Advanced transistors with punch through suppression

Abstract

An advanced transistor with punch through suppression includes a gate with length Lg, a well doped to have a first concentration of a dopant, and a screening region positioned under the gate and having a second concentration of dopant. The second concentration of dopant may be greater than 5×1018 dopant atoms per cm3. At least one punch through suppression region is disposed under the gate between the screening region and the well. The punch through suppression region has a third concentration of a dopant intermediate between the first concentration and the second concentration of dopant. A bias voltage may be applied to the well region to adjust a threshold voltage of the transistor.

Description

FIELD OF THE INVENTION

This disclosure relates to structures and processes for forming advanced transistors with improved operational characteristics, including enhanced punch through suppression.

BACKGROUND OF THE INVENTION

Fitting more transistors onto a single die is desirable to reduce cost of electronics and improve their functional capability. A common strategy employed by semiconductor manufacturers is to simply reduce gate size of a field effect transistor (FET), and proportionally shrink area of the transistor source, drain, and required interconnects between transistors. However, a simple proportional shrink is not always possible because of what are known as “short channel effects”. Short channel effects are particularly acute when channel length under a transistor gate is comparable in magnitude to depletion depth of an operating transistor, and include reduction in threshold voltage, severe surface scattering, drain induced barrier lowering (DIBL), source-drain punch through, and electron mobility issues.

Conventional solutions to mitigate some short channel effects can involve implantation of pocket or halo implants around the source and the drain. Halo implants can be symmetrical or asymmetrical with respect to a transistor source and drain, and typically provide a smoother dopant gradient between a transistor well and the source and drains. Unfortunately, while such implants improve some electrical characteristics such as threshold voltage rolloff and drain induced barrier lowering, the resultant increased channel doping adversely affects electron mobility, primarily because of the increased dopant scattering in the channel.

Many semiconductor manufacturers have attempted to reduce short channel effects by employing new transistor types, including fully or partially depleted silicon on insulator (SOI) transistors. SOI transistors are built on a thin layer of silicon that overlies an insulator layer, have an undoped or low doped channel that minimizes short channel effects, and do not require either deep well implants or halo implants for operation. Unfortunately, creating a suitable insulator layer is expensive and difficult to accomplish. Early SOI devices were built on insulative sapphire wafers instead of silicon wafers, and are typically only used in specialty applications (e.g. military avionics or satellite) because of the high costs. Modern SOI technology can use silicon wafers, but require require expensive and time consuming additional wafer processing steps to make an insulative silicon oxide layer that extends across the entire wafer below a surface layer of device-quality single-crystal silicon.

One common approach to making such a silicon oxide layer on a silicon wafer requires high dose ion implantation of oxygen and high temperature annealing to form a buried oxide (BOX) layer in a bulk silicon wafer. Alternatively, SOI wafers can be fabricated by bonding a silicon wafer to another silicon wafer (a “handle” wafer) that has an oxide layer on its surface. The pair of wafers are split apart, using a process that leaves a thin transistor quality layer of single crystal silicon on top of the BOX layer on the handle wafer. This is called the “layer transfer” technique, because it transfers a thin layer of silicon onto a thermally grown oxide layer of the handle wafer.

As would be expected, both BOX formation or layer transfer are costly manufacturing techniques with a relatively high failure rate. Accordingly, manufacture of SOI transistors not an economically attractive solution for many leading manufacturers. When cost of transistor redesign to cope with “floating body” effects, the need to develop new SOI specific transistor processes, and other circuit changes is added to SOI wafer costs, it is clear that other solutions are needed.

