WO2024124327A1 - Methods for making solid state devices having spin-photon interfaces - Google Patents
Methods for making solid state devices having spin-photon interfaces Download PDFInfo
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- WO2024124327A1 WO2024124327A1 PCT/CA2023/051611 CA2023051611W WO2024124327A1 WO 2024124327 A1 WO2024124327 A1 WO 2024124327A1 CA 2023051611 W CA2023051611 W CA 2023051611W WO 2024124327 A1 WO2024124327 A1 WO 2024124327A1
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- G—PHYSICS
- G06—COMPUTING OR CALCULATING; COUNTING
- G06N—COMPUTING ARRANGEMENTS BASED ON SPECIFIC COMPUTATIONAL MODELS
- G06N10/00—Quantum computing, i.e. information processing based on quantum-mechanical phenomena
- G06N10/40—Physical realisations or architectures of quantum processors or components for manipulating qubits, e.g. qubit coupling or qubit control
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- C—CHEMISTRY; METALLURGY
- C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
- C23C16/00—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes
- C23C16/22—Chemical coating by decomposition of gaseous compounds, without leaving reaction products of surface material in the coating, i.e. chemical vapour deposition [CVD] processes characterised by the deposition of inorganic material, other than metallic material
- C23C16/24—Deposition of silicon only
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- G—PHYSICS
- G06—COMPUTING OR CALCULATING; COUNTING
- G06N—COMPUTING ARRANGEMENTS BASED ON SPECIFIC COMPUTATIONAL MODELS
- G06N10/00—Quantum computing, i.e. information processing based on quantum-mechanical phenomena
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y20/00—Nanooptics, e.g. quantum optics or photonic crystals
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- 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
- G02B6/12004—Combinations of two or more optical elements
Definitions
- This invention relates to generating spin-photon interfaces in silicon.
- Specific embodiments provide methods and apparatus for creating point defect colour centres such as T centres or G centres in silicon crystals.
- Quantum informatics involves storing and/or manipulating information represented by the state of a quantum system or a set of quantum systems.
- Quantum information may, for example be represented by the states of quantum systems as diverse as photons, superconducting loops, electron spins, nuclear spins, ions and others.
- Point defect colour centres have shown promise for use as quantum systems for storing and manipulating quantum information. Radiation damage centres in silicon are a class of point defect colour centres that shows promise for use as quantum systems for quantum informatics.
- the T centre notably possesses highly coherent electron and nuclear spin degrees of freedom as well as narrow, spindependent ensemble optical transitions that can emit and/or absorb photons at wavelengths of approximately 1326 nm, which lies in the telecommunications O-band. T centres can serve as long-lived colour centres.
- a T centre is made up of two carbon atoms and a hydrogen atom which occupy a location in a silicon crystalline lattice where one silicon atom is missing.
- the two carbon atoms share the substitutional site of the missing silicon atom.
- the interstitial hydrogen atom is chemically bonded to one of the carbon atoms while the other carbon atom remains stable with an unpaired electron.
- T centre ensemble can be fabricated in a silicon device layer of a silicon-on-insulator (SOI) wafer by ion implantation to introduce carbon and hydrogen ions into a silicon crystal and subsequent annealing of the silicon crystal.
- SOI silicon-on-insulator
- one drawback of this approach to creating T centres is that it is hard to control the depth in the silicon crystal at which the T centres are formed.
- the vertical distribution of T centres created by such ion implantation techniques is determined by implantation and annealing parameters, including implantation dose, acceleration voltage and annealing temperature. It would be beneficial to have finer control of the depth at which T centres are formed, for example, so that T centres can be placed at defined locations relative to other structures such as optical structures.
- T centres by ion implantation creates disorder/damages near the surface of the silicon due to the bombardment of the crystalline silicon with carbon atoms.
- Lattice disorder and crystal damage may degrade performance of T centres, for example by enhancement of trap states and recombination centres. Damage to the crystal lattice and formation of recombination centres inside the crystal lattice near the surface can lead to lower exciton lifetime and reduce coherence time of T centres. Qubit decoherence, relaxation from adsorbates on surfaces, impurities at interfaces, and material defects can all negatively impact performance of the T centres in quantum data processing applications.
