The disclosure pertains to semiconductor manufacturing, including manufacturing of wafers.
Modern semiconducting devices, such as processing circuits, memory devices, light detectors, solar cells, light-emitting semiconductor devices, devices that deploy complementary metal-oxide-semiconductor (CMOS) structures, and the like, are often manufactured on silicon wafers (or other suitable substrates). Wafers may undergo numerous processing operations, such as physical vapor deposition, chemical vapor deposition, etching, photo-masking, polishing, and/or various other operations. In a continuous effort to reduce the cost of semiconductor devices, multi-layer stacks of dies, insulating films, patterned and/or doped semiconducting films, and/or other features are often deposited on a single wafer, resulting in high aspect ratio devices, which are used, e.g., in 3D flash memory devices and other applications. Deposition, patterning, etching, polishing, etc., of stacks of multi-layered structures often result in significant stresses applied to the underlying wafers. Such stresses lead to both an out-of-plane distortion and an in-plane distortion of features supported by the wafers. These distortions result in misalignment of deposited features and can significantly degrade quality of manufactured devices.
The present disclosure will be understood more fully from the detailed description given below and from the accompanying drawings of various implementations of the disclosure.
In one embodiment, disclosed is a method that includes obtaining a first substrate supporting one or more transferred features (TFs) and transferring the one or more TFs from the first substrate to a second substrate. The method further includes transferring the one or more TFs from the first substrate to the second substrate. The method further includes applying stress mitigation to a target substrate, wherein the target substrate comprises at least one of the first substrate, an auxiliary substrate supporting the one or more TFs prior to transferring the one or more TFs from the auxiliary substrate to the first substrate, or the second substrate. Applying stress mitigation to the target substrate includes obtaining, using optical inspection data, an out-of-plane deformation (OPD) profile of the target substrate, causing a stress compensation layer (SCL) to be deposited on the target substrate, and exposing the SCL to a stress-mitigation beam Settings of at least one or more of (i) the SCL or (ii) the stress-mitigation beam are determined using the OPD profile of the target substrate.
In another embodiment, disclosed is a system that includes a memory and a processing device communicatively coupled to the memory. The processing device to cause performance of operations that include obtaining a first substrate supporting one or more TFs, transferring the one or more TFs from the first substrate to a second substrate, and applying stress mitigation to a target substrate. The target substrate is at least one of the first substrate, an auxiliary substrate supporting the one or more TFs prior to transferring the one or more TFs from the auxiliary substrate to the first substrate, or the second substrate. Applying stress mitigation to the target substrate includes obtaining, using optical inspection data, an OPD profile of the target substrate, causing an SCL to be deposited on the target substrate; and exposing the SCL to a stress-mitigation beam. Settings of at least one or more of (i) the SCL or (ii) the stress-mitigation beam are determined using the OPD profile of the target substrate.
In another embodiment, disclosed is a semiconductor manufacturing system that includes one or more processing chambers to process a substrate and a computing device. The computing device is to cause performance of operations that include obtaining a first substrate supporting one or more TFs, transferring the one or more TFs from the first substrate to a second substrate, and applying stress mitigation to a target substrate. The target substrate is at least one of the first substrate, an auxiliary substrate supporting the one or more TFs prior to transferring the one or more TFs from the auxiliary substrate to the first substrate, or the second substrate. Applying stress mitigation to the target substrate includes obtaining, using optical inspection data, an OPD profile of the target substrate, causing an SCL to be deposited on the target substrate; and exposing the SCL to a stress-mitigation beam. Settings of at least one or more of (i) the SCL or (ii) the stress-mitigation beam are determined using the OPD profile of the target substrate.
In yet another embodiment, disclosed is a non-transitory computer-readable memory storing instructions thereon that, when executed by a processing device, cause the processing device to cause performance of operations that include obtaining a first substrate supporting one or more TFs, transferring the one or more TFs from the first substrate to a second substrate, and applying stress mitigation to a target substrate. The target substrate is at least one of the first substrate, an auxiliary substrate supporting the one or more TFs prior to transferring the one or more TFs from the auxiliary substrate to the first substrate, or the second substrate. Applying stress mitigation to the target substrate includes obtaining, using optical inspection data, an OPD profile of the target substrate, causing an SCL to be deposited on the target substrate, and exposing the SCL to a stress-mitigation beam. Settings of at least one or more of (i) the SCL or (ii) the stress-mitigation beam are determined using the OPD profile of the target substrate.
