The present invention relates to semiconductor devices and methods of making such devices. More particularly, the invention relates to solid state materials and to a novel method of forming buried conductor patterns in such solid state materials.
Monocrystalline solid state materials such as single-crystal semiconductors are the basis of the current microelectronics industry. Solid state materials are characterized by a variety of properties, for example, electrical properties such as electrical conductivity or charge mobility, optical properties such as refractive index or speed of photons, thermal properties such as thermal conductivity or thermal expansion, mechanical properties such as stress or strain curves, and chemical properties such as resistance to corrosion or reaction consistency, among others.
Over the past years, the semiconductor industry has constantly explored new ways of increasing the amount of active surface area on the integrated circuit chips, particularly on those employing monocrystalline semiconductor substrates.
Accordingly, attempts to modify the electrical, optical, thermal and/or mechanical properties of such monocrystalline substrates have been made in an effort to minimize the dimensions of the IC devices, while maximizing the corresponding available active area. For example, new epitaxial growth processes such as the Epitaxial Lateral Overgrowth (ELO) have been used in an attempt to extend the amount of surface area available to active devices. However, these growth processes had limited results mainly because they consume part of the precious surface areas for seeding purposes, defeating therefore the primary purpose of increasing the available active area.
Another technology proposed by the semiconductor industry is the so-called Silicon-On-Insulator (SOI) process, wherein oxygen atoms are implanted at high dose and energy to form a silicon dioxide insulating layer between the upper surface of the original monocrystalline substrate and the bottom bulk portion of the same substrate. Although the SOI devices have many advantages, such as reduced parasitic capacitance due to the buried insulating layer, the process is relatively expensive because of the high costs of implanting the oxygen atoms and curing of the implant-induced defects.
Accordingly, there is a need for an improved method of increasing the available active surface area on integrated circuit chips fabricated on monocrystalline substrates. There is also a need for a more advantageous method of forming monocrystalline superconducting substrates for low power and high speed microelectronics devices, as well as a method for minimizing the cost of fabricating such substrates. There is further a need for an improved metallization scheme which facilitates the formation of active devices on SOI substrates and on the more novel Silicon-On-Nothing (SON) substrates.
The present invention provides a method of forming a plurality of buried conductors and/or buried plate patterns in semiconductor substrates, such as monocrystalline silicon substrates. According to an exemplary embodiment of the invention, a plurality of empty-spaced buried patterns are formed in a monocrystalline substrate. Holes are next formed in the monocrystalline substrate to connect surfaces of the substrate with the previously formed empty-spaced patterns. The whole assembly is subsequently exposed to an oxidizing atmosphere so that the inner surfaces of the empty-spaced patterns are oxidized. The empty-spaced patterns are then filled with a suitable conducting material by suitable methods.
These and other features and advantages of the invention will be more clearly apparent from the following detailed description which is provided in connection with accompanying drawings and which illustrates exemplary embodiments of the invention.
a)–(f) illustrate a portion of a silicon substrate undertaking a sequence of steps for single sphere-shaped empty space formation.
a)–(c) illustrate a portion of a silicon substrate undertaking a sequence of steps for single pipe-shaped empty space formation, performed in accordance with a method of forming a buried pattern of the present invention.
a)–(b) illustrate a portion of a silicon substrate undertaking a sequence of steps for plate-shaped empty space formation, performed in accordance with a method of forming a buried pattern of the present invention.
In the following detailed description, reference is made to various exemplary embodiments for carrying out the invention. These embodiments are described with sufficient detail to enable those skilled in the art to practice the invention, and it is to be understood that other embodiments may be employed, and that structural, electrical and process changes may be made, and equivalents substituted, without departing from the invention. Accordingly, the following detailed description is exemplary and the scope of the present invention is defined by the appended claims.