- This invention has a number of aspects. These include but are not limited to:
- the spinphoton interfaces may, for example, comprise T centres or G centres. • precursor devices that include spin-photon interfaces; and
- One example aspect of the invention provides a method for making a device that includes luminescent centres. The method comprises the steps of:
- the method may further comprise providing the substrate and forming the first silicon layer on the substrate.
- the annealing process is a second annealing process and the method comprises causing carbon atoms to diffuse into the first and second silicon layers from the first interfacial layer by applying a first annealing process after forming the second silicon layer.
- the first annealing process has an annealing temperature of at least 500 °C.
- the second annealing process includes processing at an annealing temperature of at least 400 °C.
- the method comprises forming a plurality of alternating interfacial layers and silicon layers by alternately applying step (a)(i) to each successive silicon layer and step (a)(ii) to each successive interfacial layer before step (b).
- at least one of the silicon layers is formed through epitaxial growth or chemical vapor deposition.
- At least one of the silicon layers comprises isotopically purified silicon-28.
- the carbon containing material is elemental carbon. In some embodiments the carbon containing material is silicon carbide. In some embodiments the carbon containing material is isotopically enriched in 13 C. In some embodiments the carbon containing material is isotopically enriched in 12 C. In some embodiments the carbon containing material is a mixture of isotopically enriched 12 C and 13 C. In some embodiments the carbon containing material is carbon doped silicon. In some embodiments the carbon containing material contains isotopically purified silicon-28.
- a concentration of the luminescent centres is greatest at a depth corresponding to the interfacial layer.
- At least the step or introducing hydrogen atoms into the device layer is performed in a high vacuum environment.
- the first silicon layer has a thickness of less than 50 nm.
- the first interfacial layer has a thickness of less than 5 nm. In some embodiments the first interfacial layer has a thickness of about 5 Angstroms.
- the second silicon layer has a thickness in the range of about 10 nm to about 500 nm.
- a thickness of the device layer is about 500 nm or less.
- the first interfacial layer has a carbon concentration of at least 1x10 18 atoms cm' 3 . In some embodiments the first interfacial layer has a carbon concentration of at least 1x10 19 atoms cm' 3 .
- the first interfacial layer has a carbon density in a range of about 1x10 11 atoms cm' 2 to about 1x10 13 atoms cm' 2 . In some embodiments the first interfacial layer has a carbon density in a range of about 1x10 12 atoms cm' 2 to about 1x10 13 atoms cm' 2 .
- the method comprises forming an intermediate silicon layer on the first silicon layer prior to forming the first interfacial layer.
- a thickness of the second silicon layer is at least equal to a combined thickness of the first silicon layer, the intermediate silicon layer and the first interfacial layer.
- the substrate is a silicon on insulator (SOI) comprising an oxide insulator layer wherein the first silicon layer is formed on the oxide insulator layer.
- SOI silicon on insulator
- the first silicon layer is a seed layer.
- the silicon layers of the plurality of alternating interfacial layers and silicon layers each has a thickness of 20 nm or less.
- Another example aspect of the invention provides a precursor device comprising: a substrate comprising a carrier silicon layer and an insulator layer; a device layer supported on the substrate, the device layer comprising: a first silicon layer adjacent to the insulator layer of the substrate; an interfacial layer of carbon containing material deposited on the first silicon layer, the interfacial layer having a thickness not exceeding 2 nm; and a second silicon layer deposited on the interfacial layer.
- the precursor comprises a second interfacial layer of carbon containing material deposited on the second silicon layer and a third silicon layer deposited on the second interfacial layer.
- the precursor comprises a third interfacial layer of carbon containing material deposited on the third silicon layer and a fourth silicon layer deposited on the third interfacial layer.
- At least one of the silicon layers comprises isotopically purified silicon-28.
- the carbon containing material is silicon carbide. In some embodiments the carbon containing material is carbon doped silicon. In some embodiments the carbon containing material is elemental carbon. In some embodiments the carbon containing material contains isotopically purified silicon-28. In some embodiments the carbon containing material is isotopically enriched in 13 C. In some embodiments the carbon containing material is isotopically enriched in 12 C.
- the first silicon layer has a thickness of less than 50 nm.
- the interfacial layer has a thickness of about 5 Angstrom.
- the second silicon layer has a thickness in the range of about 10 nm to about 500 nm.
- a thickness of the device layer is 500 nm or less.
