WO2005011003A1 - Photodetector and method for the production thereof - Google Patents
Photodetector and method for the production thereof Download PDFInfo
- Publication number
- WO2005011003A1 WO2005011003A1 PCT/DE2004/001295 DE2004001295W WO2005011003A1 WO 2005011003 A1 WO2005011003 A1 WO 2005011003A1 DE 2004001295 W DE2004001295 W DE 2004001295W WO 2005011003 A1 WO2005011003 A1 WO 2005011003A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- absorption layer
- electrodes
- photodetector
- ohmic contacts
- resistance
- Prior art date
Links
- 238000004519 manufacturing process Methods 0.000 title claims abstract description 9
- 238000000034 method Methods 0.000 title claims description 12
- 238000010521 absorption reaction Methods 0.000 claims abstract description 45
- 230000005684 electric field Effects 0.000 claims abstract description 12
- 239000000758 substrate Substances 0.000 claims abstract description 12
- 239000004065 semiconductor Substances 0.000 claims description 17
- 239000002800 charge carrier Substances 0.000 claims description 12
- 238000005468 ion implantation Methods 0.000 claims description 12
- 239000000463 material Substances 0.000 claims description 11
- 238000002513 implantation Methods 0.000 claims description 6
- 239000002184 metal Substances 0.000 claims description 5
- 229910052751 metal Inorganic materials 0.000 claims description 5
- 238000000407 epitaxy Methods 0.000 claims description 3
- 150000002500 ions Chemical class 0.000 claims description 3
- 238000005275 alloying Methods 0.000 claims description 2
- 238000009792 diffusion process Methods 0.000 claims description 2
- 230000004048 modification Effects 0.000 claims description 2
- 238000012986 modification Methods 0.000 claims description 2
- 239000002019 doping agent Substances 0.000 claims 1
- 230000007704 transition Effects 0.000 claims 1
- 230000009467 reduction Effects 0.000 abstract description 2
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 6
- 229910052710 silicon Inorganic materials 0.000 description 3
- 230000001133 acceleration Effects 0.000 description 2
- 238000009826 distribution Methods 0.000 description 2
- 238000005530 etching Methods 0.000 description 2
- 239000012535 impurity Substances 0.000 description 2
- 230000008569 process Effects 0.000 description 2
- 238000005215 recombination Methods 0.000 description 2
- 230000006798 recombination Effects 0.000 description 2
- 230000004044 response Effects 0.000 description 2
- 239000010703 silicon Substances 0.000 description 2
- 241000589614 Pseudomonas stutzeri Species 0.000 description 1
- 239000006096 absorbing agent Substances 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 238000001459 lithography Methods 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 230000003287 optical effect 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 at least one potential-jump barrier or surface barrier, e.g. phototransistors
- H01L31/101—Devices sensitive to infrared, visible or ultraviolet radiation
- H01L31/102—Devices sensitive to infrared, visible or ultraviolet radiation characterised by only one potential barrier or surface barrier
- H01L31/108—Devices sensitive to infrared, visible or ultraviolet radiation characterised by only one potential barrier or surface barrier the potential barrier being of the Schottky type
- H01L31/1085—Devices sensitive to infrared, visible or ultraviolet radiation characterised by only one potential barrier or surface barrier the potential barrier being of the Schottky type the devices being of the Metal-Semiconductor-Metal [MSM] Schottky barrier type
-
- 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
- H01L31/09—Devices sensitive to infrared, visible or ultraviolet radiation
Definitions
- the invention relates to a photodetector and a method for its production.
- Photodetectors are used to convert light signals into electrical signals and z. B. used in optical communication.
- a photodetector known from the prior art consists of two metal contacts on the surface of a semiconductor. With this so-called MSM photodetector (MSM: Metal-Semiconductor-Metal), the
- Electrodes z. B. be designed as Schottky contacts. Then the component works as a photodiode with two anti-serial Schottky diodes. However, if the electrodes are designed as ohmic contacts, a photoresistor is obtained.
- MSM photodetectors are manufactured according to the state of the art on all common semiconductor materials, e.g. B. on Si, GaAs, InP, GaN, both with Schottky contacts and as photoresistors.
- Materials with a high density of recombination centers are particularly suitable for the production of ultrafast photoresistors, which greatly reduce the lifespan of the photogenerated charge carriers.
- One example is the so-called low temperature grown GaAs (LT-GaAs), which is produced at low temperatures of eg 200 ° C for epitaxial conditions.
- Ion implantation is also used to isolate electrical components by greatly reducing the conductivity in the areas between the components.
- a further disadvantage is that the field peaks generated by the inhomogeneous field distribution lead to a reduced dielectric strength of the detector.