Modern technology often aims to maximize chip area utilization by manufacturing three-dimensional devices having multiple layers of semiconducting structures. For example, in NAND flash memory devices, lateral relative arrangement (CMOS near Array, or CnA) of memory cells (e.g., floating gate transistors) and peripheral transistors (e.g., CMOS circuitry used to support write/read operations with memory cells) has mostly given way to a vertical arrangement (CMOS under Array, or CuA) in which peripheral CMOS circuitry is disposed below an array of memory cells. Deposition of memory cells on top of a previously deposited CMOS circuitry, however, limits the range of temperatures available for memory cell deposition since higher temperatures (e.g., 800-1200° C.) desired for efficient cell deposition can be detrimental for the integrity of the deposited CMOS circuitry. It is, therefore, advantageous to initially deposit memory cells on one wafer, e.g., wafer A, while depositing the peripheral circuitry on another wafer, e.g., wafer B, and then transfer memory cells from wafer A to wafer B, bonding the cells to the corresponding circuitry.
Patterning and/or depositing memory cells/CMOS circuitry, however, can cause stress in wafer A and/or wafer B, which induces deformation in the respective wafer(s), e.g., a parabolic deformation, a cylindric deformation, a saddle deformation, or some more complicated deformation, and/or a combination thereof. Deformation of the wafers makes alignment of various features deposited/etched/patterned on the wafers difficult. This results in an increase of sub-optimally processed wafers and a corresponding decrease in the yield of the manufacturing process.
Existing technology includes a number of methods that address wafer deformation. For example, a deformed (warped) wafer with various films and features deposited on one side (referred to as the front side, top side, or main side herein) can be coated on the other side (referred to as the back side or bottom side herein) with a film that exerts a compression stress or tensile stress on the wafer. Such a back side-deposited deformation-correcting film, also referred to as a stress-compensation layer herein, usually imparts a uniform (or global) stress to the entire wafer and cannot compensate for local stress modulation and/or anisotropic stress. Additional correction can be achieved by implanting ions into the stress-compensation layer, e.g., using a beam of ions to bombard the stress-compensation layer, to adjust the stress in the stress-compensation layer and, consequently, to further mitigate the deformation of the underlying wafer.
A “wafer,” as used herein, refers to any substrate or material surface formed on a substrate upon which film processing is performed during a fabrication process. For example, a wafer surface on which processing can be performed includes materials such as silicon, silicon oxide, silicon nitride, strained silicon, silicon on insulator, carbon doped silicon oxides, amorphous silicon, doped silicon, germanium, gallium arsenide, glass, sapphire, and any other materials such as metals, metal nitrides, metal alloys, and other conductive materials, depending on the application. Wafers include, without limitation, semiconductor wafers. In some instances, wafers can include plastic substrates. Wafers may be exposed to a pretreatment process to polish, etch, reduce, oxidize, hydroxylate, anneal, UV cure, e-beam cure and/or bake the substrate surface. In addition to film processing directly on the surface of the wafer itself, any of the film processing steps disclosed may also be performed on an underlayer formed on the wafer as disclosed in more detail below, and the term “wafer surface” is intended to include such underlayer as the context indicates. Thus, for example, where a film/layer or partial film/layer has been deposited onto a wafer surface, the exposed surface of the newly deposited film/layer becomes the wafer surface. In some embodiments, wafers have a thickness in the range of 0.25 mm to 1.5 mm, or in the range of 0.5 mm to 1.25 mm, in the range of 0.75 mm to 1.0 mm, or more. In some embodiments, wafers have a diameter of about 10 cm, 20 cm, 30 cm, or more.
Deposition of stress-compensation layers with ion implantation can be quite efficient in correcting stresses that are uniform and isotropic, σxx≈σyy. On the other hand, mitigating stresses that vary with location x, y on the wafer, σjk (x,y), stresses that are anisotropic, σxx≠σyy, or both is a much more challenging problem. Certain feature patterns can result in stresses that are compressive along one direction, e.g., σxx>0, and tensile along a perpendicular direction, σyy<0, resulting in saddle-shaped wafers, e.g., as illustrated in
Aspects and implementations of the present disclosure address these and other challenges of the modern semiconductor manufacturing technology by providing for systems and techniques that can mitigate non-uniform and/or anisotropic stresses and deformations (e.g., out-of-plane deformations) of wafers prior to wafer-on-wafer bonding. In some embodiments, a wafer's deformation can be measured (e.g., using optical measurements techniques) and parameters of a stress-compensation layer (e.g., layer's material, thickness, etc.) can be determined such that the sign of the stress is the same throughout the wafer. For example, if the wafer's deformation is concave, the parameters of the stress-compensation layer can be selected to overcorrect the wafer into a convex shape. An ion implantation map (a distribution of local doses of ion implants) n(x,y) can then be computed to reduce the local stress in the wafer to a degree that brings the convex shape to a flat (or nearly flat) shape. A number of techniques may be used to determine optimal ion implantation maps.
