US20140110805A1 - Silicon light trap devices, systems and methods - Google Patents
Silicon light trap devices, systems and methods Download PDFInfo
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- US20140110805A1 US20140110805A1 US13/654,917 US201213654917A US2014110805A1 US 20140110805 A1 US20140110805 A1 US 20140110805A1 US 201213654917 A US201213654917 A US 201213654917A US 2014110805 A1 US2014110805 A1 US 2014110805A1
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- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 title claims abstract description 63
- 238000000034 method Methods 0.000 title claims description 13
- 229910052710 silicon Inorganic materials 0.000 title abstract description 16
- 239000010703 silicon Substances 0.000 title abstract description 16
- 239000000463 material Substances 0.000 description 8
- 230000001419 dependent effect Effects 0.000 description 5
- 239000002800 charge carrier Substances 0.000 description 4
- 238000010348 incorporation Methods 0.000 description 3
- JBRZTFJDHDCESZ-UHFFFAOYSA-N AsGa Chemical compound [As]#[Ga] JBRZTFJDHDCESZ-UHFFFAOYSA-N 0.000 description 2
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 229910052732 germanium Inorganic materials 0.000 description 2
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 2
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 230000005693 optoelectronics Effects 0.000 description 2
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 1
- KWYUFKZDYYNOTN-UHFFFAOYSA-M Potassium hydroxide Chemical compound [OH-].[K+] KWYUFKZDYYNOTN-UHFFFAOYSA-M 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 239000012670 alkaline solution Substances 0.000 description 1
- 238000013459 approach Methods 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 238000000407 epitaxy Methods 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 239000001257 hydrogen Substances 0.000 description 1
- 229910052739 hydrogen Inorganic materials 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 239000011159 matrix material Substances 0.000 description 1
- 229910021421 monocrystalline silicon Inorganic materials 0.000 description 1
- 238000005215 recombination Methods 0.000 description 1
- 230000006798 recombination Effects 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
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Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/12002—Three-dimensional structures
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/122—Basic optical elements, e.g. light-guiding paths
- G02B6/1223—Basic optical elements, e.g. light-guiding paths high refractive index type, i.e. high-contrast waveguides
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/40—Optical elements or arrangements
- H10F77/413—Optical elements or arrangements directly associated or integrated with the devices, e.g. back reflectors
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/40—Optical elements or arrangements
- H10F77/42—Optical elements or arrangements directly associated or integrated with photovoltaic cells, e.g. light-reflecting means or light-concentrating means
- H10F77/488—Reflecting light-concentrating means, e.g. parabolic mirrors or concentrators using total internal reflection
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B2006/12035—Materials
- G02B2006/12061—Silicon
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B2006/12083—Constructional arrangements
- G02B2006/121—Channel; buried or the like
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/12—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type of the integrated circuit kind
- G02B6/13—Integrated optical circuits characterised by the manufacturing method
- G02B6/136—Integrated optical circuits characterised by the manufacturing method by etching
-
- 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
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/50—Photovoltaic [PV] energy
- Y02E10/52—PV systems with concentrators
Definitions
- the invention relates generally to silicon devices and more particularly to optoelectronic silicon devices.
- light rays are absorbed and generate charge carriers within the device.
- charge carriers typically are desired to be generated within a particular light ray absorption region, which can be defined by a depth within the device, such that they can be collected near the surface of the device.
- Charge carriers generated deeper than the depth of this region can be thought of us undesirable noise.
- Conventional approaches to dealing with these charge carriers often relate to transporting them to the surface by extended electric fields or annihilating them by the targeted introduction of recombination centers.
- the former is not suitable in all situations, such as those with regions that must remain free of electrical fields for physical reasons, and is also limited by available voltage, while the latter reduces internal quantum efficiency and can be technically difficult to realize at very high impurity atom densities.
- Reduced quantum efficiency in turn can affect devices dimensions, and increased complexity and technological challenges can increase costs, which are undesired.
- Embodiments relate to light trap devices, systems and methods.
- a device comprises a silicon structure having a surface to be exposed to light rays; and a light trap structure formed within the silicon structure spaced apart from the surface and comprising a plurality of light trap elements adjacent one another and each having a surface proximate to and unparallel with the surface to be exposed to light rays.