- the interfacial layer has a carbon concentration of at least 1x10 18 atoms cm' 3 . In some embodiments the interfacial layer has a carbon concentration of at least 1x10 19 atoms cm' 3 .
- the interfacial layer has a density of about 1x10 11 atoms cm' 2 to about 1x10 13 atoms cm' 2 . In some embodiments the interfacial layer has a density of about 1x10 12 atoms cm' 2 to about 1x10 13 atoms cm' 2 .
- the precursor device comprises an intermediate silicon layer between the first silicon layer and the interfacial layer.
- a thickness of the second silicon layer is at least equal to a combined thickness of the first silicon layer, the intermediate silicon layer and the interfacial layer.
- the substrate is a silicon on insulator (SOI) substrate.
- SOI silicon on insulator
- Another example aspect of the invention provides a device comprising: a substrate; a device layer supported on the substrate, the device layer comprising crystalline silicon and having a thickness of 500 nm or less; a plurality of luminescent centres localized within the device layer and concentrated within a first depth range that is equal to one half of the thickness of the device layer ⁇ 25%, wherein an average concentration of the luminescent centres within the first depth range is at least five times greater than an average concentration of the luminescent centres in a second depth range that extends from an outer surface of the device layer by a distance equal to 10% of the thickness of the device layer.
- the luminescent centres are T centres.
- the device further comprises an optical layer on the device layer wherein the optical layer comprises a plurality of optical resonators which have resonances at wavelengths corresponding to optical transitions of the T centres.
- the optical layer comprises a plurality of optical resonators which have resonances at wavelengths corresponding to optical transitions of the T centres.
- Another aspect of the invention provides methods having any new and inventive steps, acts, combination of steps and/or acts or sub-combination of steps and/or acts as described herein.
- FIG. 1 is a model that shows the structure of a T centre.
- FIG. 2 is a schematic cross sectional view of a SOI substrate.
- FIG. 3 is a flowchart for an example method of generating spin-photon interface in substrates with doping according to an example embodiment.
- FIG. 4A is a schematic cross sectional view of a substrate according to an example embodiment.
- FIG. 4B is a schematic cross sectional view of a substrate according to another example embodiment.
- FIG. 4C is a schematic cross sectional view of a substrate according to another example embodiment.
- FIG. 5 schematically illustrates an example carbon concentration profile within a modified device layer in the example embodiment substrate shown in FIG. 2A.
- FIG. 6 schematically illustrates another example carbon profile within another modified device layer in another example embodiment substrate.
- a spinphoton interface is a structure which includes at least one particle that has intrinsic spin and a plurality of states wherein the states can exist in quantum superpositions, such that there exists at least one spin-dependent (optical) transition between the states.
- a spin photon interface may selectively absorb a photon having a wavelength corresponding to the spin-dependent transition depending on a spin eigenstate of the particle.
- a spin photon interface may be caused to selectively emit a photon having a wavelength corresponding to the spin-dependent transition depending on a spin state of the particle.
- a spin-photon interface may, for example be applied (i.e.
- An example structure that may be used as a spin-photon interface is a T centre.
- Another example structure that may be used as a spin photon interface is a G centre.
- a spin-photon interface e.g. a T centre
- a device layer e.g. a device layer of a SOI wafer
- the optical mode intensity is maximum.
- One aspect of this invention provides methods for making structures that include silicon crystals that contain spin-photon interfaces such as T centres. Another aspect of this invention provides devices that include silicon crystals that contain spinphoton interfaces such as T centres. Another aspect of the invention provides devices that incorporate spin photon interfaces and have novel structures as described herein. Some embodiments provide devices that includes spin-photon interfaces such as T centres that are provided within a layer of silicon. The layer of silicon may be supported on a silicon on insulator (SOI) substrate. Spin photon interfaces may be distributed in the layer of silicon as described herein.
- SOI silicon on insulator
- FIG. 1 is a model that shows the structure of a T centre 10.
- the T centre is a structure in which a silicon atom in a silicon crystal has been replaced by two carbon atoms 11 A and 11 B and a hydrogen atom 12 bonded to carbon atom 11 B.
- Carbon atom 11 A has one unpaired electron.
- the spin state of the unpaired electron of carbon atom 11 A may be used as a quantum system.
- the nucleus of hydrogen atom 12 may also be used as a quantum system.
- one or both of the carbon atoms in a T centre are the carbon isotope 13 C.
