The field of the invention generally relates to methods for forming stressed (e.g., compressive of tensile) thin films. More particularly, the field of the invention relates to methods used to form dislocation-free stressed thin films.
The use of strained silicon devices is known to increase semiconductor device performance. For example, in the context of transistors, strained silicon increases the transistor drive current which improves switching speed by making current flow more smoothly. Generally, a very thin layer of single-crystal silicon with built in stress (or strain) improves drive current making the devices run faster. When the layer of silicon is under stress, the silicon lattice lets electrons and holes flow with less resistance. For transistors, the lower resistance translates in to faster switching properties, thereby permitting semiconductor devices to operate at faster speeds.
Because of the advantages inherent in the strained lattice structure, strained silicon or silicon germanium based devices have become an attractive alternative to current microelectronic devices that are composed of a silicon channel layer on a silicon substrate. Several approaches have been developed to form strained silicon on substrates. For example, relaxed silicon germanium buffer layers have been employed as a “virtual substrate” to grow strained silicon. Typically, the relaxed silicon germanium buffer layer, which has a higher lattice constant than the silicon substrate, is formed in a graded manner and is used as an epitaxial growth template.
If a constant (i.e., non-graded composition) silicon germanium buffer layer is used, high densities of dislocations nucleate during growth and interact with one another. This interaction prevents dislocations from propagating to the edge of the substrate (e.g., a wafer), thereby leaving a significant number of threading arms on the surface of the silicon germanium layer. In contrast, by grading the germanium composition during growth of the relaxed silicon germanium layer on a silicon substrate, the nucleation rate of dislocations is retarded by reducing the strain accumulation rate. Consequently, the interaction between dislocations is reduced, significantly reducing the density of threading arm dislocations on the surface of the silicon germanium layer. For example, the threading dislocation density in a constant (non-graded) silicon germanium grown directly on a silicon substrate is on the order of about 108˜9/cm2. If a graded silicon germanium buffer layer is formed on a silicon substrate, the threading dislocation density improves to around 104˜5/cm2.
Unfortunately, there are several disadvantages to graded silicon germanium buffer layers. First, the threading dislocation density, while lower in graded buffer layers, is still non-zero, which leads to degradation of electron and hole mobility. Moreover, a large thickness of graded silicon germanium buffer layer is needed for achieving low threading dislocation densities. The large thickness increases the size of the devices as well as the cost of production. Second, the strain-relaxed graded silicon germanium buffer layer has a rough surface which degrades the mobility of strained silicon. In addition, the strain at the top layer of silicon is not homogeneous due to the stress fields from buried dislocations, which also adversely affects carrier transport.
Another problem with existing techniques is that the stressed thin films have lattice constants at discrete values due to the availability of limited types of substrates along the spectrum of potential lattice constant values. It would be beneficial if the lattice constant could be varied or modified, to some extent, to expand the coverage of total available spectrum of lattice constants. In this regard, by expanding the universe of potential lattice constants would enable the creation of microelectronic devices within unique and advantageous properties.
In a first aspect of the invention, a method of forming a stressed thin film on a substrate includes the steps of depositing a thin crystalline film of silicon on a first substrate, and subsequently transforming the first substrate into a porous substrate via an electrochemical process. The porous substrate containing the thin film of silicon is then transformed into a stressed state such that at least a portion of the stress is transferred to the thin film. The thin film may be under compressive stress or tensile stress. For example, volumetric expansion of the porous substrate imparts tensile stress to the thin film while volumetric contraction of the porous substrate imparts compressive stress to the thin film. The porous substrate containing the stressed thin film of silicon is then bonded to a second substrate. The porous substrate is removed so as to deposit the stressed thin film of silicon to the second substrate.
