The present application relates generally to semiconductor devices, and more particularly to metallic doped silicon-on-insulator (SOI) substrates having improved thermal conduction and fin field effect transistor devices formed on such SOI substrates.
Fully-depleted devices such as fin field effect transistors (FinFETs) are candidates to enable scaling of next generation gate lengths to 14 nm and below. Fin field effect transistors (FinFETs) present a three-dimensional architecture where the transistor channel is raised above the surface of a semiconductor substrate, rather than locating the channel at or just below the surface. With a raised channel, the gate can be wrapped over the top and the sides of the channel, which provides improved electrostatic control of the device.
The manufacture of FinFETs typically leverages a self-aligned process to produce extremely thin fins, e.g., 20 nm wide or less, on the surface of a substrate using selective-etching techniques. A gate structure is then deposited to contact multiple surfaces of each fin to form a multi-gate architecture.
The characteristics of FinFET-based devices compare favorably with traditional transistor architectures. For example, a 16 nm FinFET has a higher gate density and about 25% more drive capability compared with a 20 nm planar transistor. However, the confined geometry associated with the FinFET architecture also generates 25-30% more power density and an attendant increase in localized heat, which can negatively affect device performance and reliability. Moreover, the insulating characteristics of SOI substrates, which are ubiquitous in FinFET design, exacerbate the challenges associated with thermal budget and operating temperature-driven failure.
Accordingly, it would be advantageous to develop a FinFET architecture that mitigates the operating temperature effects associated with these high power density structures.
In accordance with embodiments of the present application, a FinFET is constructed on an SOI substrate having a doped isolation (i.e., buried oxide) layer. Metallic doping of the isolation layer increases its thermal conductivity, which improves heat conduction and decreases the susceptibility of the device to temperature-induced deterioration and/or failure over time. The amount as well as the configuration of the doping can be tailored to specific circuit architectures.
An example SOI substrate includes a handle portion, an isolation layer disposed over the handle portion, and a semiconductor layer disposed over the isolation layer defining an interface boundary with the isolation layer. The isolation layer includes a dopant such that the doped isolation layer exhibits a thermal conductivity greater than that of an undoped corresponding isolation layer.
A method of manufacturing such an SOI substrate includes forming an isolation layer over a handle portion of a semiconductor substrate, forming a semiconductor layer over the isolation layer, and incorporating a dopant into the isolation layer to increase the thermal conductivity of the isolation layer.
The following detailed description of specific embodiments of the present application can be best understood when read in conjunction with the following drawings, where like structure is indicated with like reference numerals and in which:
Reference will now be made in greater detail to various embodiments of the subject matter of the present application, some embodiments of which are illustrated in the accompanying drawings. The same reference numerals will be used throughout the drawings to refer to the same or similar parts. It is noted that the drawings are provided for illustrative purposes and, as such, may not be drawn to scale.
In the following description, numerous specific details are set forth, such as particular structures, components, materials, dimensions, processing steps and techniques, in order to provide an understanding of the various embodiments of the present application.
However, it will be appreciated by one of ordinary skill in the art that the various embodiments of the present application may be practiced without these specific details. In other instances, well-known structures or processing steps have not been described in detail in order to avoid obscuring the present application.
As an alternative to a conventional bulk silicon wafer platform for integrated circuit (IC) manufacture, SOI (silicon-on-insulator or semiconductor-on-insulator) substrates have been embraced by the microelectronics industry. SOI substrates are composite structures that include two semiconductor layers separated by an isolation layer. Compared to bulk silicon substrates, SOI substrates provide a number of advantages to circuit designers, including faster switching speeds, greater resistance to radiation effects, higher component packing densities, smaller leakage currents and parasitic capacitances, and the avoidance of low-impedance paths between power supply rails, i.e., “SCR latch-up.”
Referring to
The SOI substrate 100 is not limited to silicon-containing materials. Each of the handle portion 110 and the semiconductor layer 130 may independently comprise other semiconductor materials, including germanium (Ge), III-V compound semiconductors such as GaAs, GaN, GaP, InAs, InSb, ZnSe, and ZnS, and II-VI compound semiconductors such as CdSe, CdS, CdTe, ZnSe, ZnS and ZnTe.