In some embodiments, a vertical profile of wafer deformation z=h({right arrow over (r)}) can be measured using optical metrology (e.g., optical interferometry) techniques. The wafer profile h({right arrow over (r)}) can then be represented via a number of parameters that qualitatively and quantitatively characterize geometry of the wafer deformation, e.g., a set of Zernike (or a similar set of) polynomials, h({right arrow over (r)})=Σj AjZj({right arrow over (r)}). Consecutive coefficients A1, A2, A3, A4 . . . represent weights of specific geometric features (elemental deformations) of the wafer described by the corresponding Zernike polynomials Zj({right arrow over (r)}). In some embodiments, a material of stress-compensation layer (e.g., a tensile or compressive film) can be selected based on the sign of a paraboloid bow coefficient coefficient A4. In some embodiments, selection of a thickness d of a stress-compensation layer can be made based on a value of the paraboloid bow coefficient A4. The stress-compensation layer can be deposited using any suitable deposition techniques including physical vapor deposition (e.g., sputtering), chemical vapor deposition (e.g., plasma-assisted deposition), epitaxy, exfoliation, and/or the like. Deposition can be performed at room temperature or at temperatures different from room temperature (e.g., at an elevated temperature). In some embodiments, thickness d of stress-compensation layer can be selected to overcorrect the deformation to some degree. The overcorrection can be chosen in conjunction with the implant species, energy, and dose to ensure maximum effect from the stress compensation. Stress in the combined structure of the wafer and the stress-compensation layer can be further controlled by an ion implantation beam that strikes the stress-compensation layer and deposits ions therein. Substitution defects and/or vacancies created by the beam of ions modify (e.g., reduce) stress in the stress-compensation layer and can reduce the degree of stress overcorrection caused by the film deposition. This causes the combination of the wafer and the stress-compensation layer to flatten.
In some embodiments, the number of ions deposited per various areas of the wafer can be determined using simulations, e.g., Monte Carlo simulations. The Monte Carlo simulations can be performed for a film made of the actual material used in deposition and having a specific thickness d. An initial Monte Carlo simulation can be performed for specific baseline (default) conditions of the ion implantation (e.g., default settings of an ion implantation apparatus). The baseline conditions can include a default type of ions, a default energy of ions, a default dose of ions to be imparted to the film (e.g., a default velocity of scanning and a default scanning pattern), and the like. The baseline conditions can subsequently be modified (e.g., optimized) using the Monte Carlo simulations. The Monte Carlo simulations can use measurement data (calibration data) collected for actual ion implantation performed for various ion energies, types of ions, types and materials of deposition films, angles of ion incidence on the films, and/or the like.
In some embodiments, the implantation map n({right arrow over (r)}) can be computed using an influence function G({right arrow over (r)}; {right arrow over (r)}′) that characterizes a response (e.g., deformation) at a point {right arrow over (r)} of the wafer as caused by a point-like force applied at another point {right arrow over (r)}′ of the wafer. In some embodiments, the influence function G({right arrow over (r)}; {right arrow over (r)}′), also known as the Green's function, can be determined from computational simulations or from analytical calculations. In some embodiments, the implantation map n({right arrow over (r)}) can be determined by accessing a stored dataset that includes a representation of the influence function G({right arrow over (r)}; {right arrow over (r)}′) for the target wafer and performing a regression computation to determine, based on the deformation of the target wafer and using G({right arrow over (r)}; {right arrow over (r)}′), a distribution of ion implants into the SCL. In some embodiments, the influence function can be determined from one or more experiments, which can include performing ion implantation into a film deposited on a reference wafer.