- a light trap structure buried within a silicon structure and comprises a plurality of light trap elements adjacent one another and each having a surface proximate to and unparallel with a surface of the silicon structure to be exposed to light rays.
- a method comprises providing a silicon structure; and forming a plurality of light trap elements adjacent one another in the silicon structure and each having a surface proximate to and unparallel with a surface of the silicon structure to be exposed to light rays.
- FIG. 1 is a side cross-sectional view of a light trap structure in a silicon structure according to an embodiment.
- FIG. 2 is a side cross-sectional view of a light trap structure in a silicon structure according to an embodiment.
- FIG. 3 is a side cross-sectional view of a light trap structure in a silicon structure according to an embodiment.
- FIG. 4 is a side cross-sectional view of a light ray striking a silicon structure having a light trap structure according to an embodiment.
- FIG. 5A is a side cross-sectional view of a silicon structure according to an embodiment.
- FIG. 5B is a side cross-sectional view of a plurality of trenches formed in a silicon structure according to an embodiment.
- FIG. 5C is a side cross-sectional view of a plurality of cavities formed from the trenches of FIG. 5B according to an embodiment.
- FIG. 5D is a side cross-sectional view of a photodetector device comprising a light trap structure according to an embodiment.
- FIG. 6 is a side cross-sectional view of a light trap structure in a silicon structure having a light-focusing roof structure according to an embodiment.
- Embodiments relate to buried structures for silicon devices which can alter light paths and thereby form light traps.
- Embodiments of the lights traps can couple more light to a photosensitive surface of the device, rather than reflecting the light or absorbing it more deeply within the device, which can increase efficiency, improve device timing and provide other advantages appreciated by those skilled in the art.
- Silicon structure 102 can comprise or consist of silicon in various embodiments, and in still other embodiments can comprise material(s) other than silicon.
- Light trap structure 100 comprises a plurality of light trap elements 104 arranged immediately adjacent one another.
- Light trap elements 104 can have length and/or width dimensions of about 0.5 ⁇ m to about 3 ⁇ m, height dimensions of about 1 ⁇ m to about 5 ⁇ m, and be disposed about 0.7 ⁇ m to about 50 ⁇ m from a top surface of silicon structure 102 in embodiments, though these dimensions can vary in other embodiments.
- light trap elements 104 can be formed from trenches that extend partially, substantially or entirely along a length of silicon structure 102 .
- light trap elements 104 comprise cavities filled with air or some other suitable gas or material.
- Light trap structure 100 also can comprise a single light trap element 104 having the overall outline shape of structure 100 depicted in FIG. 1 but with the individual cavities being linked or joined to form a single cavity structure.
- Light trap structure 100 can comprise a single row of light trap elements 104 or a matrix of light trap elements, for example comprising four rows having eight elements 104 each. Though depicted in FIG. 1 as extending from one side of silicon structure 102 to the other, in other embodiments light trap structure can be formed in only a portion of silicon structure 102 , such as is depicted in FIG. 2 .
- light trap elements 104 comprise curved, rounded or arched top and bottom (with respect to the depiction of the drawing on the page) portions.
- the top can be curved and the bottom can have some other shape or structure, for example being generally flat and therefore parallel with a top surface of silicon structure 102 .
- light trap elements 104 can have other shapes, such as peaked or pointed as depicted in FIG. 3 . In general, however, it can be seen that the surface of each light trap element 104 adjacent or opposing the upper surface of silicon structure 102 are angled, curved or otherwise unparallel with that upper surface.
- the particular radius of curvature ( FIGS. 1 and 2 ) or angle ( FIG. 3 ) of the surfaces of light trap elements 104 can vary in embodiments according to materials used, light wavelengths and other factors.
- silicon has a relatively high refractive index, such as between about 3.5 and 5.5 depending upon the wavelength of light.
- a critical angle of about 16 degrees exists: all light rays impinging from silicon structure 102 on an interface with a vacuum or air layer at an angle greater than about 16 degrees will be totally reflected.
- light rays which enter silicon structure 102 and are reflected internally at an angle greater than 16 degrees will be subject to total reflection within silicon structure 102 .
- silicon structure 102 can comprise some other material, such as germanium, gallium arsenide, another 3-5 group semiconductor material, or another suitable material.
