GB2071415A - Schottky Barrier Photovoltaic Detector and Process - Google Patents

Schottky Barrier Photovoltaic Detector and Process Download PDF

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GB2071415A
GB2071415A GB8105367A GB8105367A GB2071415A GB 2071415 A GB2071415 A GB 2071415A GB 8105367 A GB8105367 A GB 8105367A GB 8105367 A GB8105367 A GB 8105367A GB 2071415 A GB2071415 A GB 2071415A
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layer
approximately
barrier
gold
substrate
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General Dynamics Corp
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor 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
    • H01L31/04Semiconductor 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 adapted as photovoltaic [PV] conversion devices
    • H01L31/06Semiconductor 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 adapted as photovoltaic [PV] conversion devices characterised by potential barriers
    • H01L31/07Semiconductor 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 adapted as photovoltaic [PV] conversion devices characterised by potential barriers the potential barriers being only of the Schottky type
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor 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
    • H01L31/02Details
    • H01L31/0216Coatings
    • H01L31/02161Coatings for devices characterised by at least one potential jump barrier or surface barrier
    • H01L31/02162Coatings for devices characterised by at least one potential jump barrier or surface barrier for filtering or shielding light, e.g. multicolour filters for photodetectors
    • H01L31/02164Coatings for devices characterised by at least one potential jump barrier or surface barrier for filtering or shielding light, e.g. multicolour filters for photodetectors for shielding light, e.g. light blocking layers, cold shields for infrared detectors
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor 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
    • H01L31/08Semiconductor 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
    • H01L31/10Semiconductor 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
    • H01L31/101Devices sensitive to infrared, visible or ultraviolet radiation
    • H01L31/102Devices sensitive to infrared, visible or ultraviolet radiation characterised by only one potential barrier
    • H01L31/108Devices sensitive to infrared, visible or ultraviolet radiation characterised by only one potential barrier the potential barrier being of the Schottky type
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy

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  • 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

A platinum-cadmium sulfide Schottky barrier photovoltaic UV/IR detector is fabricated with both the ohmic and barrier contacts 70, 72 located on the same side of the cadmium sulfide substrate 30 to facilitate wire attachment by high- speed bonding techniques. A titanium-gold-titanium infrared shield structure 32 is deposited directly on the substrate and is utilized to provide a connection between the ohmic contact and the substrate. An insulating layer 34 of silicon dioxide covers the shield structure. A thin layer 36 of platinum is deposited directly on the substrate in a small central optically active area surrounded by the insulated shield structure. A metal boundary layer 42A overlies the periphery of the platinum layer and prevents the barrier contact metalization from affecting the properties of the Schottky barrier. Both the ohmic and barrier contacts 70, 72 may be formed of a titanium adhesion layer and a layer of gold. <IMAGE>

Description

SPECIFICATION Schottky Barrier Photovoltaic Detector and Process The present invention relates to solid state radiation detectors and processes of manufacturing the same. More particularly, the present invention relates to an improved platinum-cadmium sulfide Schottky barrier photovoltaic detector and process of fabrication.
There exists a demand in high technology optical systems, such as in the optical guidance systems for radiation seeking missiles, for a high quantum efficiency, short-time response, solid state radiation detector. In these systems, such a detector must have a high response to near ultraviolet (UV) radiation, but must be sustantially insensitive to radiation in the visible spectrum.
Silicon photodiodes have been proposed for these applications. However, such photodiodes are sensitive to the visible spectrum through approximately 8000 angstroms, and therefore they must be used in association with optical filtering to remove the visible radiation.
Additionally, these detector-filter combinations have a relatively low quantum efficiency, e.g. 30% or less.
Cadmium sulfide based solid state radiation detectors have been utilized; however, the known characteristics of cadmium sulfide detectors suggest that they are useful primarily in visible range, and that they are relatively insensitive to ultraviolet radiation. It is desirable to provide a solid state radiation detector sensitive to near ultraviolet and short wavelength visible radiation and transparent to infrared radiation. This is particularly true if such a detector can be fabricated to have a high quantum efficiency and a relatively small optically active area so that it may be utilized in conjunction with the high resolution optics.Good infrared (IR) transmission characteristics enable the detector to be utilized in association with an IR sensor to produce a coaxial transducer suitable for use in association with unfiltered, high-resolution optics Recently cadmium sulfide base Schottky barrier diodes have been proposed as radiation detectors. Broadly speaking, a Schottky barrier diode is a junction diode in which the junction is formed between a semiconductor material and a metal contact, rather than between dissimilar semiconductor materials or carrier types, as in the case of an ordinary PM diode. Disclosed in the prior art is a platinum-cadmium sulfide Schottky barrier photovoltaic detector fabricated with the ohmic and barrier contacts located on the opposite sides of the cadmium sulfide substrate.
This prior art detector exhibits high quantum efficiency in the UV spectrum with good IR transmission characteristics.