- the MSM photodetector is designed as a photoresistor, the requirement for a high electrical resistance of the semiconductor in order to achieve the lowest possible dark current contradicts Desire for a low contact resistance of the electrodes, which requires the lowest possible resistance of the semiconductor material.
- the object of the invention is to provide a photodetector with a high electrical resistance of the semiconductor to achieve the lowest possible dark current, which has a low contact resistance of the electrodes with the lowest possible resistance of the semiconductor material.
- the photodetector comprises an absorption layer and at least two electrodes designed as ohmic contacts on and / or in the absorption layer.
- the specific resistance of the absorption layer in the area between the electrodes is greater than one in relation to the specific resistance of the absorption layer in the immediate area at the electrodes.
- the ratio is advantageously at least 10.
- the specific resistance between the electrodes can be, for example, in the megohm or gigaohm range, the resistance in the immediate range of the electrodes in the ohm or kiloohm range.
- the absorption layer has between the electrodes thus a comparatively high resistance.
- the absorption layer has a lower resistance.
- the specific resistance of the absorption layer between the electrodes or in the immediate area at the electrodes is set in such a way that a homogeneous electric field is present between the electrodes.
- a high resistance of the absorption layer in the area between the contacts creates a homogeneous electric field there, which is aligned essentially parallel to the surface when an electrical voltage is present between the contacts. This suppresses the reduction in the speed of the detector by generating charge carriers in low-field areas and avoids field peaks that lead to breakdown even at low applied voltages.
- the electrodes in the absorption layer, provided that a lower resistance than in the area between the electrodes can then be set towards the surface of the absorption layer or towards the substrate.
- the two electrodes are usually n- or p-doped for better contactability
- Semiconductor layer arranged as an absorption layer.
- the area between the contacts is provided with so many impurities that the ohmic resistance is greatly increased and photogenerated charge carriers quickly recombine.
- the absorption layer below the contact is highly conductive.
- absorption layer and electrodes is advantageously arranged on an insulating or semi-insulating substrate as a base layer.
- Such photodetectors thus represent semiconductor-based components for converting light into electrical current.
- the light penetrates into the component from above, essentially perpendicular to the substrate surface.
- the process for producing the photodetector comprises the steps:
- the absorption layer can be modified by implantation or by diffusion with suitable ions.
- the ion implantation is then carried out with a dose and energy which is sufficient to increase the resistance of the absorption layer in the region between the electrodes from its surface to the substrate.
- the material of the absorption layer between the electrodes is changed so that the speed of the photodetector is increased overall by the creation of recombination centers and the service life of the photo-generated charge carriers is reduced.
- the ion implantation is carried out with suitable elements, such as. B. nitrogen or silicon, which greatly increase the ohmic resistance between the electrodes, so that photogenerated charge carriers recombine faster.
- the contacting of the photodetector takes place, for. B. by means of insulation layers, contact pads and so on.
- a photodetector has the known advantages of the MSM components. It is a pla- nares component, which means that no etching is required, which saves work steps and simplifies subsequent production steps, in particular the lithography.
- the conductivity of the semiconductor material below the ohmic contacts can be chosen regardless of the dark current of the photodetector.
- the ion implantation procedure is self-adjusting only in the areas outside the ohmic contacts, because the contact material itself acts as an implantation mask. This saves expensive lithographic processing steps and allows smaller dimensions between the electrodes because no adjustment tolerances have to be planned.
- Figure 1 shows a photodetector according to the prior art.
- Figure 2 shows a photodetector according to the invention.
- FIG. 3 shows a method according to the invention for producing the photodetector.
- FIG. 1 when an electrical voltage is applied between the electrodes 1, an electrical field 3 is generated in the semiconductor.
- This field 3 moves photogenerated charge carriers and thus generates a photocurrent.
- the electric field is disadvantageously inhomogeneous, that is to say it becomes weaker with increasing depth in the semiconductor, as shown in FIG. 1 in relation to the prior art. Because the speed of the photogenerated charge carriers depends on the electric field strength, the photogenerated charge carriers in the depth disadvantageously increase the response time of the detector.
- a further disadvantage is that the field peaks generated by the inhomogeneous field distribution lead to a reduced dielectric strength of the detector.
- FIG. 2 shows an MSM photoresistor based on GaAs according to the invention with a wavelength to be detected of less than 910 nanometers.
- the substrate 24 is made of semi-insulating GaAs.
- the absorption layer 22 consists of GaAs and has a thickness of, for example, 0.1 to 10 micrometers. In the present example, photons with a wavelength of 850 nanometers penetrate GaAs up to 1 micron deep into the absorption layer 22.
- the absorption layer 22 is thus of the n-type.