- Germanium and gallium arsenide for example, generally have high refraction indices, like silicon, such that the total reflection angle will be below about 20 degrees in these embodiments as well, though one skilled in the art will appreciate that the angle can vary according to the properties of the material(s) used.
- a light ray 106 impinging on silicon structure 102 is reflected by light trap structure 100 back toward the surface 108 , which is a silicon-air interface. Because of the arched structure of the light trap elements 104 , ray 106 impinges on surface 108 from within silicon structure 102 at an angle ⁇ greater than about 16 degrees. This causes ray 106 to be reflected back toward light trap structure 100 , which again causes ray 106 to strike surface 108 at an angle greater than about 16 degrees and be reflected internally.
- This internal reflection caused by altering the path of light ray 106 by light trap structure 100 can improve the efficiency of the device because a larger portion of light impinging on the device can be used by the device, such as by coupling more light to a photo surface of the device rather than be reflected externally.
- the embodiment of FIG. 3 also can provide advantages.
- the peaked light trap elements 104 of FIG. 3 can be more efficient by presenting a smaller portion of each element 104 which would cause the light to be reflected externally.
- the number of light rays striking the very peak of the light elements 104 generally will be very small, such that more light rays will be reflected internally similar to as depicted in FIG. 4 .
- FIGS. 5A-5D one example process for forming light trap structure 100 is depicted.
- a dilemma for forming cavities in monocrystalline silicon can be used, though other processes can be used in this and other embodiments.
- a silicon structure 102 such as a silicon wafer, is provided.
- FIG. 5B at least one trench 110 is etched in silicon structure 102 .
- Silicon structure 102 is then exposed to a hydrogen atmosphere and a reflow process or epitaxy step, which results in the silicon-on-nothing structure 102 depicted in FIG. 5C , in which light trap elements 104 have been formed from each of the at least one trenches 110 .
- FIG. 5A a silicon structure 102 , such as a silicon wafer, is provided.
- FIG. 5B at least one trench 110 is etched in silicon structure 102 .
- Silicon structure 102 is then exposed to a hydrogen atmosphere and a reflow process or epitaxy step, which results in the silicon-on-nothing structure 102 depict
- 5D depicts one example of a final photo-sensitive structure 112 , such as a photo diode, after formation of a photo detector 114 between light trap structure 100 and surface 108 .
- photo-sensitive structure 112 forms only a portion of surface 108 , such as a photo-sensitive “window” of the device, though this can vary in other embodiments to include an entire surface or a plurality of photo-sensitive structures spaced apart at a surface or some other arrangement.
- the process can vary for other embodiments, such as the peaked light trap structure 100 of FIG. 3 .
- silicon structure 102 and trenches 110 can be treated with an alkaline solution to anisotropically etch the silicon, thereby uncovering the (111) surface of the silicon, which results in the peaks of FIG. 3 as the angle of about 54.7 degrees between (100) and (111) planes of the silicon of silicon structure 102 .
- Other surfaces of the silicon, such as the (110) surface also can be used in embodiments to produce different angles of the peaks, which vary with the crystal orientation of the silicon, though other angles can be less efficient.
- the angle can be between about 50 degrees and about 60 degrees, such as between about 53 and 56 degrees, for example about 54.7 degrees in embodiments.
- a roof structure 116 can be used with light trap structure 100 to further maximize quantum efficiency.
- a roof structure 116 can be used in photovoltaics, such as high-powered solar cells, and other applications to better channel or focus light rays to photosensitive elements below.
- roof structure 116 comprises a plurality of inverted pyramid, funnel or other light-focusing structures and can be formed by a masked potassium hydroxide solution etch or some other suitable process step(s). Roof structure 116 need not be a separate layer as depicted but instead can be an area or portion of silicon structure 102 that is etched, patterned or otherwise altered to include one or more light-focusing structures.
- light trap structure 100 can comprise a thermal liner oxide layer in order to electrically passivate the interface between surface 108 and/or to electrically insulate the region from the substrate below.
- roof structure 116 and/or a thermal liner oxide layer in combination with a light trap structure can thereby provide benefits in embodiments.
- Embodiments thereby provide improved light trap structures for silicon devices which can alter light paths.
- Embodiments of the lights traps can couple more light to a photosensitive surface of the device, rather than reflecting the light or absorbing it more deeply within the device, which can increase efficiency, improve device timing and provide other advantages appreciated by those skilled in the art.