The improved detector of the present invention is more amenable to production fabrication and quantity assembly techniques than the prior art detector. Rather than having ohmic and barrier contact connections on opposite sides of the device, the new detector is fabricated with both contacts on the front face. Organic insulating layers made of photoresist have been replaced by a hard, inorganic insulating layer. Furthermore, the copper and indium metalizations have been replaced with gold, titanium, nichrome and other metallizations. These improvements facilitate wire attachment by high-speed bonding techniques which are more reliable and which reduce the time and effort necessary for forming electrical contacts on the device. Furthermore, the overall reliability of the device is enhanced.The manufacturing process results in a compensated layer at the surface of the cadmium sulfide substrate which protects the device when excessive voltage is applied to it.
The present invention provides s Schottky barrier photovoltaic detector suitable for detecting ultraviolet and infrared radiation comprising: a cadmium sulfide substrate having upper and lower surfaces; an infrared shield structure overlying the upper surface of the substrate, including a layer of material which is substantially opaque to infrared radiation, the shield structure being delineated to provide a first central window therein; an insulating layer covering the infrared shield structure and having a second central window and a side window therein, the second central window being coincident with and slightly smaller than the first central window; a Schottky barrier metallization layer positioned within the second central window and completely covering the portion of the substrate which is located therein, the Schottky barrier metallization layer being sufficiently thin so that it is substantially transparent to ultraviolet and infrared radiation; means positioned above the upper surface of the substrate for providing a barrier contact extending through the second central window and leaving a major portion of the Schottky barrier metallization layer exposed; and means positioned above the upper surface of the substrate for providing an ohmic contact extending through the side window.
The present invention also provides a process of fabricating a Schottky barrier photovoltaic detector comprising the steps of: slicing a wafer from a single crystalline cadmium sulfide ingot, the wafer having upper and lower substantially parallel pianar surfaces which are perpendicular to the C-axis of the hexagonal crystal of the cadmium sulfide; lapping, polishing, and etching the upper surface of the wafer to produce a substrate having a smooth upper surface and a lower surface; depositing and delineating an infrared shield structure on the upper surface of the substrate, including a layer of a material which is substantially opaque to infrared radiation, the shield structure having a first central window therein; depositing and delineating an insulating layer over the infrared shield structure, the insulating layer having a second central window and a side window therein, the second central window being coincident with and slightly smaller than the first central window; depositing and delineating a Schottky barrier metallization layer within the second central window so that it completely covers the portion of the substrate which is located therein, the Schottky barrier metallization layer being sufficiently thin so that it is substantially transparent to ultraviolet and infrared radiation; and depositing and delineating barrier and ohmic contacts which extend above the upper surface of the substrate through the second central window and the side window, respectively, the barrier contact leaving a major portion of the Schottky barrier metallization layer exposed.
According to one embodiment of the present invention, an infrared shield structure is first formed on the top surface of a polished, damaged-free cadmium sulfide substrate. It is preferably composed of a layer of gold (approximately 1500 angstroms thick) which is opaque to infrared radiation, sandwiched between two thin layers of titanium (approximately 300 angstroms thick). The titanium layers serve as bonding agents. The infrared shield structure is delineated in a generally square pattern leaving exposed a small central portion of the substrate which forms the optically active area. A relatively thick layer of silicon dioxide (preferably approximely 5000 angstroms thick) covers the infrared shield structure to prevent the shortening of subsequent layers deposited thereon.Two windows are etched in the silicon dioxide insulating layer, one coinciding with the central optically active area of the substrate, and the other to the side of this area which later receives the ohmic contact.
The Schottky barrier metallization is preferably a very thin layer of platinum deposited directly on the substrate and which completely fills the central window in the silicon dioxide layer. A boundary layer preferably made of a metal such as tungsten nichrome or gold overlies the periphery of the platinum layer and prevents the barrier contact metallization from affecting the properties of the Schottky barrier.
The barrier contact metallization is preferably composed of a titanium adhesion layer and a layer of gold. The thickness of the gold layer is increased to approximately 30,000 angstroms by electroplating. The ohmic contact is formed at the same time as the barrier contact. The second window, etched in the silicon dioxide layer at the same time as the central window, allows the ohmic contact metallization to touch the infrared shield structure. The infrared shield structure in turn makes ohmic contact to the cadmium sulfide substrate by virtue of its lower titanium adhesion layer. Gold lead wires are bonded to the top surfaces of the gold portions of the ohmic and barrier contacts by thermo-compression or thermosonic bonding.
