Semiconductor device manufacturing: process – Making field effect device having pair of active regions...
Reexamination Certificate
2000-04-24
2002-07-16
Dinh, Son T. (Department: 2824)
Semiconductor device manufacturing: process
Making field effect device having pair of active regions...
C438S155000, C438S200000, C438S225000, C438S259000, C438S589000
Reexamination Certificate
active
06420218
ABSTRACT:
FIELD OF THE INVENTION
The present invention relates to integrated circuits (ICs) and methods of manufacturing integrated circuits. More particularly, the present invention relates to integrated circuits having transistors with recessed source/drain regions and methods of manufacturing such integrated circuits.
BACKGROUND OF THE INVENTION
Currently, deep-submicron complementary metal oxide semiconductor (CMOS) is the primary technology for ultra-large scale integrated (ULSI) devices. Over the last two decades, reduction in the size of CMOS transistors has been a principal focus of the microelectronics industry. However, as the sizes of the various components of the transistor are reduced, operational parameters and performance characteristics can change. Appropriate transistor performance must be maintained as transistor size is decreased.
The ULSI circuit can include CMOS field effect transistors (FETs). The transistors can include semiconductor gates disposed between drain and source regions. The drain and source regions are typically heavily doped with a P-type dopant (e.g., boron) or an N-type dopant (e.g., phosphorous).
The drain and source regions generally include a thin extension that is disposed partially underneath the gate to enhance the transistor performance. Shallow source and drain extensions help to achieve immunity to short-channel effects which degrade transistor performance for both N-channel and P-channel transistors. Short-channel effects can cause threshold voltage roll-off and drain-induced barrier-lowering. Controlling short-channel effects is particularly important as transistors become smaller.
Conventional techniques utilize a double implant process to form shallow source and drain extensions. According to the conventional process, the source and drain extensions are formed by providing a transistor gate structure without sidewall spacers on a top surface of a silicon substrate. The silicon substrate is doped on both sides of the gate structure via a conventional doping process, such as, a diffusion process or an ion implantation process. Without the sidewall spacers, the doping process introduces dopants into a thin region (i.e., a region just below the top surface of the substrate and to the sides of the gate structure) to form the drain and source extensions as well as to partially form the drain and source regions.
After the drain and source extensions are formed, silicon dioxide spacers, which abut lateral sides of the gate structure, are provided over the source and drain extensions. The substrate is doped a second time to form deeper source and drain regions. The source and drain extensions are not further doped due to the blocking capability of the silicon dioxide spacer.
As transistors disposed on ICs become smaller, transistors with shallow and ultra-shallow source/drain extensions have become more difficult to manufacture. For example, smaller transistors should have ultra-shallow source and drain extensions with less than 30 nanometer (nm) junction depth. Forming source and drain extensions with junction depths of less than 30 nm is very difficult using conventional fabrication techniques. Conventional ion implantation and diffusion-doping techniques make transistors on the IC susceptible to short-channel effects, which result in a dopant profile tail distribution that extends deep into the substrate. Also, conventional ion implantation techniques have difficulty maintaining shallow source and drain extensions because point defects generated in the bulk semiconductor substrate during ion implantation can cause the dopant to more easily diffuse (transient enhanced diffusion, TED). The diffusion often extends the source and drain extensions vertically into the bulk semiconductor substrate.
Transistors, such as, metal oxide semiconductor field effect transistors (MOSFETs), are generally either bulk semiconductor-type devices or silicon-on-insulator (SOI)-type devices. Most integrated circuits are fabricated in a CMOS process on a bulk semiconductor substrate.
In bulk semiconductor-type devices, transistors, such as, MOSFETs, are built on the top surface of a bulk substrate. The substrate is doped to form source and drain regions, and a conductive layer is provided between the source and drain regions. The conductive layer operates as a gate for the transistor; the gate controls current in a channel between the source and the drain regions. As transistors become smaller, the body thickness of the transistor (or thickness of the depletion layer below the inversion channel) must be scaled down to achieve superior short-channel performance.
Conventional SOI-type devices include an insulative substrate attached to a thin film semiconductor substrate that contains transistors similar to the MOSFETs described with respect to bulk semiconductor-type devices. The insulative substrate generally includes a buried insulative layer above a lower semiconductor base layer. The transistors on the insulative substrate have superior performance characteristics due to the thin film nature of the semiconductor substrate and the insulative properties of the buried insulative layer. In a fully depleted (FD) MOSFET, the body thickness is so small that the depletion region has a limited vertical extension, thereby eliminating link effect and lowering hot carrier degradation. The superior performance of SOI devices is manifested in superior short-channel performance (i.e., resistance to process variation in small size transistor), near-ideal subthreshold voltage swing (i.e., good for low off-state current leakage), and high saturation current. As the physical gate length of MOS transistors shrink to dimensions of 50 nm and below, ultra-thin body MOSFETs fabricated on very thin SOI substrates provide significant architectural advantages. Ultra-thin body MOSFETs may be the enabling technology for terrabit-scale circuit integration (e.g., gate length <50 nm) due to its excellent immunity to short-channel effects, (such as threshold roll-off and drain induced barrier lowering), reduced subthreshold slope (60 mv/decade) and reduction of parasitic capacitance. The body thickness of such devices can be below 200 Angstroms (Å) (e.g., less than 150 Å) to overcome the short-channel effects (e.g., threshold voltage roll-off and drain induced barrier lowering) which tend to be severe in devices with small dimensions.
A major process challenge for fully depleted (FD) SOI devices involves the formation of silicide layers on the source/drain junctions. The source/drain junction generally has the same thickness as the semiconductor film (the silicon layer on the SOI substrate). Semiconductor films on SOI substrates often have thicknesses of less than 150 Å for sub-50 nm devices. Silicide layers often require thicknesses of greater than 350 Å to appropriately reduce sheet resistance at the source/drain junction.
The source regions and drain regions of SOI devices can be raised by selective silicon (SI) epitaxy to make connections to source and drain contacts less difficult. The raised source and drain regions provide additional material for contact silicidation processes while the thinner film in the channel region (active body region) controls short channel effects and reduces subthreshold slope. However, the raised source and drain regions do not necessarily make conventional doping processing for source and drain junctions less challenging especially with respect to transistors with small gate lengths. The spacing between the source and drain regions in devices with gate lengths below 70 nm is extremely narrow (e.g., only 25-30 nm).
According to conventional doping techniques, the dopant (e.g., CoSi
2
) implanted into the source and drain region must be activated at temperatures of 900-1100° C. for several seconds. The high thermal budget associated with conventional doping techniques can produce significant thermal diffusion which can cause a short between the source and drain region. Shorting between the source and drain region is a particular proble
Advanced Micro Devices , Inc.
Dinh Son T.
Foley & Lardner
Luu Pho
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