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- Engineering & Computer Science (AREA)
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Abstract
Embodiments relate to buried structures for silicon devices which can alter light paths and thereby form light traps. Embodiments of the lights traps can couple more light to a photosensitive surface of the device, rather than reflecting the light or absorbing it more deeply within the device, which can increase efficiency, improve device timing and provide other advantages appreciated by those skilled in the art.
Description
- The invention relates generally to silicon devices and more particularly to optoelectronic silicon devices.
- In optoelectronic devices, light rays are absorbed and generate charge carriers within the device. These charge carriers typically are desired to be generated within a particular light ray absorption region, which can be defined by a depth within the device, such that they can be collected near the surface of the device.
- Charge carriers generated deeper than the depth of this region can be thought of us undesirable noise. Conventional approaches to dealing with these charge carriers often relate to transporting them to the surface by extended electric fields or annihilating them by the targeted introduction of recombination centers. The former is not suitable in all situations, such as those with regions that must remain free of electrical fields for physical reasons, and is also limited by available voltage, while the latter reduces internal quantum efficiency and can be technically difficult to realize at very high impurity atom densities. Reduced quantum efficiency in turn can affect devices dimensions, and increased complexity and technological challenges can increase costs, which are undesired.
- Embodiments relate to light trap devices, systems and methods.
- In an embodiment, a device comprises a silicon structure having a surface to be exposed to light rays; and a light trap structure formed within the silicon structure spaced apart from the surface and comprising a plurality of light trap elements adjacent one another and each having a surface proximate to and unparallel with the surface to be exposed to light rays.
- In an embodiment, a light trap structure buried within a silicon structure and comprises a plurality of light trap elements adjacent one another and each having a surface proximate to and unparallel with a surface of the silicon structure to be exposed to light rays.
- In an embodiment, a method comprises providing a silicon structure; and forming a plurality of light trap elements adjacent one another in the silicon structure and each having a surface proximate to and unparallel with a surface of the silicon structure to be exposed to light rays.
- The invention may be more completely understood in consideration of the following detailed description of various embodiments of the invention in connection with the accompanying drawings, in which:
-
FIG. 1 is a side cross-sectional view of a light trap structure in a silicon structure according to an embodiment. -
FIG. 2 is a side cross-sectional view of a light trap structure in a silicon structure according to an embodiment. -
FIG. 3 is a side cross-sectional view of a light trap structure in a silicon structure according to an embodiment. -
FIG. 4 is a side cross-sectional view of a light ray striking a silicon structure having a light trap structure according to an embodiment. -
FIG. 5A is a side cross-sectional view of a silicon structure according to an embodiment. -
FIG. 5B is a side cross-sectional view of a plurality of trenches formed in a silicon structure according to an embodiment. -
FIG. 5C is a side cross-sectional view of a plurality of cavities formed from the trenches ofFIG. 5B according to an embodiment. -
FIG. 5D is a side cross-sectional view of a photodetector device comprising a light trap structure according to an embodiment. -
FIG. 6 is a side cross-sectional view of a light trap structure in a silicon structure having a light-focusing roof structure according to an embodiment. - While the invention is amenable to various modifications and alternative forms, specifics thereof have been shown by way of example in the drawings and will be described in detail. It should be understood, however, that the intention is not to limit the invention to the particular embodiments described. On the contrary, the intention is to cover all modifications, equivalents, and alternatives falling within the spirit and scope of the invention as defined by the appended claims.
- Embodiments relate to buried structures for silicon devices which can alter light paths and thereby form light traps. Embodiments of the lights traps can couple more light to a photosensitive surface of the device, rather than reflecting the light or absorbing it more deeply within the device, which can increase efficiency, improve device timing and provide other advantages appreciated by those skilled in the art.