- Nuclei of carbon-13 atoms have a spin of 14 and may be used as additional quantum systems (by contrast, nuclei of the carbon isotope 12 C do not have a net spin).
- T centres have properties that make their spins particularly good for use as storing quantum information. These properties include:
- T centres exhibit long spin coherence times (>2.1ms electron and >1s nuclear spin);
- T centres can couple to O-band photons (wavelengths including about 1326 nm);
- a T centre can provide multiple (e.g. up to 4) accessible spin manifolds; • A T centre couples weakly but controllably to lattice strain;
- a T centre couples weakly but controllably to electric fields
- a T centre can support excitons which may be used to store quantum information (e.g. in hole spins).
- FIG. 2 is a schematic cross sectional view of a SOI substrate 20.
- SOI substrate 20 comprises a carrier silicon layer 22, an insulator layer 24 fabricated on carrier silicon layer 22, and a silicon device layer 26 fabricated on insulator layer 24 such that insulator layer 24 is sandwiched between carrier silicon layer 22 and silicon device layer 26.
- Insulator layer 24 typically comprises silicon dioxide.
- Insulator layer 24 may be made with buried oxide in which case insulator layer 24 is sometimes referred to as a BOX layer.
- SOI substrates make convenient substrates for supporting active components of devices.
- devices as described herein include SOI substrates.
- SOI substrate 20 includes other layers. For example, additional layers may be included between carrier silicon layer 22 and BOX layer 24 to provide a Bragg reflector.
- the thickness of carrier silicon layer 22 is typically in the range of about 100 microns to about 1000 microns
- the thickness of insulator layer 24 is typically in the range of about 500 nm to about 5000 nm
- the thickness of silicon device layer 26 is typically in the range of about 100 nm to 500 nm.
- FIG. 3 is a flowchart for a method 30 of making a device that includes spinphoton interfaces.
- Method 30 involves creating a plurality of silicon layers with adjacent ones of the layers separated by thin layers of carbon (e.g. modified device layers 26A, 26B and 56 shown in FIG. 4A, FIG. 4B and FIG. 6 respectively).
- the resulting structure is annealed to cause carbon to diffuse into the silicon layers at a density which promotes formation of spin-photon interfaces such as luminescent centres and, in particular, luminescent centres in silicon that comprise carbon e.g. T centres or G centres in the silicon.
- the method 30 may include one or more additional steps to form interstitial carbon or silicon. These steps may include, for example, silicon ion implantation, plasma doping (e.g. using reactive ion etching) etc.
- a first silicon layer is created or provided.
- the first layer of silicon may, for example comprise a seed layer 21 (see Figs. 4A and 4B).
- a seed layer may serve as a catalyst layer that facilitates the growth of subsequent high quality functional layers of silicon by a process such as CVD or MBE and which establishes an orientation of one or more subsequent layers of silicon.
- the first layer of silicon might not be a seed layer.
- insulators on which crystalline material may be grown without requiring a seed layer is sapphire.
- the first layer of silicon may comprise a layer of silicon grown on sapphire.
- the first layer of silicon is preferably a thin layer.
- the first layer of silicon is preferably monocrystalline.
- the first layer of silicon is preferably a smooth layer. In some embodiments the roughness of the first layer of silicon is within a range of up to about 0.2nm root-mean-square deviation.
- the first layer of silicon has a thickness of less than 50 nm. In some embodiments the thickness of the first layer of silicon is in the range of about 5nm to about 200nm. In some embodiments the first layer of silicon comprises isotopically purified silicon-28.
- the first layer is deposited in a 111 orientation. In some embodiments the first layer of silicon and subsequent layers of silicon which make up the device layer are all deposited in a 111 orientation.
- method 30 applies an interfacial layer (see e.g. interfacial layer 23 in Figs. 4A and 4B) on the first layer of silicon.
- the first layer of silicon may be created (e.g. formed) in step S30A or may be provided as an input (e.g. as a silicon wafer, SOI substrate or the like) in step 30B of method 30.
- Interfacial layer 23 may, for example comprise a thin layer of a carbon containing material (e.g. carbon or carbon doped silicon such as silicon carbide (SiC)) on the first silicon layer.
- a carbon containing material e.g. carbon or carbon doped silicon such as silicon carbide (SiC)
- interfacial layer 23 has a thickness of about 10 nm.