Figures 1-9 are a series of vertical cross sectional views illustrating the various stages of construction of a UV detector in accordance with a first embodiment of the present invention; Figures 1 OA and lOB are vertical cross sectional and top planar views respectively of the completed UV detector constructed as shown in Figures 1-9. These views also illustrate the manner of attachment of the gold lead wires to the barrier and ohmic contacts; Figure 11 is a vertical cross sectional view of a UV/IR detector sandwich constructed in accordance with a second embodiment of the present invention;; Figures 12-1 9 are a series of vertical cross sectional views which together with Figures 1 and 2 show the various stages of construction of a UV detector in accordance with a third embodiment, of the present invention; and Figure 20 is a vertical cross sectional view of the completed UV detector constructed in accordance with Figures 1,2, and 12-1 9. This view shows the gold lead wires attached to the ohmic and barrier contacts.
A first embodiment of the present invention is shown in various stages of construction in Figures 1~9,1 OA and 1 OB. The overall configuration of the detector is best seen in Figure 1 OB. It includes a flat square of cadmium sulfide substrate 30 having a small square shaped infrared shield structure 32 deposited directly thereon and having an outer perimeter indicated in phantom lines. An insulating layer 34 of silicon dioxide covers the IR shield structure. A thin Schottky barrrier metal layer 36 is deposited directly onto the cadmium sulfide substrate in a central optically active area surrounded by the insulated IR shield structure.Ohmic and barrier contacts 38 and 40 respectively touch the IR shield structure and a boundary layer ring 42a (Figure 1 OA) overlying the periphery of the layer 36 through separate windows in the silicon dioxide insulating layer. As shown in Figures 1 OA and 1 OB, the barrier contact 40 has a substantially cyclindrical configuration. It extends within the central window of the insulating layer, leaving a major portion of the Schottky layer 36 exposed. A pair of lands 44 extend from opposite sides of the ring.
Gold wire leads 46 and 48 are attached to the ohmic and barrier contacts 38 and 40, respectively, the lead 48 being attached to one of the lands 44 of the barrier contact.
It should be born in mind that the detector illustrated in Figures 10A and 10B is a microelectronic device. By way of example, the insulating layer 34 may measure 0.038 inches on a side and the uncovered portion of the Schottky barrier metal layer 36 may have a diameter measuring 0.004 inches. Throughout the figures the relative dimensions of the various layers are distorted in order to facilitate an easier understanding of the structure of the embodiments shown. Also in Figures 2-9 and 12-19, elevations of the various layers have not been indicated in the central window for the sake of clarity.
Turning now to Figures 1-9 and 1 OA, the monolithic architecture of the first embodiment and the process by which it is formed will now be described in detail. It will be understood that a plurality of the detectors are simultaneously produced on a single semiconductor wafer in a suitable array such as 5x5 matrix. A wafer of suitable thickness, e.g. 1 millimeter, is sliced from a single crystalline cadmium sulfide ingot such as is available from Eagle-Picher or Cleveland Crystals Company.Such material is designated as being of the N-type with a resistivity of 1-20 ohm-cm, a barrier concentration of 1015 - 1015 cm-3, and a carrier mobility of at least 200 cm2 ~v~' sec#1.The preferred orientation of slicing the wafer is such that the c-axis of fhe hexagonal crystal is perpendicular to the surface of the wafer as shown in Figure 1. The wafer forms the cadmium sulfide substrate 30 of the detector.
Hereafter the reference numeral 30 will be used interchangeably to refer to the wafer and the substrate. The wafer is etched in a solution of hydrochloric acid to identify the positive and negative orientation sides of the wafer, i.e. the su Ifer-rich and cadmium-rich sides respectively (see Figure 1).
The wafer 30 is mounted on a work fixture and lapped flat to a suitable thickness, for example approximately .020 to approximately .030 inches.
The thickness of the cadmium sulfide substrate 30, i.e. the thickness of the wafer, can be varied considerably beyond this range without affecting the photovoltaic characteristics of the detector. In order to accomplish the lapping, the wafer may be mounted on a lapping holder and placed on a conventional rotating steel lapping plate. A lapping slurry, such as 5 micron alumina powder in MICRO OIL No, 1, may be applied every 30 seconds. The wafer can be lapped on both sides to obtain parallel surfaces, and lapping continues until the desired thickness is obtained.
Following the lapping operation, the wafer is polished using a felt-type polishing cloth on a rotating wheel. Initial polishing is performed with a 1 micron diamond polishing compound, followed by a final polishing with 1/4 micron polishing compound. Preferably, the work fixture utilized to perform the polishing is cleaned between polishing operations to prevent contamination by the previously used abrasive. It will be understood that the various layers of the detector are deposited only on the upper surface thereof. The lower surface lapping and polishing operations therefore need not be performed.
The final wafer preparation involves the use of an etch-polish which removes non-single-crystal cadmium sulfide from the upper surface of the wafer and gives this surface a smooth, mirror-like finish which is essentially free of damage. A wheel with sidewalls is employed to retain an etch-polish solution whose active ingredient is nitric acid or hydrochloric acid. After etchpolishing the wafer is rinsed, cleaned and dried.