The term “substrate” used in the following description includes any semiconductor-based structure having an exposed surface in which the structure of this invention may be formed. The term “substrate” is to be understood as including substrates formed of silicon, silicon-on-insulator, doped and undoped semiconductors, epitaxial layers of silicon supported by a base semiconductor foundation, and other semiconductor and dielectric structures. Furthermore, when reference is made to a substrate in the following description, previous process steps may have been utilized to form regions or junctions in the base semiconductor structure or foundation.
The following illustration is for a particular embodiment in a silicon structure. However, it should be apparent to one skilled in the art that a similar embodiment is possible in any semiconductor structure.
Referring now to the drawings, where like elements are designated by like reference numerals,
Empty spaces which are formed in silicon substrates and have various shapes, such as plates, spheres or pipes, may be formed as a result of the self-organizing migration properties on the silicon surface. As such, when deeply-etched silicon substrates are annealed in a hydrogen ambient, for example, the silicon atoms on the surface migrate so that their surface energy is minimized. Based on these findings, Sato et al. have demonstrated that the geometry of empty spaces, such as spheres, plates and pipes, formed under the surface of a silicon substrate depends on the size, number and spacing of a plurality of cylindrical holes that are initially formed at a low temperature.
For example,
As analyzed by Nichols et al., in Surface-(Interface-) and Volume-Diffusion Contributions to Morphological Changes Driven by Capillarity, Trans. AIME 233 at 1840 (Oct. 1965), the disclosure of which is incorporated by reference herein, when Lc corresponds to the surface diffusion state, the number N of empty spheres that form from a cylindrical hole depends both on the length L of the cylindrical hole and on the cylinder radius Rc. Accordingly, the number N of empty spheres formed from a cylindrical hole made in a silicon substrate could be estimated according to the following equation:
8.89Rc N<L<8.89Rc(N+1) (1)
wherein: N=number of empty spheres;
Thus, equation (1) predicts that, if L<8.89 Rc, the number of empty spheres will be N=0, which means that no empty spheres will form from a cylindrical hole.
When one or more empty spheres form with a radius Rs, then according to Nichols et al., the value of Rs is given by the following equation:
Rs=1.88 Rc (2)
wherein: Rs=sphere radius; and
When two or more empty spheres form from a cylinder hole with a cylinder radius Rc, then the distance λ between the centers of two adjacent empty-spaced spheres is calculated from the following formula:
λ=8.89 Rc (3)
wherein: λ=center-to-center distance between two adjacent spheres; and
Reference is now made to
2 Rc<Δ<3.76 Rc (4)
wherein: Rc=cylinder radius; and
Equation (4) ensures that adjacent cylindrical holes 22, 32 do not touch each other allowing, therefore, the formation of a plurality of adjacent spheres that combine to form the resulting pipe-shaped empty space 23 and plate-shaped empty space 33.