- Interfacial layer 23 may be fabricated by depositing the carbon containing material by way of a technique such as molecular beam epitaxy (MBE), chemical vapour deposition (CVD), and metal organic chemical vapour deposition (MOCVD).
- MBE molecular beam epitaxy
- CVD chemical vapour deposition
- MOCVD metal organic chemical vapour deposition
- Fabrication of interfacial layer 23 is an example of “delta doping”. Delta doping allows introduction of carbon into adjacent silicon layers with minimal damage to the surface and structure of the thin crystalline silicon layers.
- the deposited carbon layer is very thin (essentially two-dimensional).
- the dopant is concentrated in one or at most two atomic layers in a crystal plane. Delta doping has been experimentally demonstrated, for example, by H.-J. Gossmann & E. F.
- Delta doping can advantageously be applied to incorporate carbon at significantly greater concentrations than would be readily achievable using other doping approaches.
- Delta doping takes advantage of thermodynamics, such that within each layer, the dopant atoms form a self-organized surface phase. This selforganized layer of carbon containing material within the crystal is stabilized by growing silicon (i.e. crystalline layer 25) on top of the two-dimensional dopant layer (i.e. interfacial layer 23).
- the carbon containing material has a selected isotopic composition.
- the carbon in the carbon containing material is enriched in 13 C which has a nuclear spin.
- the carbon in the carbon-containing material has been processed to decrease or remove isotopes other than 12 C, which does not have a nuclear spin.
- the carbon containing material is a mixture of isotopically enriched 12 C and 13 C. This may allow for forming T centres that each include a 13 C and a 12 C.
- the thickness of interfacial layer 23 is less than 50 nm. In some embodiments the thickness of interfacial layer 23 is about 10 nm. In some embodiments, the thickness of the interfacial layer 23 is less than 5 nm. In a preferred embodiment the thickness of interfacial layer 23 is about 5 Angstroms.
- the thickness of crystalline layer 25 is less than 500 nm.
- device layer 26A has a thickness in the range of about 100nm to about 500 nm.
- device layer 26A has a thickness in the range of about 200 nm to about 350 nm (for example a thickness of about 220 nm or about 330nm).
- the material of the interfacial layer may, for example, have a carbon concentration of at least 1x10 18 carbon atoms per cm 3 e.g. at least 3x10 18 carbon atoms per cm 3 or at least 1x10 19 carbon atoms per cm 3 .
- graphite contains approximately 1.1 x10 23 carbon atoms per cm 3 and SiC contains about 5 x10 22 carbon atoms per cm 3 .
- the deposited interfacial layer has a thickness such that the interfacial layer preferably provides a density of carbon atoms of about 1x10 11 erm 2 to about 1x10 13 cm’ 2 (in some embodiments about 1x10 12 cm' 2 to about 1x10 13 erm 2 ).
- Block S31 may, for example, comprise depositing SiC or carbon-doped silicon by chemical vapor deposition (CVD), epitaxial CVD or molecular beam epitaxy (MBE).
- CVD chemical vapor deposition
- MBE molecular beam epitaxy
- the concentration of carbon is equal in all parts of the interfacial layer.
- the deposition of carbon or carbon containing material to form the interfacial layer is patterned such that in some parts of the interfacial layer the carbon concentration is higher and in other parts of the interfacial layer the carbon concentration is lower. Such patterning may be applied to create a device in which the concentration of T centers varies with position in a plane of the device layer.
- T centers may be present with a desired concentration in selected areas of the device layer and not present or present in lower concentrations in other areas of the device layer.
- patterning of the deposition of carbon containing material in block S31 is achieved by masking or applying ligands to the silicon surface on which interfacial layer 23 is being applied.
- Block S33 a crystalline layer of silicon is formed on the interfacial layer.
- the thickness of the crystalline layer is 10 nm or more.
- Block S33 may, for example, comprise depositing silicon by chemical vapor deposition (CVD) or by molecular beam epitaxy (MBE).
- the structure output by block S33 is optionally subjected to a first annealing process.
- the first annealing process is a heat treatment process that allows carbon atoms to diffuse from the layer of carbon-containing material into the adjacent silicon. The carbon atoms can then occupy substitutional sites in the crystal lattice of the silicon (i.e. sites where silicon atoms are missing from the crystalline lattice).