Another possible advanced transistor that has been investigated uses multiple gate transistors that, like SOI transistors, minimize short channel effects by having little or no doping in the channel. Commonly known as a finFET (due to a fin-like shaped channel partially surrounded by gates), use of finFET transistors has been proposed for transistors having 28 nanometer or lower transistor gate size. But again, like SOI transistors, while moving to a radically new transistor architecture solves some short channel effect issues, it creates others, requiring even more significant transistor layout redesign than SOI. Considering the likely need for complex non-planar transistor manufacturing techniques to make a finFET, and the unknown difficulty in creating a new process flow for finFET, manufacturers have been reluctant to invest in semiconductor fabrication facilities capable of making finFETs.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 illustrates a DDC transistor with a punch through suppression;

FIG. 2 illustrates a dopant profile of a DDC transistor with enhanced punch through suppression;

FIGS. 3-7 illustrate alternative useful dopant profiles; and

FIG. 8 is a flow diagram illustrating one exemplary process for forming a DDC transistor with a punch through suppression.

DETAILED DESCRIPTION

Unlike silicon on insulator (SOI) transistors, nanoscale bulk CMOS transistors (those typically having a gate length less than 100 nanometers) are subject to significant adverse short channel effects, including body leakage through both drain induced barrier lowering (DIBL) and source drain punch through. Punch through is associated with the merging of source and drain depletion layers, causing the drain depletion layer to extend across a doped substrate and reach the source depletion layer, creating a conduction path or leakage current between the source and drain. This results in a substantial increase in required transistor electrical power, along with a consequent increase in transistor heat output and decrease in operational lifetime for portable or battery powered devices using such transistors.

An improved transistor manufacturable on bulk CMOS substrates is seen in FIG. 1. A Field Effect Transistor (FET) 100 is configured to have greatly reduced short channel effects, along with enhanced punch through suppression according to certain described embodiments. The FET 100 includes a gate electrode 102, source 104, drain 106, and a gate dielectric 108 positioned over a channel 110. In operation, the channel 110 is deeply depleted, forming what can be described as deeply depleted channel (DDC) as compared to conventional transistors, with depletion depth set in part by a highly doped screening region 112. While the channel 110 is substantially undoped, and positioned as illustrated above a highly doped screening region 112, it may include simple or complex layering with different dopant concentrations. This doped layering can include a threshold voltage set region 111 with a dopant concentration less than screening region 112, optionally positioned between the gate dielectric 108 and the screening region 112 in the channel 110. A threshold voltage set region 111 permits small adjustments in operational threshold voltage of the FET 100, while leaving the bulk of the channel 110 substantially undoped. In particular, that portion of the channel 110 adjacent to the gate dielectric 108 should remain undoped. Additionally, a punch through suppression region 113 is formed beneath the screening region 112. Like the threshold voltage set region 111, the punch through suppression region 113 has a dopant concentration less than screening region 112, while being higher than the overall dopant concentration of a lightly doped well substrate 114.

In operation, a bias voltage 122 V_BS may be applied to source 104 to further modify operational threshold voltage, and P+ terminal 126 can be connected to P-well 114 at connection 124 to close the circuit. The gate stack includes a gate electrode 102, gate contact 118 and a gate dielectric 108. Gate spacers 130 are included to separate the gate from the source and drain, and optional Source/Drain Extensions (SDE) 132, or “tips” extend the source and drain under the gate spacers and gate dielectric 108, somewhat reducing the gate length and improving electrical characteristics of FET 100.

In this exemplary embodiment, the FET 100 is shown as an N-channel transistor having a source and drain made of N-type dopant material, formed upon a substrate as P-type doped silicon substrate providing a P-well 114 formed on a substrate 116. However, it will be understood that, with appropriate change to substrate or dopant material, a non-silicon P-type semiconductor transistor formed from other suitable substrates such as Gallium Arsenide based materials may be substituted. The source 104 and drain 106 can be formed using conventional dopant implant processes and materials, and may include, for example, modifications such as stress inducing source/drain structures, raised and/or recessed source/drains, asymmetrically doped, counter-doped or crystal structure modified source/drains, or implant doping of source/drain extension regions according to LDD (low doped drain) techniques. Various other techniques to modify source/drain operational characteristics can also be used, including, in certain embodiments, use of heterogeneous dopant materials as compensation dopants to modify electrical characteristics.