According to various embodiments, the handle portion 110 and the semiconductor layer 130 may comprise the same semiconductor material or different semiconductor materials. The handle portion 110 of an example semiconductor substrate may comprise (100)-oriented silicon or (111)-oriented silicon, for example, and the semiconductor layer 130 may comprise (100)-oriented silicon, single crystal SiGe or single crystal GaAs, although other materials and material combinations are contemplated. The thickness of the semiconductor layer 130 can be 10 to 100 nm, for example, although smaller and larger values are contemplated.
SOI substrate 100 may have dimensions as typically used in the art. Example substrate diameters include, but are not limited to, 50, 100, 150, 200, 300 and 450 mm. The total substrate thickness may range from 250 microns to 1500 microns, although in particular embodiments the substrate thickness is in the range of 725 to 775 microns, which corresponds to thickness dimensions commonly used in silicon CMOS processing.
In the example of
Exemplary low-k materials include but are not limited to, amorphous carbon, fluorine-doped oxides, carbon-doped oxides, SiCOH or SiBCN. Commercially-available low-k dielectric products and materials include Dow Corning's SiLK™ and porous SiLK™, Applied Materials' Black Diamond™, Texas Instrument's Coral™ and TSMC's Black Diamond™ and Coral™. As used herein, a low-k material has a dielectric constant less than that of silicon oxide.
An SOI substrate can be formed using a variety of methods such as, for example, SiMOX or bonding methods known to those skilled in the art. According to various embodiments, a wafer bonding process for manufacturing SOI wafers includes physically uniting two single crystal semiconductor wafers. For instance, one of the wafers can be thermally oxidized to form the isolation layer and, after cleaning operations, bonded to the other. Bringing two hydrophilic surfaces (such as SiO2) into direct contact can result in a strong interfacial bond. Following a thermal anneal at temperatures as high as 1100° C. (e.g., 1000° C.), the bond strength can be increased to that of bulk material. The outer surface of the composite wafer can be ground and polished to the desired thickness (e.g., 1-3 microns) using, for example, chemical mechanical polishing.
Chemical mechanical polishing (CMP) is a material removal process that uses both chemical reactions and mechanical force to remove material and planarize a surface. In general, the surface to be polished is brought into contact with a rotating pad whereupon a chemically reactive slurry containing an abrasive, such as alumina, deteriorates and progressively removes the exposed surface layer. In certain embodiments, the CMP process removes the majority of the handle portion one of the bonded substrates, leaving a thin semiconductor overlayer on the isolation layer, supported by a semiconductor substrate.
Optionally, an epitaxial layer for integrating electronic components can be formed on the thinner single crystal layer. The additional epitaxial layer, if provided, may be formed by chemical vapor deposition. For instance, a silicon epitaxial layer may be formed at deposition temperatures of ˜1000° C. using dichlorosilane (SiH2Cl2) as a source gas.
The terms “epitaxy,” “epitaxial” and/or “epitaxial growth and/or deposition” refer to the growth of a semiconductor material layer on a deposition surface of a semiconductor material, in which the semiconductor material layer being grown assumes the same crystalline habit as the semiconductor material of the deposition surface. For example, in an epitaxial deposition process, chemical reactants provided by source gases are controlled and the system parameters are set so that depositing atoms alight on the deposition surface and remain sufficiently mobile via surface diffusion to orient themselves according to the crystalline orientation of the atoms of the deposition surface. Therefore, an epitaxial semiconductor material has the same crystalline characteristics as the deposition surface on which it is formed. For example, an epitaxial semiconductor material deposited on a (100) crystal surface will take on a (100) orientation.
A further example wafer bonding method can be performed in conjunction with a layer transfer process where, by way of example, a gallium arsenide surface to be bonded is cleaved from a source wafer of gallium arsenide. In such a process, a single crystal wafer of gallium arsenide (GaAs) is ion implanted, e.g., with hydrogen, to a desired depth to define a thin layer of gallium arsenide to be transferred. The implanted wafer is then pre-bonded to the isolation layer of a support substrate such as an oxidized silicon substrate. The pre-bonded assembly is heated to cause eruption of the hydrogen-rich plane and cleavage of the defined gallium arsenide layer from the gallium arsenide wafer. The support substrate with the transferred layer can then be heated to improve the bonding between the substrate and the transferred layer. The excess support substrate can be removed and the gallium arsenide layer polished to form an SOI structure. The gallium arsenide source wafer and the excess support substrate can each be recycled back into the process.