In some embodiments, wafer deformation h({right arrow over (r)})=hquad({right arrow over (r)})+hres({right arrow over (r)}) can be represented (decomposed) as a combination of a quadratic hquad ({right arrow over (r)}) and residual (non-quadratic) hres({right arrow over (r)}) contributions. The quadratic deformation can include a parabolic (paraboloid) part hpar(r), which has the complete axial symmetry, and a saddle part hsaddle({right arrow over (r)}). The thickness of the stress-compensation layer d can be computed (or empirically determined) in such a way that the layer is to apply a desired target stress to the back side of the wafer. To eliminate a non-uniform saddle deformation, the stress-compensation film can be of such thickness/material that turn the saddle deformation into a cylindric deformation having a definite sign throughout the entire area of the wafer. The uniform-sign cylindric deformation (as well as a residual higher-order non-quadratic deformation) can then be mitigated with ion implantation into the film. In some embodiments, a cylindric decomposition is not unique and can be either positive (upward-facing cylinder deformation) or negative (downward-facing cylinder deformation). Both decompositions can be analyzed and a decomposition that enables a more effective stress mitigation can be selected. For example, a decomposition that is characterized by a smaller parabolic bow deformation can be selected. The parabolic bow deformation can be mitigated using a film deposition while the remaining cylindric deformation (and the higher-order residual deformation) can be addressed by appropriately selected ion implantation doses n({right arrow over (r)}).
In some embodiments, mitigation of a cylindric deformation or a saddle deformation can include identifying principal axes (directions) of the cylinder/saddle and a magnitude of the cylindric/saddle deformation and depositing ions into appropriately selected edge regions of the stress-compensation layer. For example, the edge regions of the SCL can have a width that is at or below 30% of a diameter of the target wafer. Residual higher-order (ripple) deformations can then be mitigated with further ion implantation assist features into the area of the film.
In some embodiments, the stress-mitigation beam can delivering, to the SCL, a spatially uniform dose of ions, a radially-varying dose of ions, and/or an azimuthally-varying dose of ions
These and/or similar techniques can be applied, as part of a wafer-to-wafer bonding process, to stress mitigation of wafer A, wafer B, or both. In some embodiments, these or similar techniques can be applied to any additional (e.g., auxiliary or carrier) wafer that is used in the bonding process. For example, an initial wafer with any set of features (e.g., dies with memory cells) can be manufactured and subsequently cut into individual dies that are placed on a carrier wafer (reconstituted wafer A) before being transferred to wafer B. In such instances, the disclosed stress-mitigation techniques can be applied to the initial wafer A, the carrier wafer A, and/or receiving wafer B. Features and techniques described in conjunction with any of
Some of these techniques will now be described in more detail. In one embodiment, a vertical profile of wafer deformation z=h({right arrow over (r)}) can be measured using optical metrology techniques. For example, an interferogram of the profile h({right arrow over (r)}) can be obtained using optical interferometry measurements. The wafer profile h({right arrow over (r)}) can then be represented via a number of parameters that qualitatively and quantitatively characterize geometry of the wafer deformation. In some embodiments, a set of Zernike (or a similar set of) polynomials may be used to represent the wafer profile,
where the planar radius-vector {right arrow over (r)}=(r,ϕ) may be represented as the radial coordinate r and the polar angle ϕ within the (average) plane of the wafer. Consecutive coefficients A1, A2, A3, A4 . . . represent weights of specific geometric features (elemental deformations) of the wafer described by the corresponding Zernike polynomials Z1(r,ϕ), Z2(r,ϕ), Z3(r,ϕ), Z4(r,ϕ) . . . . (Herein, the Noll indexing scheme for the Zernike polynomials is being used.) The first three coefficients are of less interest as they describe a uniform shift of the wafer (coefficient A1, associated with the Z1(r,ϕ)=1 polynomial), a deformation-free x-tilt that amounts to a rotation around the y-axis (coefficient A2, associated with the Z2(r,ϕ)=2r cos 0 polynomial), and a deformation-free x-tilt that amounts to a rotation around the x-axis (coefficient A3, associated with the Z3(r,ϕ)=2r sin 0 polynomial) that can be eliminated by a realignment of the coordinate axes. The fourth coefficient A4 is associated with Z4(r,ϕ)=√{square root over (3)}(2r2−1) and characterizes an isotropic paraboloid deformation (“bow”). The fifth A5 and the sixth A6 coefficients are associated with Z5 (r,ϕ)=√{square root over (6)}r2 sin 2ϕ and Z6(r,ϕ)=√{square root over (6)}r2 cos 2ϕ polynomials, respectively, and characterize a saddle-type deformation. The A5 coefficient characterizes a saddle shape that curves up (A5>0) or down (A5<0) along the diagonal y=x and curves down (A5>0) or up (A5<0) along the diagonal y=−x. The A6 coefficient characterizes a saddle shape that curves up (A6>0) or down (A6<0) along the x-axis and curves down (A6>0) or up (A6<0) along the y-axis. The higher coefficients A7, A8, etc., characterize progressively faster variations of the wafer deformation h(r,ϕ) along the radial direction, along the azimuthal direction, or both and collectively represent a residual deformation, hres(r,ϕ)=h(r,ϕ)−Σj=46AjZj(r,ϕ).