- the first annealing process comprises heating the silicon layers to temperatures of at least 500°C. As carbon atoms diffuse into the adjacent layers of silicon, the concentration of carbon atoms at the interface between the adjacent layers of silicon is reduced.
- the first annealing process may comprise a rapid thermal annealing process in which temperature is rapidly ramped up to an annealing temperature, held at the annealing temperature for a short time and then rapidly reduced to below the annealing temperature.
- the first annealing process comprises applying a hold temperature of about 1000 °C for a hold time of less than 30 seconds.
- the first annealing process is conducted in an oxygen-free atmosphere.
- the carbon concentration within the silicon adjacent to the location of interfacial layer 23 is at least about 10 18 or 10 19 carbon atoms per cm 3 in order to promote formation of T centres in the silicon.
- the carbon atoms that diffuse outwardly from interfacial layer 23 form a band extending to either side of the location at which the layer of carbon containing material was deposited. In this band the carbon concentration is at least about 10 13 carbon atoms per cm 3 and may be about 10 18 or 10 19 carbon atoms per cm 3 .
- Block S37 introduces hydrogen into the silicon.
- the hydrogen may be introduced using techniques such as ion implantation or diffusion.
- the ion implantation is performed at about room temperature.
- the ion implantation has the effect of creating vacancies in the silicon lattice in which T centres may be formed and also supplying hydrogen which is required for making a T centre.
- the hydrogen is selectively supplied in some areas in the plane of the device layer and not in others (e.g., by performing the ion implantation through windows in a hard mask). Selectively implanting hydrogen in some areas of the device layer and not others is another way to control the resulting distribution of T centres in the device layer,
- a second annealing process is performed in block S39.
- the second annealing process is carried out in a temperature range that is lower than that of the first annealing process (if the first annealing process has been performed).
- the second annealing process comprises heating the silicon layers to temperatures of at least 400 °C.
- the second annealing process may, for example, involve heating the device or at least the device layer to a temperature in the range of 400 °C to 600 °C.
- the second annealing process of block S39 and the hydrogen introduction of block S37 are performed simultaneously or at overlapping times.
- the second annealing process is applied for a hold time of at least 60 seconds.
- the second annealing process is conducted in an oxygen-free atmosphere (e.g. in an inert gas atmosphere).
- the second annealing process facilitates hydrogen atoms bonding to carbon atoms at substitutional carbon sites and/or to interstitial carbon atoms which may migrate to substitutional carbon sites to form T centres.
- blocks S31 and S33 are repeated a desired number of times to add additional silicon layers having carbon containing material at interfaces between the silicon layers as indicated by loop S32. In some embodiments blocks S31 and S33 are each performed at least three times to create at least three interstitial layers of carbon containing material.
- Providing a plurality of thin interfacial layers of carbon containing material separated by thin crystalline silicon layers can facilitate providing a thicker region in which, after annealing, the carbon concentration is in a good range to yield T centres or G centres. Furthermore, providing a number of closely spaced interfacial layers 23 can yield a final carbon concentration that is more uniform with depth than could be readily achieved if only one interfacial layer 23 were provided. In some embodiments silicon layers separating adjacent interfacial layers 23 are 20 nm or less in thickness.
- Another advantage of providing multiple interfacial layers of carbon containing material separated by thin silicon layers is that the same or even a smaller density of carbon in the interfacial layers 23 can yield higher carbon densities in the silicon crystal after annealing than would be practical to achieve if only a single interfacial layer is provided.
- method 30 yields a device layer that includes T centres or G centres at depths of at least 50 nm or at least 70 nm or at least 100nm below a surface of the device layer.
- a surface of the device layer is etched in block S39A. The etching may be performed to enhance a quality of the surface of the device layer and/or to adjust a depth of the T centres relative to the surface.
- optical structures are formed in or on the device layer.
- the optical structures may, for example, comprise resonant structures such as photonic cavities that are tuned to enhance optical coupling to T centres in the device layer.
- the resonant structures may, for example, have a resonance at a photon wavelength that corresponds to an optical transition in an unpaired electron of a T centre.
- the optical structures may additionally comprise optical waveguides arranged to guide photons that are travelling to and from T centres.
- the optical structure may be created, for example, by applying silicon fabrication techniques such as selective etching to the device layer and/or by applying an optical device layer on the device layer.