The gate electrode 102 can be formed from conventional materials, preferably including, but not limited to, metals, metal alloys, metal nitrides and metal silicides, as well as laminates thereof and composites thereof. In certain embodiments the gate electrode 102 may also be formed from polysilicon, including, for example, highly doped polysilicon and polysilicon-germanium alloy. Metals or metal alloys may include those containing aluminum, titanium, tantalum, or nitrides thereof, including titanium containing compounds such as titanium nitride. Formation of the gate electrode 102 can include silicide methods, chemical vapor deposition methods and physical vapor deposition methods, such as, but not limited to, evaporative methods and sputtering methods. Typically, the gate electrode 102 has an overall thickness from about 1 to about 500 nanometers.

The gate dielectric 108 may include conventional dielectric materials such as oxides, nitrides and oxynitrides. Alternatively, the gate dielectric 108 may include generally higher dielectric constant dielectric materials including, but not limited to hafnium oxides, hafnium silicates, zirconium oxides, lanthanum oxides, titanium oxides, barium-strontium-titanates and lead-zirconate-titanates, metal based dielectric materials, and other materials having dielectric properties. Preferred hafnium-containing oxides include HfO₂, HfZrO_x, HfSiO_x, HfTiO_x, HfAlO_x, and the like. Depending on composition and available deposition processing equipment, the gate dielectric 108 may be formed by such methods as thermal or plasma oxidation, nitridation methods, chemical vapor deposition methods (including atomic layer deposition methods) and physical vapor deposition methods. In some embodiments, multiple or composite layers, laminates, and compositional mixtures of dielectric materials can be used. For example, a gate dielectric can be formed from a SiO₂-based insulator having a thickness between about 0.3 and 1 nm and the hafnium oxide based insulator having a thickness between 0.5 and 4 nm. Typically, the gate dielectric has an overall thickness from about 0.5 to about 5 nanometers.

The channel region 110 is formed below the gate dielectric 108 and above the highly doped screening region 112. The channel region 110 also contacts and extends between, the source 104 and the drain 106. Preferably, the channel region includes substantially undoped silicon having a dopant concentration less than 5×10¹⁷ dopant atoms per cm³ adjacent or near the gate dielectric 108. Channel thickness can typically range from 5 to 50 nanometers. In certain embodiments the channel region 110 is formed by epitaxial growth of pure or substantially pure silicon on the screening region.

As disclosed, the threshold voltage set region 111 is positioned under the gate dielectric 108, spaced therefrom, and above screening region 112, and is typically formed as a thin doped layer. Suitably varying dopant concentration, thickness, and separation from the gate dielectric and the screening region allows for controlled slight adjustments of threshold voltage in the operating FET 100. In certain embodiments, the threshold voltage set region 111 is doped to have a concentration between about 1×10¹⁸ dopant atoms per cm³ and about 1×10¹⁹ dopant atoms per cm³. The threshold voltage set region 111 can be formed by several different processes, including 1) in-situ epitaxial doping, 2) epitaxial growth of a thin layer of silicon followed by a tightly controlled dopant implant, 3) epitaxial growth of a thin layer of silicon followed by dopant diffusion of atoms from the screening region 112, or 4) by any combination of these processes (e.g. epitaxial growth of silicon followed by both dopant implant and diffusion from the screening layer 112).

Position of a highly doped screening region 112 typically sets depth of the depletion zone of an operating FET 100. Advantageously, the screening region 112 (and associated depletion depth) are set at a depth that ranges from one comparable to the gate length (Lg/1) to a depth that is a large fraction of the gate length (Lg/5). In preferred embodiments, the typical range is between Lg/3 to Lg/1.5. Devices having an Lg/2 or greater are preferred for extremely low power operation, while digital or analog devices operating at higher voltages can often be formed with a screening region between Lg/5 and Lg/2. For example, a transistor having a gate length of 32 nanometers could be formed to have a screening region that has a peak dopant density at a depth below the gate dielectric of about 16 nanometers (Lg/2), along with a threshold voltage set region at peak dopant density at a depth of 8 nanometers (Lg/4).