- Referring to
FIG. 1 , an embodiment of alight trap structure 100 embedded in asilicon structure 102 is depicted.Silicon structure 102 can comprise or consist of silicon in various embodiments, and in still other embodiments can comprise material(s) other than silicon.Light trap structure 100 comprises a plurality oflight trap elements 104 arranged immediately adjacent one another.Light trap elements 104 can have length and/or width dimensions of about 0.5 μm to about 3 μm, height dimensions of about 1 μm to about 5 μm, and be disposed about 0.7 μm to about 50 μm from a top surface ofsilicon structure 102 in embodiments, though these dimensions can vary in other embodiments. For example,light trap elements 104 can be formed from trenches that extend partially, substantially or entirely along a length ofsilicon structure 102. - In embodiments,
light trap elements 104 comprise cavities filled with air or some other suitable gas or material.Light trap structure 100 also can comprise a singlelight trap element 104 having the overall outline shape ofstructure 100 depicted inFIG. 1 but with the individual cavities being linked or joined to form a single cavity structure.Light trap structure 100 can comprise a single row oflight trap elements 104 or a matrix of light trap elements, for example comprising four rows having eightelements 104 each. Though depicted inFIG. 1 as extending from one side ofsilicon structure 102 to the other, in other embodiments light trap structure can be formed in only a portion ofsilicon structure 102, such as is depicted inFIG. 2 . - In the embodiment of
FIG. 1 ,light trap elements 104 comprise curved, rounded or arched top and bottom (with respect to the depiction of the drawing on the page) portions. In other embodiments, only the top can be curved and the bottom can have some other shape or structure, for example being generally flat and therefore parallel with a top surface ofsilicon structure 102. In still other embodiments,light trap elements 104 can have other shapes, such as peaked or pointed as depicted inFIG. 3 . In general, however, it can be seen that the surface of eachlight trap element 104 adjacent or opposing the upper surface ofsilicon structure 102 are angled, curved or otherwise unparallel with that upper surface. - The particular radius of curvature (
FIGS. 1 and 2 ) or angle (FIG. 3 ) of the surfaces oflight trap elements 104 can vary in embodiments according to materials used, light wavelengths and other factors. For example, silicon has a relatively high refractive index, such as between about 3.5 and 5.5 depending upon the wavelength of light. For a light wavelength of about 850 nm, a critical angle of about 16 degrees exists: all light rays impinging fromsilicon structure 102 on an interface with a vacuum or air layer at an angle greater than about 16 degrees will be totally reflected. Thus, light rays which entersilicon structure 102 and are reflected internally at an angle greater than 16 degrees will be subject to total reflection withinsilicon structure 102. In other embodiments,silicon structure 102 can comprise some other material, such as germanium, gallium arsenide, another 3-5 group semiconductor material, or another suitable material. Germanium and gallium arsenide, for example, generally have high refraction indices, like silicon, such that the total reflection angle will be below about 20 degrees in these embodiments as well, though one skilled in the art will appreciate that the angle can vary according to the properties of the material(s) used. - Referring to
FIG. 4 , alight ray 106 impinging onsilicon structure 102 is reflected bylight trap structure 100 back toward thesurface 108, which is a silicon-air interface. Because of the arched structure of thelight trap elements 104,ray 106 impinges onsurface 108 from withinsilicon structure 102 at an angle α greater than about 16 degrees. This causesray 106 to be reflected back towardlight trap structure 100, which again causesray 106 to strikesurface 108 at an angle greater than about 16 degrees and be reflected internally. This internal reflection caused by altering the path oflight ray 106 bylight trap structure 100 can improve the efficiency of the device because a larger portion of light impinging on the device can be used by the device, such as by coupling more light to a photo surface of the device rather than be reflected externally. - The embodiment of
FIG. 3 also can provide advantages. For example, the peakedlight trap elements 104 ofFIG. 3 can be more efficient by presenting a smaller portion of eachelement 104 which would cause the light to be reflected externally. In other words, the number of light rays striking the very peak of thelight elements 104 generally will be very small, such that more light rays will be reflected internally similar to as depicted inFIG. 4 . - Referring next to
FIGS. 5A-5D , one example process for forminglight trap structure 100 is depicted. In one embodiment, a Venezia process for forming cavities in monocrystalline silicon can be used, though other processes can be used in this and other embodiments. InFIG. 5A , asilicon structure 102, such as a silicon wafer, is provided. InFIG. 5B , at least onetrench 110 is etched insilicon structure 102.Silicon structure 102 is then exposed to a hydrogen atmosphere and a reflow process or epitaxy step, which results in the silicon-on-nothing structure 102 depicted inFIG. 5C , in whichlight trap elements 104 have been formed from each of the at least onetrenches 110.FIG. 5D depicts one example of a final photo-sensitive structure 112, such as a photo diode, after formation of aphoto detector 114 betweenlight trap structure 100 andsurface 108. As depicted inFIG. 5D , photo-sensitive structure 112 forms only a portion ofsurface 108, such as a photo-sensitive “window” of the device, though this can vary in other embodiments to include an entire surface or a plurality of photo-sensitive structures spaced apart at a surface or some other arrangement. - The process can vary for other embodiments, such as the peaked
