科学院半导体研究所 | Side gate transistor terahertz detector and preparation method thereof |
CN113466166A (en) * | 2021-07-08 | 2021-10-01 | 清华大学 | Gas terahertz spectrum detection system |
RU2782707C1 (en) * | 2021-11-23 | 2022-11-01 | Общество с ограниченной ответственностью "Терагерцовые оптоэлектронные решения" | Terahertz hot electron bolometer |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104091837A (en) * | 2014-06-13 | 2014-10-08 | 南京大学 | Terahertz detector based on optical antenna |
-
2018
- 2018-12-19 CN CN201811559379.4A patent/CN109686810A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104091837A (en) * | 2014-06-13 | 2014-10-08 | 南京大学 | Terahertz detector based on optical antenna |
Non-Patent Citations (1)
Title |
---|
P. SAI 等: "AlGaN/GaN Field Effect Transistors Based on Lateral Schottky Barrier Gates as Millimeter Wave Detectors", 《2018 IEEE》 * |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN109991766A (en) * | 2019-04-29 | 2019-07-09 | 电子科技大学 | A kind of high electron mobility transistor terahertz wave modulator loaded in waveguide |
CN109991766B (en) * | 2019-04-29 | 2024-01-02 | 电子科技大学 | Terahertz wave modulator with high electron mobility transistor loaded in waveguide |
CN112670371A (en) * | 2020-12-25 | 2021-04-16 | 中国科学院半导体研究所 | Side gate transistor terahertz detector and preparation method thereof |
CN113466166A (en) * | 2021-07-08 | 2021-10-01 | 清华大学 | Gas terahertz spectrum detection system |
RU2782707C1 (en) * | 2021-11-23 | 2022-11-01 | Общество с ограниченной ответственностью "Терагерцовые оптоэлектронные решения" | Terahertz hot electron bolometer |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN109686810A (en) | Side grid field effect transistor terahertz detector and preparation method thereof | |
US6690042B2 (en) | Metal oxide semiconductor heterostructure field effect transistor | |
CN105679838B (en) | Terahertz Schottky diode based on the more channel structures of AlGaN/GaN hetero-junctions and production method | |
Egawa et al. | Characterizations of recessed gate AlGaN/GaN HEMTs on sapphire | |
CN106129166B (en) | A kind of GaN MoS2Subrane detector and preparation method thereof | |
CN101512770A (en) | P-channel nanocrystalline diamond field effect transistor | |
CN103367463B (en) | A kind of Terahertz lateral direction schottky diode and preparation method thereof | |
CN104037221B (en) | Compound field plate high-performance AlGaN/GaN HEMT element structure based on polarization effect and manufacturing method | |
CN109742142A (en) | A kind of GaN base HEMT device and preparation method thereof | |
CN109873034A (en) | Normally-off HEMT power device of deposit polycrystalline AlN and preparation method thereof | |
CN103745992B (en) | AlGaN/GaN MISHEMT high tension apparatus based on compound drain electrode and preparation method thereof | |
CN106898640A (en) | A kind of enhanced nitride field-effect transistor and preparation method thereof | |
CN104037218A (en) | High-performance AlGaN/GaN HEMT high-voltage element structure based on polarization effect and manufacturing method | |
CN115377200A (en) | Semiconductor device and preparation method thereof | |
CN107154426A (en) | A kind of device architecture and implementation method for improving silicon substrate GaN HEMT breakdown voltages | |
CN113013714B (en) | Graphene terahertz light source device and manufacturing method thereof | |
WO2019114201A1 (en) | Silicon carbide power semiconductor device having low on-resistance | |
CN104064595A (en) | Enhanced AlGaN/GaN MISHEMT device structure based on groove-gate structure and method for manufacturing same | |
CN104037215B (en) | Reinforced AlGaN/GaN MISHEMT element structure based on polymer and manufacturing method thereof | |
CN110504297B (en) | Two-dimensional material transistor based on two-dimensional electron gas regulation and control back gate, manufacturing method and application | |
Wang et al. | High performance β-Ga 2 o 3 vertical Schottky barrier diodes | |
Duan et al. | Breakdown voltage analysis of Al0. 25Ga0. 75N/GaN high electron mobility transistors with partial silicon doping in the AlGaN layer | |
CN115376919A (en) | Enhanced GaN power device and preparation method thereof | |
CN104037217A (en) | AlGaN/GaN HEMT switching element structure based on composite dipole layer and manufacturing method | |
CN107425063A (en) | The GaAs HEMT with heat to electricity conversion function of internet of things oriented |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
WD01 | Invention patent application deemed withdrawn after publication |
Application publication date: 20190426 |
|
WD01 | Invention patent application deemed withdrawn after publication |