In certain embodiments, the screening region 112 is doped to have a concentration between about 5×10¹⁸ dopant atoms per cm³ and about 1×10²⁰ dopant atoms per cm³, significantly more than the dopant concentration of the undoped channel, and at least slightly greater than the dopant concentration of the optional threshold voltage set region 111. As will be appreciated, exact dopant concentrations and screening region depths can be modified to improve desired operating characteristics of FET 100, or to take in to account available transistor manufacturing processes and process conditions.

To help control leakage, the punch through suppression region 113 is formed beneath the screening region 112. Typically, the punch through suppression region 113 is formed by direct implant into a lightly doped well, but it may be formed by out-diffusion from the screening region, in-situ growth, or other known process. Like the threshold voltage set region 111, the punch through suppression region 113 has a dopant concentration less than the screening region 112, typically set between about 1×10¹⁸ dopant atoms per cm³ and about 1×10¹⁹ dopant atoms per cm³. In addition, the punch through suppression region 113 dopant concentration is set higher than the overall dopant concentration of the well substrate. As will be appreciated, exact dopant concentrations and depths can be modified to improve desired operating characteristics of FET 100, or to take in to account available transistor manufacturing processes and process conditions.

Forming such a FET 100 is relatively simple compared to SOI or finFET transistors, since well developed and long used planar CMOS processing techniques can be readily adapted.

Together, the structures and the methods of making the structures allow for FET transistors having both a low operating voltage and a low threshold voltage as compared to conventional nanoscale devices. Furthermore, DDC transistors can be configured to allow for the threshold voltage to be statically set with the aid of a voltage body bias generator. In some embodiments the threshold voltage can even be dynamically controlled, allowing the transistor leakage currents to be greatly reduced (by setting the voltage bias to upwardly adjust the V_T for low leakage, low speed operation), or increased (by downwardly adjusting the V_T for high leakage, high speed operation). Ultimately, these structures and the methods of making structures provide for designing integrated circuits having FET devices that can be dynamically adjusted while the circuit is in operation. Thus, transistors in an integrated circuit can be designed with nominally identical structure, and can be controlled, modulated or programmed to operate at different operating voltages in response to different bias voltages, or to operate in different operating modes in response to different bias voltages and operating voltages. In addition, these can be configured post-fabrication for different applications within a circuit.

As will be appreciated, concentrations of atoms implanted or otherwise present in a substrate or crystalline layers of a semiconductor to modify physical and electrical characteristics of a semiconductor are be described in terms of physical and functional regions or layers. These may be understood by those skilled in the art as three-dimensional masses of material that have particular averages of concentrations. Or, they may be understood as sub-regions or sub-layers with different or spatially varying concentrations. They may also exist as small groups of dopant atoms, regions of substantially similar dopant atoms or the like, or other physical embodiments. Descriptions of the regions based on these properties are not intended to limit the shape, exact location or orientation. They are also not intended to limit these regions or layers to any particular type or number of process steps, type or numbers of layers (e.g., composite or unitary), semiconductor deposition, etch techniques, or growth techniques utilized. These processes may include epitaxially formed regions or atomic layer deposition, dopant implant methodologies or particular vertical or lateral dopant profiles, including linear, monotonically increasing, retrograde, or other suitable spatially varying dopant concentration. To ensure that desired dopant concentrations are maintained, various dopant anti-migration techniques, are contemplated, including low temperature processing, carbon doping, in-situ dopant deposition, and advanced flash or other annealing techniques. The resultant dopant profile may have one or more regions or layers with different dopant concentrations, and the variations in concentrations and how the regions or layers are defined, regardless of process, may or may not be detectable via techniques including infrared spectroscopy, Rutherford Back Scattering (RBS), Secondary Ion Mass Spectroscopy (SIMS), or other dopant analysis tools using different qualitative or quantitative dopant concentration determination methodologies.