light trap structure 100 ofFIG. 3 . For such an embodiment, for example,silicon structure 102 andtrenches 110 can be treated with an alkaline solution to anisotropically etch the silicon, thereby uncovering the (111) surface of the silicon, which results in the peaks ofFIG. 3 as the angle of about 54.7 degrees between (100) and (111) planes of the silicon ofsilicon structure 102. Other surfaces of the silicon, such as the (110) surface, also can be used in embodiments to produce different angles of the peaks, which vary with the crystal orientation of the silicon, though other angles can be less efficient. For example, the angle can be between about 50 degrees and about 60 degrees, such as between about 53 and 56 degrees, for example about 54.7 degrees in embodiments. - Other features and elements can be incorporated in embodiments. For example, and referring to
FIG. 6 , aroof structure 116 can be used withlight trap structure 100 to further maximize quantum efficiency. Such aroof structure 116 can be used in photovoltaics, such as high-powered solar cells, and other applications to better channel or focus light rays to photosensitive elements below. In embodiments,roof structure 116 comprises a plurality of inverted pyramid, funnel or other light-focusing structures and can be formed by a masked potassium hydroxide solution etch or some other suitable process step(s).Roof structure 116 need not be a separate layer as depicted but instead can be an area or portion ofsilicon structure 102 that is etched, patterned or otherwise altered to include one or more light-focusing structures. In another example,light trap structure 100 can comprise a thermal liner oxide layer in order to electrically passivate the interface betweensurface 108 and/or to electrically insulate the region from the substrate below. Usingroof structure 116 and/or a thermal liner oxide layer in combination with a light trap structure can thereby provide benefits in embodiments. - Embodiments thereby provide improved light trap structures for silicon devices which can alter light paths. Embodiments of the lights traps can couple more light to a photosensitive surface of the device, rather than reflecting the light or absorbing it more deeply within the device, which can increase efficiency, improve device timing and provide other advantages appreciated by those skilled in the art.
- Various embodiments of systems, devices and methods have been described herein. These embodiments are given only by way of example and are not intended to limit the scope of the invention. It should be appreciated, moreover, that the various features of the embodiments that have been described may be combined in various ways to produce numerous additional embodiments. Moreover, while various materials, dimensions, shapes, configurations and locations, etc. have been described for use with disclosed embodiments, others besides those disclosed may be utilized without exceeding the scope of the invention.
- Persons of ordinary skill in the relevant arts will recognize that the invention may comprise fewer features than illustrated in any individual embodiment described above. The embodiments described herein are not meant to be an exhaustive presentation of the ways in which the various features of the invention may be combined. Accordingly, the embodiments are not mutually exclusive combinations of features; rather, the invention can comprise a combination of different individual features selected from different individual embodiments, as understood by persons of ordinary skill in the art. Moreover, elements described with respect to one embodiment can be implemented in other embodiments even when not described in such embodiments unless otherwise noted. Although a dependent claim may refer in the claims to a specific combination with one or more other claims, other embodiments can also include a combination of the dependent claim with the subject matter of each other dependent claim or a combination of one or more features with other dependent or independent claims. Such combinations are proposed herein unless it is stated that a specific combination is not intended. Furthermore, it is intended also to include features of a claim in any other independent claim even if this claim is not directly made dependent to the independent claim.
- Any incorporation by reference of documents above is limited such that no subject matter is incorporated that is contrary to the explicit disclosure herein. Any incorporation by reference of documents above is further limited such that no claims included in the documents are incorporated by reference herein. Any incorporation by reference of documents above is yet further limited such that any definitions provided in the documents are not incorporated by reference herein unless expressly included herein.
- For purposes of interpreting the claims for the present invention, it is expressly intended that the provisions of
Section 112, sixth paragraph of 35 U.S.C. are not to be invoked unless the specific terms “means for” or “step for” are recited in a claim.