In another aspect of the invention, a method of forming a stressed semiconductor thin film on a substrate includes the steps of providing a porous substrate that includes an oxide layer disposed thereon. The porous substrate is then bonded to a transfer substrate formed from a semiconducting material. A portion of the transfer substrate is removed so as to leave a semiconductor thin film on the porous substrate. The porous substrate containing the semiconductor thin film is transformed so as to form a stressed semiconductor thin film. The porous substrate containing the stressed semiconductor thin film is bonded to a recipient substrate. The porous substrate is then removed along with the oxide layer to expose the stressed semiconductor thin film on the recipient substrate.
In still another aspect of the invention, an article of manufacture includes a substrate, an intermediate layer disposed on the substrate, and a stressed thin film overlying the intermediate layer. The stressed thin film is formed from a semiconductor material and is homogeneously stressed across substantially the entire surface of the substrate. The stressed thin film is formed on a first, separate substrate that is subsequently transferred to a second, final substrate.
In step 110, an un-doped epilayer 14 of silicon is formed on the doped, p+ type silicon substrate 12. Alternatively, n-type silicon may be used for the epilayer 14. The epilayer 14 may be grown or deposited using a chemical vapor deposition (CVD) process or other epitaxial growth process. The thickness of the epilayer 14 may vary but generally is below around 100 nm. The thickness of the epilayer 14 should fall below the critical thickness at which dislocations are generated. The critical thickness may vary as a function of temperature and strain. Generally, the operating range for the thickness of the epilayer 14 should fall below the thickness/strain curve of so-called metastable silicon at any given temperature. In other words, the critical thickness is the thickness of the epilayer 14 at which the homogeneous strain energy becomes so large that misfit dislocations are introduced. The calculated critical layer thickness of latticed mismatched stressed heterostructures may be obtained using the methods illustrated in R. People at al., Calculation of Critical Layer Thickness Versus Lattice Mismatch For GexSi1-x/Si Strained-Layer Heterostructures, Applied Physics Letters, Vol. 47, p. 322-24 (1985).
Next, as illustrated in step 120, the doped, p+ silicon substrate 12 is transformed into porous silicon 16. This process may be carried out by placing the p+ silicon substrate 12 with the epilayer 14 into an anodization cell 70 of the type disclosed in
The anodization process taking place within the anodization cell 70 transforms the doped, p+ silicon substrate 12 into porous silicon 16. Anodization of the doped, p+ silicon substrate 12 is stopped when the advancing anodization front reaches the interface with the epilayer 14. During the anodization process at constant applied current, the measured voltage drop as a function of time stabilizes once the advancing anodization front reaches the interface substrate 12 and the epilayer 14. At this point, the anodization process is stopped and the porous silicon substrate 16 is removed from anodization cell 70.
In one aspect of the invention, the porous silicon 16 has a substantially uniform distribution of pores throughout the entire thickness of the porous silicon 16. That is to say, the pore size and pore distribution are substantially uniform across the entirety of the porous silicon 16. This feature of the invention permits subsequent uniform stressing of the porous silicon 16 (through volumetric expansion or contraction). The uniform stressing of the porous silicon 16 can then be transferred to the stressed thin film 10, thereby creating a homogeneously stressed thin film 10.
Next, and with reference to step 120 in
In the annealing process taking place in the reaction chamber 82, the input steam decomposes to 2 H++O−2 and the oxygen reacts with the silicon surface of the pore walls to form SiO2 (thereby consuming silicon). In other words, the silicon is replaced by SiO2. The oxidation forms an oxide layer 18 (e.g., SiO2) on the epilayer 14 in addition to the interior porous structure of the porous silicon substrate 16. This causes the porous silicon substrate 16 to undergo volumetric expansion. The expansion of the porous silicon substrate 16 imparts a tensile stress on the silicon epilayer 14. It should also be noted that the silicon epilayer 14 has a uniform thickness and a smooth interface is formed between the porous substrate 16 and the crystalline portion.