The values of the pipe radius Rp and of the plate thickness Tp are given by the following two expressions:
Rp=(8.86 Rc3/Δ)1/2 (5)
Tp=27.83 Rc3/Δ2 (6)
wherein: Rp=pipe radius;
Reference is now made to
Radius R1 (
Subsequent to the formation of the pipe-shaped empty space 23, a second pipe-shaped empty space 43 (
Radius R2 (
Although
Radius R3 (
Subsequent to the formation of the first pipe-shaped empty space 23, second pipe-shaped empty space 43, and plate-shaped empty space 53, additional interconnect structures and associated dielectric layers could be formed to create operative electrical paths down from the empty-spaced structures formed within the silicon substrate 10 and up to the silicon surfaces, such as the upper silicon surface 11, and any IC devices formed thereon. Accordingly, as illustrated in
Alternatively, or in addition to the oxidizing atmosphere, a barrier layer 72 may be formed on surfaces of the silicon substrate 10, within each of the interconnect holes 24, 45, 55, and on the inner surfaces of each of the first pipe-shaped empty space 23, the second pipe-shaped empty space 43, and the plate-shaped empty space 53, as also shown in
Preferred materials for the barrier layer 72 are metals, such as titanium (Ti), zirconium (Zr), tungsten (W), or hafnium (Hf), or metal compounds, such as tantalum nitride (TaN) or silicon nitride (Si3N4). If desired, the barrier layer 72 may be formed of refractory metal compounds, such as refractory metal nitrides (for example TiN and HfN), refractory metal carbides (for example TiC or WC), or refractory metal borides (for example TiB or MoB). The selection of a material for the barrier layer 72 depends upon the specific conductor to be deposited and the method which is chosen to deposit such conductor. In turn, the selection of the conductor material will depend upon the type and temperature of subsequent processing steps. For example, aluminum (Al) would not be chosen as the conductor material if the subsequent processing steps require temperatures above approximately 600° C. Similarly, tungsten (W) would be a preferred conductor for temperatures above approximately 1,000° C. In any event, the barrier layer 72 suppresses the diffusion of the metal atoms from the subsequently deposited conductive material (
Although in an exemplary embodiment of the invention the barrier layer 72 is simultaneously deposited in the interconnect holes 24, 45, 55, and on the inner surfaces of each of the first pipe-shaped empty space 23, the second pipe-shaped empty space 43, and the plate-shaped empty space 53, the invention is not limited to this embodiment. For example, the barrier layer 72 may be deposited first in the interconnect hole 24 and its corresponding pipe-shaped empty space 23, before the formation of the interconnect hole 45 and its corresponding second pipe-shaped empty space 43, and before the formation of the interconnect hole 55 and its corresponding plate-shaped empty space 53. In this embodiment, the barrier layer 72 may be formed of a first barrier material corresponding to the pipe-shaped empty space 23, of a second barrier material corresponding to the second pipe-shaped empty space 43, and of a third barrier material corresponding to the plate-shaped empty space 53. The first, second and third barrier materials may be the same or different, depending on the characteristics of the IC device.
As illustrated in
After the deposition of the conductive material 73, excess barrier material and excess metal formed above the upper silicon surface 11 may be removed by either an etching or a polishing technique to form the buried silicon structure 100 illustrated in
Although the buried silicon structure 100 is shown in
The processing steps of the present invention may be also reduced if the lower level buried conductor patterns do not cross over each other below upper level buried patterns, such as the plate-shaped empty space 53 (
In addition, further steps to create a functional memory cell on the silicon substrate 10 may be carried out. Thus, additional multilevel interconnect layers and associated dielectric layers could be formed to create operative electrical paths from the buried silicon structure 100 to a source/drain region (not shown) adjacent to a transistor gate structure (not shown) of the substrate 10, or to any active devices 102, 104, 106 (
The invention thus provides a technique for forming buried conductors in a semiconductor, for example, silicon, substrate which may be used for example as interconnects to various structures and devices in an integrated circuit.
A typical processor-based system 400 which includes a memory circuit 448, for example a DRAM, is illustrated in
In the case of a computer system, the processor system may include peripheral devices such as a floppy disk drive 454 and a compact disk (CD) ROM drive 456 which also communicate with CPU 444 over the bus 452. Memory 448, the CPU 444 or others of the illustrated electrical structures may be constructed as an integrated circuit, which includes one or more buried silicon structures 100 in accordance with the invention. If desired, the memory 448 may be combined with the processor, for example CPU 444, in a single integrated circuit.
The above description and drawings are only to be considered illustrative of exemplary embodiments which achieve the features and advantages of the present invention. Modification and substitutions to specific process conditions and structures can be made without departing from the spirit and scope of the present invention. Accordingly, the invention is not to be considered as being limited by the foregoing description and drawings, but is only limited by the scope of the appended claims.
This application is a divisional of application Ser. No. 09/734,547, filed on Dec. 13, 2000 now U.S. Pat. No. 6,383,924, which is hereby incorporated by reference.
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