Claims (25)
1. A device comprising:
a silicon structure having a surface to be exposed to light rays; and
a light trap structure formed within the silicon structure spaced apart from the surface and comprising a plurality of light trap elements adjacent one another and each having a surface proximate to and unparallel with the surface to be exposed to light rays.
2. The device of claim 1 , wherein the surface proximate to and unparallel with the surface to be exposed to light rays has a radius.
3. The device of claim 1 , wherein the surface proximate to and unparallel with the surface to be exposed to light rays comprises a peak.
4. The device of claim 3 , wherein am angle of the peak is between about 50 degrees and about 60 degrees.
5. The device of claim 4 , wherein the angle of the peak is about 54.7 degrees.
6. The device of claim 1 , wherein the plurality of light trap elements each comprise a cavity within the silicon structure.
7. The device of claim 6 , wherein each cavity is formed from a trench etched in the silicon structure.
8. The device of claim 1 , wherein each surface proximate to and unparallel with the surface to be exposed to light rays is configured to reflect light toward the surface to be exposed to light rays at an angle greater than about 16 degrees.
9. The device of claim 1 , wherein the device comprises a photodetector device.
10. The device of claim 1 , wherein each light trap element is about 0.5 micrometers (μm) to about 3 μm wide and about 1 μm to about 5 μm high.
11. The device of claim 1 , wherein each light trap element is spaced apart from the surface to be exposed to light rays by at least about 0.7 μm and not more than about 50 μm.
12. The device of claim 1 , further comprising a structure formed on the surface to be exposed to light and comprising a plurality of light-focusing structures.
13. A light trap structure buried within a silicon structure and comprising:
a plurality of light trap elements adjacent one another and each having a surface proximate to and unparallel with a surface of the silicon structure to be exposed to light rays.
14. The light trap structure of claim 13 , wherein the plurality of light trap elements comprise a plurality of cavities.
15. The light trap structure of claim 13 , wherein the surface proximate to and unparallel with the surface to be exposed to light rays has a radius.
16. The device of claim 13 , wherein the surface proximate to and unparallel With the surface to be exposed to light rays comprises a peak.
17. The device of claim 16 , wherein an angle of the peak is between about 53 degrees and about 56 degrees.
18. The device of claim 13 , wherein the plurality of light trap elements each comprise a cavity within the silicon structure.
19. The device of claim 18 , wherein each cavity is formed from a trench etched in the silicon structure.
20. The device of claim 13 , wherein each surface proximate to and unparallel with the surface to be exposed to light rays is configured to reflect light toward the surface to be exposed to light rays at an angle greater than about 16 degrees.
21. The device of claim 13 , wherein each light trap element is about 0.5 micrometers (μm) to about 3 μm wide and about 1 μm to about 5 μm deep.
22. The device of claim 13 , wherein each light trap element is spaced apart from the surface to be exposed to light rays by at least about 0.7 μm and not more than about 50 μm.
23. A method comprising:
providing a silicon structure; and
forming a plurality of light trap elements adjacent one another in the silicon structure and each having a surface proximate to and unparallel with a surface of the silicon structure to be exposed to light rays.
24. The method of claim 23 , wherein forming a plurality of light trap elements further comprises:
forming a plurality of trenches in the silicon structure; and
producing a cavity from each of the plurality of trenches.
25. The method of claim 24 , further comprising forming a light-focusing structure on the silicon structure.
Priority Applications (2)
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US13/654,917 US20140110805A1 (en) | 2012-10-18 | 2012-10-18 | Silicon light trap devices, systems and methods |
US15/390,178 US10007056B2 (en) | 2012-10-18 | 2016-12-23 | Silicon light trap devices, systems and methods |
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US13/654,917 US20140110805A1 (en) | 2012-10-18 | 2012-10-18 | Silicon light trap devices, systems and methods |
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US10007056B2 (en) | 2012-10-18 | 2018-06-26 | Infineon Technologies Dresden Gmbh | Silicon light trap devices, systems and methods |
US10784147B2 (en) | 2017-07-20 | 2020-09-22 | Infineon Technologies Ag | Method for producing a buried cavity structure |
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US10007056B2 (en) | 2018-06-26 |
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