Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode
Reexamination Certificate
2001-08-29
2003-06-17
Fourson, George (Department: 2823)
Active solid-state devices (e.g., transistors, solid-state diode
Field effect device
Having insulated electrode
C257S407000
Reexamination Certificate
active
06580137
ABSTRACT:
TECHNICAL FIELD
This invention relates generally to transistors. More particularly, this invention relates to a transistor that is fully planar and operates at low voltages.
BACKGROUND OF THE INVENTION
The shrinking of silicon-based CMOS transistors from 10 um to sub-100 nm channel lengths has been the driving force behind the incredible advances in integration density of digital circuits. This exponential growth in circuit density (Moore's Law) has enabled increasingly sophisticated and fast microprocessors and digital signal processors. However, in this “post-PC age”, the markets driving the semiconductor industry are handheld consumer electronics, wireless communications, and Internet infrastructure. The ITRS Roadmap for the next ten years calls as much or more for increased diversity of integrated functions as for increased density.
CMOS switching frequencies (f
T
) exceeding 150 GHz have recently been achieved. Because this high-performance can be achieved using a relatively low cost manufacturing process, CMOS is rapidly becoming a serious option for many wireless Radio Frequency (RF) applications that were previously considered to be the exclusive domain of more expensive technologies, such as bipolar and gallium arsenide. This has led to a research focus shift to highly-integrated, highly-diverse CMOS System-On-a-Chip (SOC) technologies, integrating entire wireless mixed-signal systems on a single chip. Innovative device and technology changes are needed to provide high quality passive elements and high-gain, high-linearity, low-noise, low-power, RF capable transistors on carefully engineered substrates which reduce coupling and crosstalk noise of digital circuits from affecting sensitive on-chip RF receivers.
RF SOC's with the lowest possible energy consumption will use advanced spread-spectrum communication algorithms. Current research spans the circuit, architecture, and algorithm issues which impact the design of SOC CMOS wireless transceivers. Research activities also span bulk Si, SiGe, and SOI deep-sub-micron CMOS designs, the design of analog RF front ends, the design of A/D interface circuitry, and digital baseband signal processing. However, it is clear that single chip RF SOC solutions will require more than simply innovative circuit designs in order to be optimized.
The most serious limitation of these portable SOCs is power dissipation. The system battery typically comprises a large percentage of the cost, size, weight, and reliability problems in current handheld RF devices. As these systems become more highly integrated by utilizing sub-100 nm RF-CMOS devices, the power dissipation will become an even greater concern. Therefore, in order for the low-cost and high-integration density of RF-CMOS to be fully realized, it is imperative that new ultra-low power device structures and circuit design techniques be developed. These devices should preferably maintain multi-GHz level performance while operating with power supply voltages down to 0.25 volts. They also should preferably maintain high transconductance and low noise, and be easily integrated with on-chip, high-Q, tunable passive elements such as spiral inductors.
In summary, there is a need in the art for devices that operate at ultra low power. There is a need in the art for innovative transistors that provide for increased density. Additionally, there is a need to simplify the process for manufacturing transistors. Finally, there is a need to reduce the cost of manufacturing transistors.
SUMMARY OF THE INVENTION
An object of the present invention is provide unique transistors that enable increased density. Another object of the present invention is provide transistors that operate at ultra low power. An additional object of the present invention is to simplify the process for manufacturing transistors. Finally, an object is to reduce the cost of manufacturing transistors.
The above and other objects and advantages, which will be apparent to one of skill in the art, are achieved in the present invention which is directed to, in the first aspect, a method of manufacturing a Damascene double gated transistor, and the structure made by the method. More particularly, the invention provides a method for simultaneously making both four-terminal and dynamic threshold MOSFET devices. The method starts with either 1) a high-resistivity bulk silicon substrate (with or without an epitaxial layer) or 2) a silicon-on-insulator substrate or similar substrate having an isolated semiconductor region defined on its surface. These substrates may be created by any of the existing methods for making 1) high-resistivity bulk silicon or 2) high-resistivity SOI i.e. SIMOX, BESOI, SmartCut, Metal-induced recrystallization, Laser-induced recrystallization, etc.
In one embodiment, a silicon trench etch hard mask and polish stop “pad” layer (e.g. silicon nitride) is first deposited on the top silicon layer. A merged isolation/gate trench is then etched partially through this top silicon layer. A second mask and etch are used to completely remove the remaining silicon from the bottom of the isolation trenches, while leaving a thin active region of silicon under the gate trench which will become the channel. The remaining silicon “island” is barbell shaped, with large, thick source/drain regions on either side of the narrow, thin channel region. The gate trench is used for subsequently forming the bottom gate, channel, and top gate which are all self-aligned to this trench opening. A complementary set of shallow and deep implants is used to form a counter-doped channel and to heavily, uniformly dope the source/drain regions, respectively. This counter-doped channel is especially useful for maximizing the dynamic threshold swing, since it enhances body effect. Sidewall spacer material is then deposited, both to narrow the gate opening for sub-lithographic channel length and to isolate the sidewalls of the source/drain regions. Following the spacer formation, a highly-doped buried bottom gate is formed by ion implantation. This implant is masked by both the pad and the spacers, which space it away from both the heavily doped source and drain regions to prevent leakage and capacitance. The energy of this implant is high enough to place it below the counter-doped channel layer. High atomic weight ions are used (Indium for p+ and arsenic for n+) in order to obtain a super-steep retrograde implant profile between this buried layer and the channel above. Optionally, a thin undoped selective epitaxial silicon layer may be grown on top of the counter-doped channel to enhance the mobility of the device. At this point in the process, all high temperature steps are complete, meaning that temperature-sensitive materials (such as hafnium oxide and copper) may be used for the gate stack. Polysilicon or polysilicon/germaninum with an adjustable percentage of Ge may be used as the first gate conductor layer, in order to achieve additional threshold voltage design control. Alternately, a metal or silicide may also be used for the first gate conductor layer. The isolation/gate trenches are overfilled with this first gate conductor material, planarized back to the pad layer, and plasma recessed. Next, the entire channel and gate stack is patterned and etched, stopping on the bottom gate layer. The alignment of this mask to the original channel mask determines whether the resulting device is four-terminal, DTMOS, or floating body. All three types of devices are fabricated simultaneously on the same substrate and may be used as needed for various circuit applications. Next, the trenches are refilled with isolation dielectric (e.g. silicon dioxide) and planarized. This trench dielectric is then patterned and etched out in order to form a “Damascene” metal local interconnect (LI or M
0
) for wiring the top and bottom gates to adjacent circuits. This metal (second gate conductor) is deposited to overfill the trenches, planarized back to the pad layer, and plasma recessed slightly. This recess is then filled with a “cap” dielectric (e
Boise State University
Fourson George
Pham Thanh V
Stoel Rives LLP
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