According to various embodiments, the thermal conductivity of an SOI substrate can be increased by incorporating a metallic dopant, i.e., impurity, into the isolation layer. Introduction of the dopant atoms can be performed before or after defining the SOI structure. Increasing the thermal conductivity of the SOI substrate facilitates heat transfer and heat dissipation, which can improve the performance and reliability of SOI-based devices. Example dopants include C, Al, Si, Ge, Ta, W, Mo, and alloys thereof, including SiC, AlN and TaSi, for example.
Within a locally-doped region, the spatial distribution of one or more dopants within the isolation layer 120 can be homogeneous or non-homogeneous. Further, according to various embodiments, and as illustrated with respect to several exemplary methods, spatial non-homogeneity of a dopant can independently vary in each of three dimensions, i.e., length, width and depth. As used herein, a depth of the isolation layer is defined with reference to a top surface thereof, i.e., from an interface boundary with the semiconductor material layer. In certain embodiments, the isolation layer includes one or more doped regions, which can be configured to accommodate particular device architectures, for example.
One example method of forming a semiconductor-on-metallic-doped insulator (SOMDI) wafer is illustrated in
In the instant embodiment, as illustrated in
A further example method of forming an SOMDI substrate is illustrated in
As shown in
The dopant concentration within the isolation layer 120 may be constant, or vary as a function of isolation layer thickness. For instance, the dopant concentration may be greatest at the interface between the isolation layer 120 and the semiconductor layer 130 and decrease with increased thickness. Alternatively, the dopant concentration may be greatest at the interface of the isolation layer 120 with handle substrate 110. In the latter case, the dopant concentration may increase from a minimum concentration at the interface between the isolation layer and the semiconductor layer 130 to a maximum at the interface of the isolation layer with the handle substrate 110.
A variant of the embodiment illustrated in
According to various embodiments, an implant dose for the dopant can range from 1×1014/cm2 to 1×1016/cm2, e.g., 1×1014, 2×1014, 5×1014, 1×1015, 2×1015, 5×1015 or 1×1016/cm2, including ranges between any of the foregoing values. The ion implantation energy can range from 20 to 60 keV, e.g., 20, 40, or 60 keV, including ranges between any of the foregoing values. In various embodiments, the dopant profile in the thickness dimension of the isolation layer is defined by the ion implantation energy.
Referring to
Expressed as a percentage of the thickness of the isolation layer 120 from a top surface thereof to the interface with the supporting handle substrate 110, as seen with reference to
A variant of the embodiment illustrated in
In the embodiments illustrated in
As used herein, “horizontal” refers to a general direction along a primary surface of a substrate, and “vertical” is a direction generally orthogonal thereto. Furthermore, “horizontal” and “vertical” are generally perpendicular directions relative to one another independent of orientation of the substrate in three-dimensional space. Thus, a vertically-discrete doped region adjoins at least one of an overlying or an underlying un-doped region.
For instance, a vertically-discrete doped region may be bounded by at least one of an overlying or an underlying un-doped region. A horizontally-discrete doped region adjoins an adjacent un-doped region such that, for example, a horizontally-discrete doped region is bounded by an adjacent un-doped region.
Referring to
Referring to
As illustrated in
According to certain embodiments, the ion implantation energy can be adjusted to control the depth of the implantation profile. For example, referring to
Referring to
A hybrid doping profile is illustrated in
While the locally-doped region 160a and the globally-doped region 160b are each shown extending to a respective upper and lower surface of the isolation layer 120, it will be appreciated that the depth profile of the doped regions can extend from any suitable first depth to any suitable second depth of the isolation layer. Moreover, it will be appreciated that the dopant architecture of
In the structures shown in
The dopant concentration within the doped regions 160 may be constant or may vary, for example, as a function of isolation layer thickness. According to various embodiments, the dopant profile may be engineered to control the thermal conductivity of the isolation layer 120 and hence the effective thermal conductivity of the SOI substrate. Moreover, the dopant profile within the isolation layer can be configured to balance the properties of thermal conduction and electrical insulation.