With reference to step 130, a second or transfer substrate 20 is provided. The transfer substrate 20 may be formed, for example, from silicon. With reference to
Still referring to
As an alternative to the embodiment described above, the oxide layer 18 is replaced with silicon nitride (Si3N4). Specifically, after the transformation of the doped, p+ silicon substrate 12 into porous silicon 16 by anodization, silicon nitride is deposited thereon. The silicon nitride may be deposited using low pressure chemical vapor deposition (LPCVD) which typically occurs at or around 800° C. although other temperatures used to deposit silicon nitride via LPCVD may also be used. Alternatively, silicon nitride may be deposited using plasma enhance chemical vapor deposition (PECVD). Typical temperatures associated with PECVD deposition of silicon nitride fall between around 100° C. to around 400° C. although other temperatures capable of silicon nitride deposition via PECVD are also contemplated. Silicon nitride deposition takes place outside an oxidative environment, for example, either in vacuum or in the presence of an inert gas. A layer of silicon nitride thus replaces the oxide layer 18 shown in step 120. The silicon nitride also enters the interstitial pores of the porous silicon 16. The deposition of silicon nitride within the porous silicon 16 causes contraction or shrinkage of the porous silicon 16 substrate 12. This, in turn, imparts a compressive stress on the silicon epilayer 14.
In this embodiment, after the bonding step (step 150), the porous silicon 16 is etched away using an etching solution. For example, the porous silicon 16 may be etched away by a solution of potassium hydroxide (KOH) and phosphoric acid (H2PO4). The potassium hydroxide is used to etch away the porous silicon 16 while the phosphoric acid removes silicon nitride formed on the surface thereof. Of course, other etchants may also be used to remove the porous silicon 16 and adherent silicon nitride layer.
Next, as illustrated in step 230, the thin film or epilayer 14 of silicon is removed. The thin film 14 may be removed using conventional CMP processing. The purpose of the thin film 14 in this embodiment is needed to form a substantially smooth or flat surface for subsequent processing steps. In an alternative embodiment, the formation of the thin film 14 may be bypassed entirely and CMP processing may be used to obtain the substantially smooth or flat surface. In step 240, the porous silicon 16 is then deposited with an oxide layer 18. Alternatively, the oxide layer 18 may be substituted with silicon nitride. For example, the oxide (or silicon nitride) layer 18 may be deposited using plasma enhanced chemical vapor deposition (PECVD). Still referring to step 240, the layer 18 may then be planarized by CMP processing to form a substantially flat upper surface. The flat surface facilitates subsequent wafer bonding of the porous silicon 16 with layer 18 to a transfer substrate (described in more detail below).
Referring now to
The transfer substrate 30 is then subject to hydrogen ion implantation. As seen in
Next, in step 260, the porous silicon 16 containing the oxide layer 18 is then bonded to the transfer substrate 30 via the front face 30a of the transfer substrate 30. The porous silicon-containing substrate 12 may be bonded to the transfer substrate 30 using a hydrophilic wafer bonding process like the those described herein. The porous silicon-containing substrate 12 and transfer substrate 30 may be subject to a low temperature anneal to establish the initial bonding. After initial bonding, the substrates 12, 30 are subject to a medium temperature annealing process used in the well known SMART-CUT process to thereby separate the transfer substrate 30 along the weakened region containing the implanted hydrogen ions. The separation of the transfer substrate 30 along the weakened region is illustrated in step 270 of
Because the separation of the transfer substrate 30 along the weakened zone creates a rough surface, the porous silicon substrate 12 containing the oxide layer 18 and portion of the silicon transfer substrate 30 is then subject to a planarization step as is shown in step 280. For example, CMP processing may be used to form a substantially flat surface silicon exfoliation layer 34 from the transfer substrate 30.
Referring to step 290, the now polished substrate 12 containing the porous silicon 16, layer 18, and silicon exfoliation layer 34 is then subject to an annealing process. The annealing process imparts a stress (e.g., tensile) to the exfoliation layer 34. For example, the porous silicon substrate 12 with the oxide layer 18 and silicon exfoliation layer 34 is then subject to an oxidating environment. For example, the structure shown in step 280 may be placed in a reaction chamber 82 of the type disclosed in
Still referring to step 290 in
As seen in step 290, the recipient substrate 40 may have formed thereon a thermally grown oxide layer 42, for example, if the recipient substrate 40 is formed from silicon. In cases where the recipient substrate 40 is not silicon, the oxide layer 42 may be formed using PECVD. The thermally grown oxide layer 42 assists in bonding the recipient substrate 40 to the oxidized substrate 12. For example, the thermally grown oxide layer 42 may be formed from silicon dioxide. The thermally grown oxide layer acts as an interface or intermediate layer.