In some embodiments, selection of a thickness d of the stress-compensation film can be made based on a value of the paraboloid bow coefficient A4.
A material (type) of stress-compensation layer 108 can be selected based on the sign of coefficient A4. For example, for a negative bow, A4<0, and stress-compensation layer 108 can be selected to have a compressive stress (as illustrated in
The overcorrection is chosen in conjunction with the implant species, energy, and dose to ensure maximum entitlement from the stress compensation. The overcorrection makes the combined structure of wafer 102 and stress-compensation layer 108 susceptible to further control of stress (and thus deformation of the wafer hcorr(r,ϕ)). As illustrated in
Although, for the sake of specificity, a stress-mitigation beam that is used to modify the stress in stress-compensation layer 108 is referred to as ion beam (e.g., ion beam 112) throughout this disclosure, the stress-mitigation beam (irradiation) can include other matter particles (e.g., electrons), electromagnetic waves (e.g., UV light, visible light, infrared light, etc.), and/or a suitable combination thereof. The stress-mitigation beam strikes stress-compensation layer 108 and changes the bonding network of stress-compensation layer 108. For example, the stress-mitigation beam of low energy may interact with surface atoms of stress-compensation layer 108, e.g., removing some of the surface atoms, effectively implementing etching of surface regions of stress-compensation layer 108. The effectiveness of such etching may be controlled by a choice of ion species/radicals/ambient gasses. In another example, the stress-mitigation beam of high energy can deposit ions inside stress-compensation layer 108. Ions and/or photons can break bonds of the bonding network (or crystal lattice) of stress-compensation layer 108 forming vacancies therein, and can further cause annealing due to local heating, UV curing, and/or other effects.
In some embodiments, the number of ions ΔNj deposited per small area ΔA=ΔxΔy of the wafer may be determined using simulations (performed as described in more detail below) based on the local value of the corrected deformation hcorr(r,ϕ), which may include a saddle deformation, a residual deformation, and the part of the paraboloid bow deformation Acorr(d)+A4 that has been overcorrected by the deposition of stress-compensation layer 108. The desired local density n(x,y)=ΔNi/ΔxΔy of the ions can be delivered by controlling the scanning velocity v of ion beam 112. In some embodiments, ion beam 112 has a profile that can be approximated with a Gaussian function, e.g., the ion flux j(φ)=j0 exp(−x2/a2−y2/b2), where x and y are Cartesian coordinates, j0 is the maximum ion flux at the center of the beam, and a and b is are characteristic spreads of the beam along the x-axis and y-axis, respectively. Correspondingly, a point that is located at distance y from the path of the center of the beam receives an ion dose that includes the following number of ions:
Correspondingly, by reducing the scanning velocity v, the number of ions received by various regions of stress-compensation layer 108 can be increased, and vice versa. Additionally, ion beam 112 can perform multiple scans with different offsets y so that various points of stress-compensation layer 108 receive multiple doses of ions with different factors e−y2/b2 that can average to a target dose. For example, after n passes of ion beam implanter 110, each made with a respective velocity vk at a different distance yk from the center of ion beam 112 to the area ΔxΔy, the total dose of ions received by this area will be
As illustrated in
The techniques of strain and deformation mitigation illustrated in
This structure of the stress tensor is usually a good approximation since the wafer is typically in a state of pure bending and independent of the shear stresses that are represented by the off-diagonal terms in the stress tensor. Correction of the saddle shape requires special handling in the computation of the dose map and optimization to ensure that additional residual terms are not introduced into the wafer as a result.