It is known that the ratio of the electronic contribution of the thermal conductivity (κ) to the electrical conductivity (σ) of a metal is proportional to temperature according to the relationship κ/σ=LT, where L is the Lorenz number. It will be appreciated that uniform metallic doping of the entire isolation layer 120 will desirably increase the thermal conductivity of the isolation layer 120 but may undesirably increase the electrical conductivity of the isolation layer 120. A metallic dopant may be chosen from C, Al, Si, Ge, Ta, W, Mo, SiC, AlN and TaSi, as well as combinations thereof.
Current-voltage (I-V) traces for tungsten-doped isolation layers at various temperatures are shown in
In the case of an isolation layer consisting essentially of silicon dioxide (SiO2), which has an un-doped thermal conductivity of 1.3-1.4 W/mK, modeled data have shown that the incorporation of a dopant into the isolation layer can increase the effective thermal conductivity to 250 W/mK. In various embodiments, the effective thermal conductivity of an SOMDI substrate can range from 5 to 250 W/mK, e.g., 5, 10, 15, 20, 50, 100, 150, 200 or 250 W/mK, including ranges between any of the foregoing values. Through global and/or local doping of the isolation layer and the attendant increase in thermal conductivity, a significant reduction in device temperature can be realized.
Thermal simulations have demonstrated that both the maximum temperature increase and the average temperature increase within a silicon dioxide isolation layer can be impacted by global and local doping profiles. Simulation results are summarized in
For an undoped, 182 nm thick SiO2 isolation layer, the maximum and average temperature rise from the 3-dimensional thermal model assuming 40 parallel silicon fins having a fin height of 28 nm and a fin length of 5000 nm overlying the isolation layer, are 100K and 90K, respectively.
Global (unmasked) doping into the near surface region of the isolation layer increases the thermal conductivity of the isolation layer to 5 W/mK and 15 W/mK, depending on the dopant concentration. The data in
Local doping into the near surface region of the isolation layer can form a local thermal pipe having a dramatically increased thermal conductivity. Depending on the dopant concentration, the effective thermal conductivity in the near surface region of the isolation layer is increased to 50 or 150 W/mK. Referring to
The combination of local doping and global doping can be used to tailor both the thermal conductivity and the electrical resistivity of the SOMDI substrate. The formation of a locally-doped interfacial region between the isolation layer and the overlying semiconductor layer, for example, in conjunction with a deeper globally doped region can dampen the maximum temperature increase by as much as 20%, e.g., 5, 10 or 20%, including ranges between any of the foregoing values, and dampen the average temperature increase by as much as 40%, e.g., 10, 20, 30 or 40%, including ranges between any of the foregoing values, while maintaining good electrical insulating properties at the interface with the semiconductor layer 130, which can be used to form the fins of a fin field effect transistor (FinFET), for example.
Referring to
Each fin has a height (H) that may range from 10 nm to 100 nm and a width (W) that may range from 4 nm to 30 nm. Other heights and widths that are less than or greater than the ranges mentioned can also be used. In structures comprising plural fins, each fin may be spaced apart from its nearest neighbor by a pitch (i.e., repeat distance) of 20 nm to 100 nm. Such plural fins are typically oriented parallel to each other. Plural fins may have identical or substantially identical dimensions, i.e., height and/or width. As used herein, substantially identical dimensions vary by less than 10%, e.g., less than 5%, 2% or 1%. As shown in
Epitaxial source and drain raised active regions 310a, 310b are formed over the fins 202 at opposing ends thereof, while a gate stack 400 is formed over the fins 202 defining a channel region between the source and drain regions. Gate stack 400 includes a gate dielectric 402, a gate conductor 404, and a gate cap 406. Gate stack 400 is formed generally orthogonal to the length-wise dimension of the fins 202 such that gate dielectric 402 and gate conductor 404 straddle the fins.