In step 300, the oxidized substrate 12 and the recipient substrate 40 are bonded together. The transfer or bonding of the oxidized substrate 12 (with the silicon exfoliation layer 34) may be performed using a hydrophilic wafer bonding process of the type disclosed herein. Next, as shown in step 310, the bonded structure is subject to a wet etching process to remove the porous silicon 16. For example, an etching solution of potassium hydroxide (KOH) may be used to etch away the porous silicon 16. Next, as seen in step 320, the oxide layer 18 may then be removed using another etching solution. For instance, an etching solution of hydrogen fluoride (HF) may be used to remove the oxide layer 18. Removal of the oxide layer 18 then exposes the stressed silicon exfoliation layer 34 on the recipient substrate 40. Because of the volumetric expansion of the porous silicon 16, a tensile stress is imparted to the silicon exfoliation layer 34 (also referred to as stressed thin film layer 34). The stressed thin film layer 34 is substantially, if not entirely, free of any dislocation defects. In addition, the stressed thin film layer 34 is homogeneously stressed across substantially the entire surface.
In one alternative aspect of the invention, the process disclosed in
In this alternative embodiment, after the bonding step (step 300), the porous silicon 16 is etched away using an etching solution. For example, the porous silicon 16 may be etched away by a solution of potassium hydroxide (KOH) and phosphoric acid (H2PO4). The potassium hydroxide is used to etch away the porous silicon 16 while the phosphoric acid removes silicon nitride formed on the surface thereof. Of course, other etchants may also be used to remove the porous silicon 16 and adherent silicon nitride layer.
In another alternative embodiment, in the process illustrated in
The fabrication methods described herein are able to produce relatively large, homogenously strained semiconductor thin films that are substantially, if not entirely, free of dislocations. The methods described herein can be used to grow relatively thin semiconductor epitaxial layers that are below the critical thickness where dislocations are generated. Moreover, the methods do not employ graded buffer layers (like SiGe) that provide a source of dislocation generation. In addition, the use of a porous substrate like porous silicon that has a substantially uniform pore distribution ensures that subsequent processing that expands or contracts the porous substrate imparts a substantially uniform stress to the thin film. The thin film formed is this homogeneous with respect to stress across substantially the entire surface. Another benefit of the current method is that relatively low processing temperatures (e.g., around or below 500° C.) prevent or mitigate contamination of the stressed thin film from dopants.
Importantly, the methods described herein may be used to expand the total available spectrum of lattice constants available for manufacturing semiconductor devices. Rather than relying on a few discrete lattice constant points in the available spectrum, individual materials may be selectively stressed to modify their lattice constants. Tensile and/or compressive stresses applied to thin films alter the film's underlying lattice constant. In this regard, selectively applied stresses to thin films may be used to significantly expand the available lattice constants of semiconductor thin films. The varying lattice constants may be used to manufacture microelectronic or optoelectronic devices with new, useful properties.
While embodiments of the present invention have been shown and described, various modifications may be made without departing from the scope of the present invention. The invention, therefore, should not be limited, except to the following claims, and their equivalents.
This Application claims priority to U.S. Provisional Patent Application No. 60/700,448 filed on Jul. 19, 2005. U.S. Provisional Patent Application No. 60/700,448 is incorporated by reference as if set forth fully herein.
The U.S. Government may have a paid-up license in this invention and the right in limited circumstances to require the patent owner to license others on reasonable terms as provided for by the terms of contract number: No. FA9550-04-1-0370 awarded by the United States Air Force.
Number | Date | Country | |
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60700448 | Jul 2005 | US |