After the wafer 30 has been prepared, it is mounted on a carrier, which is typically a glass slide measuring 1 xl x0.032 inches in order to facilitate handling. The glass slide carrying the wafer is placed in a conventional vacuum deposition apparatus. Hereafter, the discussion will center around the formation of a single detector on top of the cadmium sulfide wafer, it being understood that a plurality of such detectors are simultaneously formed at various spaced apart locations on top of the wafer.
In the vacuum deposition apparatus, various layers of material are deposited on top of the cadmium sulfide substrate 30 in order to form the infrared shield structure 32 (Figure 2). The deposition temperature may range from approximately 200C to approximately 2750C depending upon the type of metal being deposited. The infrared shield structure is formed on the upper surface of the cadmium sulfide substrate which is chosen so that it is the cadmium-rich side of the wafer. Preferably, the infrared shield structure is composed of a layer 50 of gold which is opaque to infrared radiation, sandwiched between two thin layers 52 of an adhesion metal. The layer of gold may be approximately 500 angstroms to approximately 10,000 angstroms thick. Preferably, when the layer 50 is made of gold, it is approximately 1,500 angstroms thick.The adhesion metal is preferably-titanium but it also may be aluminum, magnesium, zirconium, hafnium, or alloys of various combinations thereof. Preferably, the layer of gold is sandwiched between two relatively thin layers of titanium which may each measure approximately 50 angstroms to approximagely 5,000 angstroms of thickness, and which preferably each measure 300 angstroms in thickness.
Conventional photolithographic techniques are employed so that the three layers of metal which comprise the infrared shield structure have an identical square shape and a central, round window 54 (Figure 2) which will be the optically active region through which the infrared radiation can pass.
After the delineation of the infrared shield structure, the wafer is placed in a sputtering apparatus and a layer of silicon dioxide is deposited in order to form the insulating layer 34 (Figure 3). One suitable sputtering apparatus is manufactured by Balzer's high Vacuum Company.
The silicon dioxide insulating layer covers the infrared shield structure and may have a thickness of approximately 500 to approximately 20,000 angstroms, and preferably has a thickness of approximately 5,000 angstroms.
Conventional photolithographic techniques are employed in order to obtain the desired insulating layer pattern. The insulating layer 34 (Figure 1 OB) is generally square shaped, and has first and second windows therethrough. The first window 56 (Figure 3) corresponds in location and overall shape to the first window 54 (Figure 2) formed in the infrared shield structure 32, except that the window 56 is slightly smaller. In other words, the second central window 56 is coincident with and slightly smaller than, the first central window 54.
Both have a round configuration. It will be noted that in Figures 2 and 3 the insulating layer 34 overlaps the inner edges of the infrared shield structure defining the window 54 and contacts the cadmium sulfide substrate 30. The second window 58 (Figure 3) formed in the insulating layer 34 is spaced from the first window and receives the ohmic contact 38 (Figure 1 OB) as later described. Etching the insulating layer 34 to obtain the window 58 results in the removal of a small portion of the upper one of the layers 52.
Sputtering causes damage to the upper surface of the cadmium sulfide substrate which can adversely affect the performance of the detector.
This damage is removed by annealing the wafer at a suitable temperature for a predetermined time period, for example, 1 5 minutes at a temperature of approximately 2750C.
After annealing, a thin layer of photoresist is employed as a lift-off mask 60 (Figure 4) for the Schottky barrier metallization. This lift-off mask covers the wafer except for the central window 56 and the inner shoulder 62 of the insulating layer 34. To form the lift-off mask, a photoresist layer may be deposited over the entire surface of the wafer. This layer is then masked in the regions where the photoresist is to remain and the central portion is exposed to ultraviolet light. The exposed photoresistive material is then developed and chemically dissolved away leaving the central window 56 and the shoulder 62 exposed.
After the formation of the lift-off mask, the wafer is placed in a conventional vacuum apparatus where two metallization layers are deposited over the entire surface of the wafer (not shown) by electron beam evaporation. The photoresist lift-off mask 60 is then dissolved by spraying a jet of acetone on the wafer surface.
This also removes the two metallization layers except in the central window of the photoresist lift-off mask as shown in Figure 5. In that Figure, the lower of these two metallization layers, a portion of which lies directly on top of the substrate 30, is the Schottky barrier metallization layer 36. The upper one of these two layers is the boundary layer 42. It is important that the entire exposed area of the substrate in the window 56 (Figure 4) be covered by the layer 36. Therefore, the lift-off mask is delineated to leave both the window 56 and the shoulder 62 uncovered. This results in the formation of a pair of ring shaped layers 36' and 42' (Figure 5) on top of the shoulder 62.As hereafter explained the central portion of the boundary layer 42 is etched away and the periphery thereof (42a in Figure 9) remains to prevent the barrier contact metullization from affecting the properties of the Schottky barrier formed at the junction between the metal layer 36 and the cadmium sulfide substrate 30.