Gate dielectric 402 may comprise silicon oxide, silicon nitride, silicon oxynitride, a high-k dielectric, or other suitable material. As used herein, a high-k material has a dielectric constant greater than that of silicon oxide. A high-k dielectric may include a binary or ternary compound such as hafnium oxide (HfO2).
A gate conductor 404 is formed over the gate dielectric 402, and a gate cap 406 is formed over the gate conductor 404. The gate conductor 404 may include a conductive material such as polysilicon, silicon-germanium, a conductive metal such as Al, W, Cu, Ti, Ta, W, Pt, Ag, Au, Ru, Ir, Rh and Re, alloys of conductive metals, e.g., Al—Cu, silicides of a conductive metal, e.g., W silicide, and Pt silicide, or other conductive metal compounds such as TiN, TiC, TiSiN, TiTaN, TaN, TaAlN, TaSiN, TaRuN, WSiN, NiSi, CoSi, as well as combinations thereof. The gate conductor 404 may comprise one or more layers of such materials such as, for example, a metal stack including a work function metal layer and/or a liner.
Sidewall spacers 408 may be formed on the sides of the gate stack 400. The gate spacers 408 can be formed around the gate stack 402, 404, 406. The gate spacers 408 can be formed, for example, by depositing a conformal dielectric material layer on the plurality of semiconductor fins 202 and the gate stack, and anisotropically etching the conformal dielectric layer.
According to various embodiments, the substrate used to support the device architecture is a semiconductor-on-metallic-doped insulator (SOMDI) substrate. The metallic atom or metallic compound-doped substrate exhibits enhanced thermal conduction properties. For instance, the gate conductor of the device can be located at least partially over a doped region in order to enhance heat dissipation away from the gate conductor. The dopant profile within the buried oxide layer of the substrate may be engineered to conduct and remove heat without negatively impacting the electrical properties of the substrate in order to preserve device performance.
For instance, upper regions of the isolation layer of an example SOMDI substrate may be doped locally proximate to semiconductor fins that are defined over the isolation layer to provide thermal conduction while retaining sufficient electrical isolation between the fins and the semiconductor substrate. Lower regions of the isolation layer, spaced away from the fins, may be doped globally to enhance the thermal conductivity of the isolation layer.
As used herein, the singular forms “a,” “an” and “the” include plural referents unless the context clearly dictates otherwise. Thus, for example, reference to a “dopant” includes examples having two or more such “dopants” unless the context clearly indicates otherwise.
Unless otherwise expressly stated, it is in no way intended that any method set forth herein be construed as requiring that its steps be performed in a specific order. Accordingly, where a method claim does not actually recite an order to be followed by its steps or it is not otherwise specifically stated in the claims or descriptions that the steps are to be limited to a specific order, it is no way intended that any particular order be inferred. Any recited single or multiple feature or aspect in any one claim can be combined or permuted with any other recited feature or aspect in any other claim or claims.
As used herein, an element such as a layer or region that is “on” or “over” or “disposed over” a substrate or other layer refers to formation above, or in contact with, a surface of the substrate or layer. For example, where it is noted or recited that a layer is disposed over a substrate or other layer, it is contemplated that intervening structural layers may optionally be present between the layer and the substrate. In contrast, when an element is referred to as being “directly on” or “directly over” another element, there are no intervening elements present. It will also be understood that when an element is referred to as being “beneath” or “under” another element, it can be directly beneath or under the other element, or intervening elements may be present. In contrast, when an element is referred to as being “directly beneath” or “directly under” another element, there are no intervening elements present.
While various features, elements or steps of particular embodiments may be disclosed using the transitional phrase “comprising,” it is to be understood that alternative embodiments, including those that may be described using the transitional phrases “consisting” or “consisting essentially of,” are implied. Thus, for example, implied alternative embodiments to an oxide layer that comprises silicon dioxide include embodiments where an oxide layer consists essentially of silicon dioxide and embodiments where an oxide layer consists of silicon dioxide.
It will be apparent to those skilled in the art that various modifications and variations can be made to the present invention without departing from the spirit and scope of the invention. Since modifications, combinations, sub-combinations and variations of the disclosed embodiments incorporating the spirit and substance of the invention may occur to persons skilled in the art, the invention should be construed to include everything within the scope of the appended claims and their equivalents.