- the electrodes 21 comprise a metallic layer sequence made of Ni / AuGe / Ni with respective thicknesses of 5, 90 and 25 nanometers. If necessary, the electrodes can be reinforced with an additional metal layer (e.g. gold) with a thickness of 50 to 500 nanometers for better shielding during ion implantation.
- the electrodes 21 have a length of 100 nanometers to 20 micrometers and a distance of 100 nanometers to 20 micrometers.
- FIG. 2 shows a 2-finger layout with respect to the electrodes 21. However, an interdigital multifinger layout can also be implemented.
- the first step is to produce a conductive absorption layer 32 on an insulating or semi-insulating semiconductor material as substrate 34, e.g. B. by epitaxy or by ion implantation.
- electrodes 31 are produced as ohmic contacts on the conductive layer 32, e.g. B. by applying suitable metal layers and alloying ( Figure 3b).
- the implantation process which is indicated by arrows in FIG. 3c, runs in a self-adjusting manner only in the areas between the contacts 31. If necessary, the ohmic contacts 31 can be strengthened by applying suitable materials.
- the ion implantation is carried out with N, Ar, 0, H, He, Si or another suitable element.
- the acceleration voltage is, for example, 10 kV to 10 MV.
- the dose is, for example, 10 12 to 10 18 cm “2 .
- the high-resistance absorption layer is first generated by epitaxy or by ion implantation on a suitable substrate.
- the low-resistance areas below the ohmic contacts still to be produced are then produced by means of ion implantation.
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Electromagnetism (AREA)
- General Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Computer Hardware Design (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Light Receiving Elements (AREA)
Abstract
Description
Claims
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE112004001156T DE112004001156B4 (en) | 2003-07-24 | 2004-06-19 | Method for producing a photodetector |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
DE2003133669 DE10333669A1 (en) | 2003-07-24 | 2003-07-24 | Photodetector and method for its production |
DE10333669.9 | 2003-07-24 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2005011003A1 true WO2005011003A1 (en) | 2005-02-03 |
Family
ID=34088787
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/DE2004/001295 WO2005011003A1 (en) | 2003-07-24 | 2004-06-19 | Photodetector and method for the production thereof |
Country Status (2)
Country | Link |
---|---|
DE (2) | DE10333669A1 (en) |
WO (1) | WO2005011003A1 (en) |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN107546283B (en) * | 2017-08-29 | 2019-03-19 | 重庆大学 | The GaN ultraviolet photoelectric detection sensor and its application circuit module of buried type electrode |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4998154A (en) * | 1990-01-18 | 1991-03-05 | Northern Telecom Limited | MSM photodetector with superlattice |
EP0651448A1 (en) * | 1993-10-28 | 1995-05-03 | Hitachi Europe Limited | Improved metal-semiconductor-metal photodetector |
DE19846063A1 (en) * | 1998-10-07 | 2000-04-20 | Forschungszentrum Juelich Gmbh | Method of manufacturing a double-gate MOSFET |
WO2000041456A2 (en) * | 1999-01-12 | 2000-07-20 | Forschungszentrum Jülich GmbH | Optical detector with a filter layer made of porous silicon and method for the production thereof |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6194382A (en) * | 1984-10-09 | 1986-05-13 | ゼロツクス コーポレーシヨン | 2-terminal thin film photodetector |
DE19621965A1 (en) * | 1996-05-31 | 1997-12-04 | Forschungszentrum Juelich Gmbh | Semiconductor photo-detector converting light into electric current |
-
2003
- 2003-07-24 DE DE2003133669 patent/DE10333669A1/en not_active Withdrawn
-
2004
- 2004-06-19 WO PCT/DE2004/001295 patent/WO2005011003A1/en active Application Filing
- 2004-06-19 DE DE112004001156T patent/DE112004001156B4/en not_active Expired - Fee Related
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4998154A (en) * | 1990-01-18 | 1991-03-05 | Northern Telecom Limited | MSM photodetector with superlattice |
EP0651448A1 (en) * | 1993-10-28 | 1995-05-03 | Hitachi Europe Limited | Improved metal-semiconductor-metal photodetector |
DE19846063A1 (en) * | 1998-10-07 | 2000-04-20 | Forschungszentrum Juelich Gmbh | Method of manufacturing a double-gate MOSFET |
WO2000041456A2 (en) * | 1999-01-12 | 2000-07-20 | Forschungszentrum Jülich GmbH | Optical detector with a filter layer made of porous silicon and method for the production thereof |
Also Published As
Publication number | Publication date |
---|---|
DE10333669A1 (en) | 2005-03-03 |
DE112004001156D2 (en) | 2006-03-23 |
DE112004001156B4 (en) | 2009-01-08 |
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