The Schottky barrier metal layer 36 may be made of platinum, gold, iridium, or alloys of various combinations thereof. Preferably the layer 36 is made of platinum. The layer 36 must be sufficiently thin to be substantially transparent to both UV and IR radiation.
For example, where the layer 36 is made of platinum it may have a thickness of approximately 5 angstroms to approximately 50 angstroms, and preferably 1 5 angstroms. The depth of the platinum is controlled to be within plus or minus 5 angstroms as determined by measurement with a Talystep I profilometer.
The boundary layer 42 may be made of gold, tungsten, nichrome, iridium, rehenium, paiadium, rhodium, or alloys of various combinations of these. Preferably the layer 42 is made of gold and has a thickness of approximately 100 to approximately 300 angstroms. The layers 36 and 42 cannot both be made of the same metal in any case.
Next the wafer 30 is again placed in the vacuum apparatus where it is heated to a suitable temperature between approximately 200C to approximately 2350C, depending upon the type of ohmic and barrier contact metallization that will be utilized. Preferably the wafer is heated to approximately 1 750C. Thereafter, approximately 50 angstroms to approximately 5000 angstroms, and preferably approximately 300 angstroms of contact adhesion layer 66 (Figure 6) are deposited over the entire surface of the wafer.
Preferably this contact adhesion layer is made of titanium, although nichrome, chromium or tungsten can also be utilized. While still in the vacuum apparatus, a contact metallization layer 68 (Figure 6) is deposited over the just deposited contact adhesion layer. This contact metallization layer may be made of gold or aluminum.
Preferably the contact metallization layer 68 is made of gold and has a thickness of approximately 1000 to approximately 2000 angstroms.
The wafer is removed from the vacuum apparatus and it is coated over its entire surface with a layer of photoresist (not shown). A suitable reverse image is made in this photoresist layer so that a pair of contact pads 70 and 72 (Figure 7) can be electroplated onto the wafer to complete the ohmic and barrier contacts 38 and 40, respectively, as shown.
The pad 70 completely fills the side window 58 and it has surfaces which are bonded to a pair of stepped layer portions 68a and 68b of the contact metallization layer 68. The pad 72 has a lower cyclindrical portion positioned within the central window 36 surfaces which are bonded to a pair of stepped layer portions 68c and 68d of the layer 68.
The pads 70 and 72 are made of the same type of metal as the contact metallization layer 68.
Preferably they are made of gold which is built up by electroplating until the combined thickness of the pad 70 and the layer portion 68a or of the pad 72 and the layer portion 68c is approximately 50,000 angstroms.
After the aforementioned electroplating, the photoresist is removed and the portions of the contact metallization layer 66 which are not underneath the electroplated pads 70 and 72 are etched away as shown in Figure 8. Next the portions of the contact adhesion layer 66 which are not underneath the pads 70 and 72 are etched away as shown in Figure 9. This leaves the ohmic and barrier contacts 38 and 40 isolated from each other. Thus, viewing Figures 8 and 9 together, it can be seen that the completed ohmic contact 38 consists of the layer portions 66a, 66b, 68a and 68b and the pad 70. Likewise the completad barrier contact 40 consists of the layer portions 66c, 66d, 68c and 68d and the pad 72.
Finally, the portion of the boundary layer 42 (Figure 8) which is not beneath the pad 72 is etched away to expose the Schottky barrier metal layer 36 as shown in Figure 9. The remaining boundary layer ring 42a (Figure 9) of the boundary layer overlies the periphery of the Schottky layer 36. It prevents the contact adhesion layer portion 66c which is preferably titanium, from affecting the properties of the Schottky barrier formed between the layer 36 and the cadmium sulfide substrate 30. The boundary layer ring 42a is not absolutely necessary and may be eliminated where the contact adhesion layer 66 is made of a metal that will not form an ohmic type contact between the layer 66c and the Schottky barrier metal layer 36.
Next the wafer is mounted face down on a work fixture suitable for lapping so that the unprocessed lower surface of the wafer is facing upwardly. It is necessary to prevent damage to the various layers of material that have been deposited on the upper surface of the wafer.
Therefore, a quantity of wax is applied to the work fixture to prevent the detector from contacting the metal portions of the lapping fixture. The lower side of the wafer is lapped to a suitable thickness, such as 0.006 inches and the lower surface is polished as previously described in conjunction with the lapping and polishing of the upper surface. It will be understood that the lower surface lapping and polishing operations are necessary only where layers are to be deposited on the same, for example, in the formation of ohmic contacts on the lower surfaces of the cadmium sulfide substrate, or when the device is to be used in a sandwich-type detector.
Furthermore, the final thickness of the substrate is not critical. It's ultimate thickness is limited only in the sense that it is desired to have the finished detector configured in the form of a relatively flat chip.