At block 610, process 600 includes obtaining wafer A, which can be any wafer that is used in any suitable wafer-to-wafer bonding process, e.g., a silicon wafer, a glass wafer, a gallium arsenide wafer, a gallium nitride wafer, a silicon carbide wafer, a corundum wafer, and/or the like. Wafer A can have any features manufactured thereon that are to be transferred to wafer B, and which are referred to as transferred features (TFs) herein. For example, TFs can include dies with memory cells, logic circuits, optical circuits (e.g., photonic circuits), optoelectronic circuits, multiplexing/switching fabrics, and/or the like. In some embodiments, dies (or other TFs) can be deposited, etched, patterned, grown, and/or otherwise manufactured directly on wafer A.
In some embodiments, TFs can first be manufactured on a different-initial-wafer, as indicated with block 602. In some embodiments, initial wafer with TFs can undergo, at block 604, wafer stress mitigation (as discussed below in conjunction with process 650) followed by a transfer of TFs to wafer A, which serves as a carrier wafer (block 606). For example, TFs can be prepared on the initial wafer and subsequently cut into individual pieces (e.g., dies) that are then placed on carrier wafer A. The placed TFs can be bonded, adhered, or otherwise secured on carrier wafer A.
Referring again to
At block 630, process 600 includes obtaining wafer B, which can (similarly to wafer A) be any suitable wafer. Wafer B can have any features manufactured thereon that are to be matched to TFs transferred from wafer B, herein referred to as receiving features (RFs) of wafer B. For example, RFs can include any circuits (e.g., CMOS peripheral circuits), patterning, and/or the like.
In some instances, wafer A (with any number of features deposited, etched, and/or otherwise engineered thereon) can be adhered (bonded) to wafer B. In such instances, wafer A serves as carrier wafer (initial wafer) but remains adhered to wafer B (rather than serving as a carrier wafer to transferred features).
Referring again to
Referring again to
Stress mitigation of initial wafer (block 604), carrier wafer (block 620), wafer B (block 640 and/or block 670), and/or the like, can be performed using one or more operations of process 650.
More specifically, at block 651, a shape of a wafer (initial wafer, carrier wafer A, wafer B, etc.) can be measured. A displacement hw({right arrow over (r)}) of a surface (e.g., top surface or bottom surface) of the wafer can be represented as a function of radius-vector {right arrow over (r)} using any suitable set of in-plane coordinates, e.g., polar coordinates, hw(r,ϕ), Cartesian coordinates, hw(x,y), or any other coordinates. In some embodiments, wafer deformation hw({right arrow over (r)}) can be represented via a decomposition of the determined shape over a suitable set of basis functions, e.g., Zernike polynomials, or some other set of polynomials. The wafer deformation hw({right arrow over (r)}) can be caused by a deforming pressure applied to the top surface of the wafer as a result of local stresses caused by patterning/etching of the wafer, deposition of one or more films on the top surface of the wafer, and/or any other technological operations performed on the wafer.
At block 652, the determined deformation hw({right arrow over (r)}) can be used to identify properties (e.g., material and thickness) of a target stress-compensation film to be deposited on the wafer. In some implementations, the film can be selected in such as a way as to make the stress σWF in the new wafer/film structure of a definite sign. In the example of
At block 653 of
The measured (and/or estimated) deformation hWF({right arrow over (r)}) of the wafer can be used to determine a ion implantation dose map n({right arrow over (r)}) that mitigates the stress σWF({right arrow over (r)}) and reduces deformation to zero (or near zero), hWF({right arrow over (r)})→0. Non-uniform ion implantation causes the uniform pressure exerted by the film to be reduced by an amount determined by a properly chosen local ion dose n({right arrow over (r)}).
Operations of block 655 can include one or more techniques to determine n({right arrow over (r)}). In some embodiments, ion implantation map n({right arrow over (r)}) can be computed using statistical, e.g., Monte Carlo simulations. For example, stored measurement data can be collected from previously (e.g., historically) performed measurements of ion multiple types of SCL materials, thicknesses of SCLs, types of particles (e.g., photons, electrons, ions of various types, etc.), angles of incidence, and/or other parameters. The stored measurement data can be statistically processed and stored (e.g., in a memory of a processing device performing the Monte Carlo simulations) in the form of probability distributions of various quantities, e.g., distribution of the density of ion implantation with depth for different ion types, ion energies, angles of incidence, distribution of the number of vacancies produced at different depths (per unit of length of travel of the ions) for different ion types, ion energies, and angles of incidence, distribution of stresses created by implanted ions for different densities of ion implantation and/or the number of produces vacancies, and/or the like. Performing the Monte Carlo simulation can include sampling from the stored statistical distributions and identifying a likelihood that a target stress mitigation will be achieved with various specific settings of SCL and/or stress-mitigation beam (e.g., ion beams).