- FIGs. 4A and 4B are examples of intermediate structures that are ready for the first annealing process of block S35. Each of these structures has a SOI configuration.
- FIG. 4A is a schematic cross sectional view of a device precursor 40A according to an example embodiment of this invention.
- FIG. 4B is a schematic cross sectional view of a device precursor 40B according to another example embodiment. Parts of device precursors 40A and 40B which are also present in SOI structure 20 of FIG. 2 are indicated with the same references used in FIG. 2.
- Device precursor 40A includes a device layer 26A.
- Device layer 26A comprises a plurality of sub-layers.
- Device layer 26A of device precursor 40A comprises a seed layer 21 fabricated on insulator layer 24, an interfacial layer 23 of a carbon containing material fabricated on seed layer 21 and a crystalline silicon layer 25 fabricated on interfacial layer 23. Interfacial layer 23 is sandwiched between seed layer 21 and crystalline silicon layer 25.
- device layer 26A has a thickness in the range of 100 to 500 nm.
- luminescent centres such as T centres are concentrated at a depth within device layer 26A that is equal to one half of the thickness of device layer 26A ⁇ 25%.
- FIG. 4B shows another example embodiment device precursor 40B.
- Device precursor 40B differs from substrate 40A in that an additional first crystalline layer 27 is fabricated on seed layer 21 and then interfacial layer 23 is fabricated on first crystalline layer 27 before another crystalline layer 25 is fabricated on interfacial layer 23.
- the first crystalline layer 27 may thus form an intermediate silicon layer.
- the thickness of crystalline layer 25 is at least equal to the combined thickness of seed layer 21 , first crystalline layer 27, and interfacial layer 23.
- An advantage of providing additional first crystalline layer 27 on seed layer 21 is to increase separation between interfacial layer 23 and seed layer 21 . This can reduce migration of unwanted isotopes from seed layer 21 into areas where luminescent centres such as T centres will be present.
- seed layer 21 comprises natural silicon (containing 29 Si which has a nuclear spin of 14) and it is desired to provide T centres in a body of silicon which is isotopically enriched with a silicon isotope that has zero nuclear spin (such as 28 Si)
- first crystalline layer 27 may be enriched in 28 Si.
- the presence of first crystalline layer 27 reduces the amount of unwanted isotopes from natural silicon (e.g.
- FIG. 40 shows another example embodiment device precursor 40C.
- Device precursor 400 differs from substrate 40A in that carbon rich silicon-based material such as SiC or carbon doped silicon is applied to seed layer 21 to form a carbon rich crystalline silicon layer 28. Seed layer 21 and carbon rich crystalline silicon layer 28 form device layer 260.
- carbon rich crystalline silicon layer 28 comprises isotopically enriched 28 Si.
- carbon rich crystalline silicon layer 28 is formed with a gradient of carbon concentration such that carbon has a concentration that is lower close to seed layer 21 and increases toward the face of carbon rich crystalline silicon layer 28 that is away from seed layer 21.
- FIG. 5 is a cross sectional view of an example device 40A that shows an example carbon concentration profile 47 within modified device layer 26A.
- concentration of carbon is represented by shading. Darker shading indicates a higher concentration and a lighter shading indicates a lighter concentration. Carbon concentration is the highest (shown with the darkest shade) at interfacial layer 23.
- FIG. 5 shows concentration of carbon outside of interfacial layer 23 in parts of seed layer 21 and crystalline layer 25 that are closest to interfacial layer 23, reflecting the migration/diffusion of carbon atoms during the annealing process.
- a carbon profile 47 of substrate 40A shows the carbon concentration at various depths within modified device layer 26A.
- Carbon doping profile 47 shows carbon concentration peaking at the depth corresponding to interfacial (dopant) layer 23 and falling off with distance away from interfacial layer 23.
- FIG. 6 shows another example carbon profile 57 within another example modified device layer 56 in a cross sectional view of another example device 50. Parts of device 50 which serve the same or similar functions in substrate 20 and precursor devices 40A and 40B are indicated with the same references as used in FIGs. 2-5.
- Device 50 differs from precursor devices 40A and 40B in that device layer 56 of substrate 50 has multiple interfacial layers 23 that alternate with crystalline layers 25.
- interfacial layers 23 are created by deposition of two- dimensional (i.e. very thin) carbon layers.