After the lower surface of the wafer has been lapped and polished, the wafer is demounted from the work fixture, cleaned and dried. Suitable cleaning and drying steps are disclosed in U.S.
Patent No. 4,000,502. The detector is checked for pinholes in the infrared shield structure 32.
The existence of such pinholes is undesirable since they allow extraneous radiation through the cadmium sulfide substrate at locations other than the central window 56. This will interfere with the proper operation of an infrared sensor positioned below the cadmium sulfide substrate when the detector is used in a UV/IR sandwiched configuration.
The wafer is mounted onto a pedestal and it is diced into individual detectors using a suitable saw and abrasive slurry. One suitable saw in manufactured by South Bay Technology. It incorporates a blade having a diameter measuring approximately 0.005 inches. The abrasive slurry may consist of 5 micron alumina powder in glycerol and water.
Finally, the gold wire leads 46 and 48 (Figure 1 OA) are attached to the ohmic and barrier contacts 36 and 40, respectively, by thermocompression or thermosonic bonding.
Apparatuses are commercially available for attaching the leads in this manner at high speed, and this high speed bonding is facilitated by having both the ohmic and barrier contacts on the same side of the substrate. No conductive epoxy need be applied to affix leads to the respective contacts. The thermo-compression bonding technique results in the formation of mushroomlike lobes 74 at the ends of the wires which are firmly bonded to the gold contact pads 70 and 72, assuming gold has been utilized as the contact metallization. In Figure 10A, the elevations of the layers 42a, 66c and 68c surrounding the central window 56 are depicted.
The foregoing process by which the various layers of the detector are built up results in the formation of a compensated layer 76 (Figure 1 OA) adjacent the upper surface of the substrate 30. Its lower planar boundary is indicated by the phantom line in Figure 1 or. This compensated layer forms an avalanche region which protects the detector when excessive voltage is applied to it. This may occur when static electricity discharges from a person into the device through attached contacts such as probes, headers, etc.
An unprotected detector can develop a potential difference of hundreds of volts across the insulating layer 34. Such a voltage potential can induce dielectric breal < down in the insulating layer which can cause permanent damage to the detector. The compensated layer 76 allows the electric field within the cadmium sulfide substrate to build up faster than it does in the insulating layer. When the electric field in the cadmium sulfide substrate exceeds a certain threshold level, a conductor path within the semiconductor substrate is formed by virtue of an avalanche effect. When the potential voltage is discharged, the current flow ceases and no permanent damage results to the detector.
Figure 11 depicts a second embodiment of the present invention in the form of a UV/lR detector sandwich. The upper portion of this detector is the first embodiment of the UV detector of Figure 1 OA and 1 OB just described. The lower portion of this UV/lR detector is an IR sensor 78 in the form of a suitable P-N junction photovoltaic diode.
One suitable diode uses indium antimonide semiconductor materials. Preferably, the IR sensor 78 is spaced closely adjacent to the lower surface of the UV detector. In other words, the P and N semiconductor materials which form the IR sensor are not directly bonded to the lower surface of the cadmium sulfide substrate of the UV detector. The infrared shield structure 32 of the UV detector preferably extends beyond the side edges of the IR sensor 78 so that this sensor receives IR radiation only through the central window 56 of the UV detector.
Silicon dioxide has been known to exhibit poor bonding characteristics in conjunction with some cadmium sulfide surfaces. The third embodiment of the present invention represented by Figures 12-20 overcomes this problem and thereby insures the reliability of the insulating layer.
Throughout Figures 1-21, like parts are indicated with like reference numerals except where otherwise stated. The initial steps of the process for forming the third embodiment are the same as those explained in conjunction with Figures 1 and 2. After the infrared shield structure 32 has been formed, the wafer is placed into a sputtering apparatus where it is preheated, and a first relatively thin layer 80 of silicon dioxide (Figure 12) measuring approximately 1000 angstroms in thickness is deposited so that it covers the entire surface of the wafer. This layer is then patterned using photolithographic techniques to produce the first window 58, previously described in conjunction with the first embodiment.Again, damage caused to the cadmium sulfide substrate as a result of the sputtering process is removed by annealing the wafer for approximately 1 5 minutes at a temperature of approximately 2750C.
After annealing, the Schottky barrier metal layer 36 and the boundary metallization layer 42 are deposited and delineated as shown in Figures 13 and 14, the process steps being similar to those described in conjunction with Figures 4 and 5.
Next the wafer is again placed into the sputtering apparatus and a second relatively thick layer 82 of silicon dioxide (Figure 15) measuring approximately 4000 angstroms in thickness is deposited on top of the first layer of silicon dioxide 80. Photolithographic techniques are again employed in order to delineate the second insulating layer 82 to provide the first and second windows 56 and 58. This time, however, the second layer of silicon dioxide is delineated to provide a slightly smaller active area window 56' than that etched in the first layer of silicon dioxide 80. A single etching step removes portion of both the insulating layers 80 and 82 and of the upper one of the layers 52 to provide the window 58.