In some embodiments, ion implantation map n({right arrow over (r)}) can be computed using cylindric decomposition of hWFV({right arrow over (r)}). In some embodiments, ion implantation map n({right arrow over (r)}) can be computed for selected edge regions of the stress-compensation layer (e.g., to mitigate a cylindric deformation or a saddle deformation) and, optionally, using assist feature-based ion implantation assist features into the area of the film (e.g., to mitigate a residual non-quadratic wafer deformation). In some embodiments, the implantation map n({right arrow over (r)}) can be computed using an influence function G({right arrow over (r)}; {right arrow over (r)}) that can be analytically computed, experimentally measured, and/or determined using computational simulations. In some embodiments, a combination of multiple techniques of ion implantation computations can be used.
Operations of ion implantation system 1000 can be controlled by a controller 1014, which can include any suitable computing device, microcontroller, or any other processing device having a processor, e.g., a central processing unit (CPU), a field-programmable gate array (FPGA), an application-specific integrated circuit (ASIC), and/or the like, and a memory device, e.g., a random-access memory (RAM), read-only memory (ROM), flash memory, and/or the like or any combination thereof. Controller 1014 can control operations of power source 1006, support stage 1012, and/or various other components and modules of ion implantation system 1000. Controller 1014 can include an ion beam simulation module 1016 capable of performing simulations that determine a target intensity of ion beam 112 to be used to mitigate various wafer deformations. In some embodiments, support stage 1012 can impart a tilt, e.g., in one or two spatial directions to wafer 102 to change an angle of incidence of ion beam 112 relative to wafer 102. In some embodiments, instead of tilting wafer 102, controller 1014 can cause a tilt of ion implantation system 1000 relative to wafer 102.
Example computer system 1100 may include a processing device 1102 (also referred to as a processor or CPU), a main memory 1104 (e.g., read-only memory (ROM), flash memory, dynamic random access memory (DRAM) such as synchronous DRAM (SDRAM), etc.), a static memory 1106 (e.g., flash memory, static random access memory (SRAM), etc.), and a secondary memory (e.g., a data storage device 1118), which may communicate with each other via a bus 1130.
Processing device 1102 represents one or more general-purpose processing devices such as a microprocessor, central processing unit, or the like. Processing device 1102 can include processing logic 1126. Processing device 1102 may be a complex instruction set computing (CISC) microprocessor, reduced instruction set computing (RISC) microprocessor, very long instruction word (VLIW) microprocessor, processor implementing other instruction sets, or processors implementing a combination of instruction sets. Processing device 1102 may also be one or more special-purpose processing devices such as an application specific integrated circuit (ASIC), a field programmable gate array (FPGA), a digital signal processor (DSP), network processor, or the like. In accordance with one or more aspects of the present disclosure, processing device 1102 may be configured to execute instructions implementing example process 600 of wafer-to-wafer bonding that deploys stress compensation layer deposition and ion implantation.
Example computer system 1100 may further comprise a network interface device 1108, which may be communicatively coupled to a network 1120. Example computer system 1100 may further comprise a video display 1110 (e.g., a liquid crystal display (LCD), a touch screen, or a cathode ray tube (CRT)), an alphanumeric input device 1112 (e.g., a keyboard), a cursor control device 1114 (e.g., a mouse), and an acoustic signal generation device 1116 (e.g., a speaker).
Data storage device 1118 may include a computer-readable storage medium (or, more specifically, a non-transitory computer-readable storage medium) 1124 on which is stored one or more sets of executable instructions 1122. In accordance with one or more aspects of the present disclosure, executable instructions 1122 may comprise executable instructions implementing example process 600 of wafer-to-wafer bonding that deploys stress compensation layer deposition and ion implantation.
Executable instructions 1122 may also reside, completely or at least partially, within main memory 1104 and/or within processing device 1102 during execution thereof by example computer system 1100, main memory 1104 and processing device 1102 also constituting computer-readable storage media. Executable instructions 1122 may further be transmitted or received over a network via network interface device 1108.