- interfacial layers 23 are created by deposition of two-dimensional carbon doped silicon layers.
- the alternate deposition of two-dimensional carbon layers (i.e. interfacial layers 23) and growth of crystalline layers 25 create a carbon-silicon superlattice structure.
- material of crystalline layers 25 is isotopically purified crystalline silicon-28.
- Carbon doping profile 57 shows multiple carbon concentration peaks corresponding to multiple interfacial layers 23A-C.
- First and second crystalline layers 25A and 25B have the highest carbon concentration in areas near the adjacent interfacial layers 23 and the carbon concentration tapers off towards approximately the centre of crystalline layers 25A and 25B.
- their lowest carbon concentration levels at approximately centre positions are still relatively high compared to areas in seed layer 21 and crystalline layer 25C that are the same distance or further away from their respective adjacent interfacial layers 23.
- a superlattice of alternating interfacial layers 23A-C separated by thin crystalline layers 25A-C in substrate 50 creates regions of comparatively constant carbon doping concentration in the silicon layers that are located between interfacial layers 23. Accordingly, in substrate 50, the spin-photon interfaces may be formed in layers at desired depths within modified silicon device layer 56.
- luminescent centres such as T centres
- the way in which luminescent centres, such as T centres, are distributed in a device created by the methods as described herein may be controlled by one or more of:
- a component e.g. a substrate, tool, device, optical element, etc.
- reference to that component should be interpreted as including as equivalents of that component any component which performs the function of the described component (i.e. , that is functionally equivalent), including components which are not structurally equivalent to the disclosed structure which performs the function in the illustrated exemplary embodiments of the invention.
- connection means any connection or coupling, either direct or indirect, between two or more elements; the coupling or connection between the elements can be physical, logical, or a combination thereof;
- the stated range includes all sub-ranges of the range. It is intended that the statement of a range supports the value being at an endpoint of the range as well as at any intervening value to the tenth of the unit of the lower limit of the range, as well as any subrange or sets of sub ranges of the range unless the context clearly dictates otherwise or any portion(s) of the stated range is specifically excluded. Where the stated range includes one or both endpoints of the range, ranges excluding either or both of those included endpoints are also included in the invention.
- the numerical value is in the range of C to D where C and D are respectively lower and upper endpoints of the range that encompasses all of those values that provide a substantial equivalent to the value 10
- Any recited method can be carried out in the order of events recited or in any other order which is logically possible.
- processes or blocks are presented in a given order, alternative examples may perform routines having steps, or employ systems having blocks, in a different order, and some processes or blocks may be deleted, moved, added, subdivided, combined, and/or modified to provide alternative or subcombinations.
- Each of these processes or blocks may be implemented in a variety of different ways.
- processes or blocks are at times shown as being performed in series, these processes or blocks may instead be performed in parallel, simultaneously or at different times.
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| Application Number | Priority Date | Filing Date | Title |
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| EP23901831.0A EP4612740A4 (en) | 2022-12-15 | 2023-12-05 | METHOD FOR PRODUCING SOLID DEVICES WITH SPIN-PHOTON INTERFACES |
| AU2023394105A AU2023394105A1 (en) | 2022-12-15 | 2023-12-05 | Methods for making solid state devices having spin-photon interfaces |
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| US202263387534P | 2022-12-15 | 2022-12-15 | |
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| WO2022020951A1 (en) * | 2020-07-28 | 2022-02-03 | Photonic Inc. | Storage and transduction of quantum information |
| GB202209944D0 (en) * | 2022-07-06 | 2022-08-17 | Univ Warwick | System for quantum information processing |
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| WO2021022375A1 (en) * | 2019-08-06 | 2021-02-11 | Photonic Inc. | Systems, devices, articles, and methods to interact with information stored in bound-exciton states associated with luminescent silicon defects |
| WO2022020951A1 (en) * | 2020-07-28 | 2022-02-03 | Photonic Inc. | Storage and transduction of quantum information |
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| WO2026028157A1 (en) * | 2024-08-01 | 2026-02-05 | Photonic Inc. | Qubit containing devices and methods for making same |
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| EP4612740A4 (en) | 2026-03-18 |
| EP4612740A1 (en) | 2025-09-10 |
| TW202440451A (en) | 2024-10-16 |
| AU2023394105A1 (en) | 2025-06-12 |
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