The contact adhesion layer 66 and the contact metallization layer 68 are deposited on top of the wafer (Figure 16) in a similar manner as previously described in conjunction with Figure 6 of the first embodiment. The contact pads 70 and 72 are built up by electroplating as shown in Figure 17. And in a similar fashion to the first embodiment, the portions of the layers 66 and 68 which are not under the contact pads 70 and 72 are successively etched away as shown in Figures 18 and 19. This isolates the ohmic and barrier contacts 38 and 40 from each other. And as shown in Figure 19 the exposed portion of the boundary layer 42 is etched away in the central window 56 leaving the boundary layer ring 42a.
Finally, as shown in Figure 20, the gold wire leads 46 and 48 are attached to the ohmic and barrier contacts 38 and 40, respectively, by thermo-compression or thermosonic bonding as was done with the first embodiment. Lower surface processing of the wafer, sawing of the wafer into individual detector units, and final testing of each individual detector may then be accomplished as summarized in connection with the first embodiment.
Having described preferred embodiments of the present invention, it will be apparent to those skilled in the art that the invention permits modification in both arrangement and detail.
Therefore, the present invention should be limited only in accordance with the scope of the following

Claims (27)

claims. Claims
1. A Schottky barrier photovoltaic detector suitable for detecting ultraviolet and infrared radiation comprising: a cadmium suflide substrate having upper and lower surfaces; an infrared shield structure overlying the upper surface of the substrate, including a layer of a material which is substantially opaque to infrared radiation, the shield structure being delineated to provide a first central window therein; an insulating layer covering the infrared shield structure and having a second central window and a side window therein, the second central window being coincident with and slightly smaller than the first central window; a Schottky barrier metallization layer positioned within the second central window and completely covering the portion of the substrate which is located therein, the Schottky barrier metallization layer being sufficiently thin so that it is substantially transparent to ultraviolet and infrared radiation; means positioned above the upper surface of the substrate for providing a barrier contact extending through the second central window and leaving a major portion of the Schottky barrier metallization layer exposed; and means positioned above the upper surface of the substrate for providing an ohmic contact extending through the side window.
2. A detector according to claim 1 wherein the insulating layer is made of silicon dioxide.
3. A detector according to claim 1 or 2 and further comprising a boundary layer positioned between the barrier contact means the Schottky barrier metallization layer, the boundary layer being made of a material that prevents the barrier contact means from affecting the properties of the Schottky barrier formed by the junction of the substrate and the Schottky barrier metallization layer.
4. A detector according to claim 1, 2 or 3 wherein the infrared shield structure includes a layer of the gold sandwiched between two layers of a material selected from the group consisting of titanium, aluminum, magnesium, zirconium, and hafnium.
5. A detector according to any one of claims 1-4 wherein the Schottky barrier metallization layer is made of a material selected from the group consisting of platinum, gold and iridium.
6. A detector according to any one of claims 1-5 wherein the boundary layer is made of a material selected from the group consisting of gold, tungstem, nichrome, iridium, rhenium, paladium and rhodium.
7. A detector according to any one of the preceding claims wherein the barrier and ohmic contact means each include a lower contact adhesion layer made from a material selected from the group consisting of titanium, tungsten, nichrome, and chromium, and an upper contact pad made of a material selected from the group consisting of gold and aluminum.
8. A detector according to any one of the preceding claims and further comprising a pair of gold lead wires each having an end which is thermo-compression bonded to a respective one of the barrier and ohmic contact means.
9. A detector according to any one of the preceding claims and further comprising an infrared radiation sensor positioned closely adjacent to the lower surface of the substrate directly below the first and second central windows, the infrared shield structure extending beyond the side edges of the infrared sensor.
10. A detector according to any one of the preceding claims and further comprising a compensated layer in the substrate adjacent to its upper surface forming an avalanche region which protects the detector when excessive voltage is applied to it.
11. A process of fabricating a Schottky barrier photovoltaic detector comprising the steps of: slicing a wafer from a single crystalline cadmium sulfide ingot, the wafer having upper and lower substantially parallel planar surfaces which are perpendicular to the C-axis of the hexagonal crystal of the cadmium sulfide; lapping, polishing, and etching the upper surface of the wafer to produce a substrate having a smooth upper surface and a lower surface; depositing and delineating an infrared shield structure on the upper surface of the substrate, including a layer of a material which is substantially opaque to infrared radiation, the shield structure having a first central window therein; depositing and delineating an insulating layer over the infrared shield structure, the insulating layer having a second central window and a side window therein, the second central window being coincident with and slightly smaller than the first central window; depositing and delineating a Schottky barrier metallization layer within the second central window so that it completely covers the portion of the substrate which is located therein, the Schottky barrier metallization layer being sufficiently thin so that it is substantially transparent to ultraviolet and infrared radiation; and depositing and delineating barrier and ohmic contacts which extend above the upper surface of the substrate through the second central window and the side window, respectively, the barrier contact leaving a major portion of the Schottky barrier metallization layer exposed.