While the computer-readable storage medium 1124 is shown in
Some portions of the detailed descriptions above are presented in terms of algorithms and symbolic representations of operations on data bits within a computer memory. These algorithmic descriptions and representations are the means used by those skilled in the data processing arts to most effectively convey the substance of their work to others skilled in the art. An algorithm is here, and generally, conceived to be a self-consistent sequence of steps leading to a desired result. The steps are those requiring physical manipulations of physical quantities. Usually, though not necessarily, these quantities take the form of electrical or magnetic signals capable of being stored, transferred, combined, compared, and otherwise manipulated. It has proven convenient at times, principally for reasons of common usage, to refer to these signals as bits, values, elements, symbols, characters, terms, numbers, or the like.
It should be borne in mind, however, that all of these and similar terms are to be associated with the appropriate physical quantities and are merely convenient labels applied to these quantities. Unless specifically stated otherwise, as apparent from the following discussion, it is appreciated that throughout the description, discussions utilizing terms such as “identifying,” “determining,” “storing,” “adjusting,” “causing,” “returning,” “comparing,” “creating,” “stopping,” “loading,” “copying,” “throwing,” “replacing,” “performing,” or the like, refer to the action and processes of a computer system, or similar electronic computing device, that manipulates and transforms data represented as physical (electronic) quantities within the computer system's registers and memories into other data similarly represented as physical quantities within the computer system memories or registers or other such information storage, transmission or display devices.
Examples of the present disclosure also relate to an apparatus for performing the methods described herein. This apparatus may be specially constructed for the required purposes, or it may be a general purpose computer system selectively programmed by a computer program stored in the computer system. Such a computer program may be stored in a computer readable storage medium, such as, but not limited to, any type of disk including optical disks, CD-ROMs, and magnetic-optical disks, read-only memories (ROMs), random access memories (RAMs), EPROMs, EEPROMs, magnetic disk storage media, optical storage media, flash memory devices, other type of machine-accessible storage media, or any type of media suitable for storing electronic instructions, each coupled to a computer system bus.
The methods and displays presented herein are not inherently related to any particular computer or other apparatus. Various general purpose systems may be used with programs in accordance with the teachings herein, or it may prove convenient to construct a more specialized apparatus to perform the required method steps. The required structure for a variety of these systems will appear as set forth in the description below. In addition, the scope of the present disclosure is not limited to any particular programming language. It will be appreciated that a variety of programming languages may be used to implement the teachings of the present disclosure.
It is to be understood that the above description is intended to be illustrative, and not restrictive. Many other embodiment examples will be apparent to those of skill in the art upon reading and understanding the above description. Although the present disclosure describes specific examples, it will be recognized that the systems and methods of the present disclosure are not limited to the examples described herein, but may be practiced with modifications within the scope of the appended claims. Accordingly, the specification and drawings are to be regarded in an illustrative sense rather than a restrictive sense. The scope of the present disclosure should, therefore, be determined with reference to the appended claims, along with the full scope of equivalents to which such claims are entitled.
This application claims the benefit of U.S. Provisional Patent Application No. 63/444,158, filed Feb. 8, 2023, entitled “Mitigation of stress and deformation in wafers”; U.S. Provisional Patent Application No. 63/491,170, filed Mar. 20, 2023, entitled “Optimized film deposition and ion implantation for mitigation of stress and deformation in wafers”; U.S. Provisional Patent Application No. 63/502,447, filed May 16, 2023, entitled “Mitigation of saddle deformation of wafers using film deposition and edge ion implantation”; U.S. Provisional Patent Application No. 63/502,448, filed May 16, 2023, entitled “Influence function-based mitigation of wafer deformation with film deposition and ion implantation”; U.S. Provisional Patent Application No. 63/502,452, filed May 16, 2023, entitled “Cylindric decomposition for efficient mitigation of wafer deformation with film deposition and ion implantation”; and U.S. Provisional Patent Application No. 63/511,414, filed Jun. 30, 2023, entitled “Wafer stress management for precise wafer-to-wafer bonding,” the contents of which are incorporated by reference in their entirety herein.
Number | Date | Country | |
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63444158 | Feb 2023 | US | |
63511414 | Jun 2023 | US | |
63491170 | Mar 2023 | US | |
63502447 | May 2023 | US | |
63502448 | May 2023 | US | |
63502452 | May 2023 | US |