12. A process according ho claim 11 and further comprising the step of depositing and delineating a boundary layer between the barrier contact and the Schottky barrier metallization layer before depositing and delineating the barrier contact, said boundary layer preventing the barrier contact from affecting the properties of the Schottky barrier formed by the junction of the upper surface of the substrate and the Schottky barrier metallization layer, said boundary layer being made from a material selected from the group consisting of gold, tungsten, nichrome, iridium, rhenium, palladium and rhodium.
13. A process according to claim 11 or 12 wherein the insulating layer is made of silicon dioxide and is approximately 500 to approximately 20,000 angstroms thick.
14. A process according to any one of claims 11-13 wherein the step of depositing and delineating an insulating layer includes depositing and delineating a first layer of silicon dioxide over the infrared shield structure, the first layer of silicon dioxide having a first window portion coincident with and slightly smaller than the first central window, depositing a second insulating layer made of silicon dioxide over the first layer of silicon dioxide, and forming a second window portion in said second insulating layer, said second window portion being coincident with and slightly smaller than said first window portion, said first and second window portions together forming said second central window, and forming said side window extending through said first and second insulation layers to the layer of material in the infrared shield structure which is substantially opaque to infrared radiation.
15. A process according to any one of claims 11-14 and further comprising the step of thermo-compression bonding the ends of a pair of gold lead wires to respective ones of the barrier and ohmic contacts.
16. A process according to any one of claims 11-15 wherein the step of depositing and delineating the infrared shield structure includes the formation of a layer of gold sandwiched between first and second layers of a material selected from the group consisting of titanium, aluminum, magnesium, zirconium and hafnium.
17. A process according to any one of claims 11-16 wherein the Schottky barrier metallization layer is made of a material selected from the group consisting of platinum, gold and iridium.
18. A process according to any one of claims 11~17 wherein the barrier and ohmic contacts each include a lower contact adhesion layer made from a material selected from the group consisting of titanium, nichrome, tungsten, and chromium, and an upper contact pad made of a material selected from the group consisting of gold and aluminum.
19. A process according to any one of claims 11~18 wherein the step of depositing and delineating the infrared shield structure includes the formation of a layer of gold sandwiched between first and second layers of titanium, each of said first and second layers of titanium being approximately 50 angstroms to approximately 5,000 angstroms thick and the gold layer is approximately 500 angstroms to approximately 1 0,000 angstroms thick.
20. A process according to any one of claims 11-19 wherein the Schottky barrier metallization layer is made of platinum and is approximately 5 angstroms to approximately 50 angstroms thick.
21. A process according to claim 12 wherein the boundary layer is made of gold and is approximately 100 angstroms to approximately 300 angstroms thick.
22. A process according to any one of claims 11-21 wherein the step of depositing and delineating the barrier and ohmic contacts includes the step of depositing a contact adhesion layer made of titanium which is approximately 50 angstroms to approximately 5,000 angstroms thick, followed by the step of depositing a contact metallization layer made of gold which is approximately 1,000 to approximately 2,000 angstroms thick, followed by the step of electroplating barrier and ohmic contact pads made of gold onto the contact metallization layer so that the contact pads extend above the insulation layer.
23. A process according to claim 14 wherein the first insulating layer of silicon dioxide is relatively thin in comparison to the thickness of the second insulating layer of silicon dioxide.
24. A process according to claim 23 wherein the first insulating layer of silicon dioxide is approximately 1,000 angstroms thick and the second insulating layer of silicon dioxide is approximately 4,000 angstroms thick.
25. A process according to any one of claims 11-24 wherein the step of depositing and delineating the infrared shield structure includes the formation of a gold layer approximately 1,500 angstroms thick, sandwiched between first and second layers of titanium, each of said first and second layers of titanium being approximately 1,500 angstroms thick.
26. A process according to any of one claims 11-25 wherein the Schottky barrier metallization layer is made of platinum and is approximately 15 angstroms thick.
27. A detector fabricated in accordance with the process of any one of the claims 11-26.
GB8105367A 1980-03-07 1981-02-20 Schottky barrier photovoltaic detector and process Expired GB2071415B (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP3520148A1 (en) * 2016-09-28 2019-08-07 Raytheon Company Ultraviolet (uv) schottky diode detector having single crystal uv radiation detector material bonded directly to a support structure with proper c-axis orientation

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP3520148A1 (en) * 2016-09-28 2019-08-07 Raytheon Company Ultraviolet (uv) schottky diode detector having single crystal uv radiation detector material bonded directly to a support structure with proper c-axis orientation

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