To better appreciate one possible transistor structure, FIG. 2 illustrates a dopant profile 202 of a deeply depleted transistor taken at midline between a source and drain, and extending downward from a gate dielectric toward a well. Concentration is measured in number of dopant atoms per cubic centimeter, and downward depth is measured as a ratio of gate length Lg. Measuring as a ratio rather than absolute depth in nanometers better allows cross comparison between transistors manufactured at different nodes (e.g 45 nm, 32 nm, 22 nm, or 15 nm) where nodes are commonly defined in term of minimum gate lengths.

As seen in FIG. 2, the region of the channel 210 adjacent to the gate dielectric is substantially free of dopants, having less than 5×10¹⁷ dopant atoms per cm³ to a depth of nearly Lg/4. A threshold voltage set region 211 increases the dopant concentration to about 3×10¹⁸ dopant atoms per cm³, and the concentration increases another order of magnitude to about 3×10¹⁸ dopant atoms per cm³ to form the screening region 212 that sets the base of the depletion zone in an operating transistor. A punch through suppression region 213 region having a dopant concentration of about 1×10¹⁹ dopant atoms per cm³ at a depth of about Lg/1 is intermediate between the screening region and the lightly doped well 214. Without the punch through suppression region, a transistor constructed to have, for example, a 30 nm gate length and an operating voltage of 1.0 volts would be expected to have significantly greater leakage. When the disclosed punch through suppression region is implanted, punch through leakage is reduced, making the transistor more power efficient, and better able to tolerate process variations in transistor structure without punch through failure.

This is better seen with respect to the following Table 1, which indicates expected performance improvements for a range of punch through dosage and threshold voltage:

	TABLE 1
	Ioff (nA/um)	Idsat (mA/um)	Vt (V)
Target Punchthrough layer	2	0.89	0.31
No Punchthrough layer	70	1	0.199
Higher Dose Punchthrough	0.9	0.54	0.488
Very deep Punchthrough	15	1	0.237

Alternative dopant profiles are contemplated. As seen in FIG. 3, an alternative dopant profile 203 that includes a slightly increased depth for the low doped channel is shown. In contrast to the embodiments of FIG. 2, the threshold voltage set region 211 is a shallow notch primarily formed by out-diffusion into an epitaxially deposited layer of silicon from the screening region 212. The screening region 212 itself is set to have a dopant concentration greater than 3×10¹⁹ dopant atoms per cm³. The punch through suppression region 213 has a dopant concentration of about 8×10¹⁸ dopant atoms per cm³, provided by a combination of out-diffusion from the screening region 212 and a separate low energy implant.

As seen in FIG. 4, an alternative dopant profile 204 that includes a greatly increased depth for the low doped channel is shown. In contrast to the embodiments of FIGS. 2 and 3, there is no distinct notch, plane or layer to aid in threshold voltage setting. The screening region 212 is set to be greater than 3×10¹⁹ dopant atoms per cm³ and the punch through suppression region 213 has a similarly high, yet narrowly defined dopant concentration of about 8×10¹⁸ dopant atoms per cm³, provided by a separate low energy implant.

Yet another variation in dopant profile is seen in FIG. 5, which illustrates a transistor dopant profile 205 for a transistor structure that includes a very low doped channel 210. The threshold voltage set region 211 is precisely formed by in-situ or well controlled implant doping of thin epitaxial layer grown on the screening region. The screening region 212 is set to be about 1×10¹⁹ dopant atoms per cm³ and the punch through suppression region 213 also has narrowly defined dopant concentration of about 8×10¹⁸ dopant atoms per cm³, provided by with a separate low energy implant. The well implant 214 concentration is gradually reduced to about 5×10¹⁷ dopant atoms per cm³.

As seen in FIG. 6, a dopant profile 206 includes a low doped channel 210 adjacent to the gate dielectric, and a narrowly defined threshold voltage set region 211. The screening region 212 increases to a narrow peak set to be about 1×10¹⁹ dopant atoms per cm³ and the punch through suppression region 213 also has broadly peak dopant concentration of about 5×10¹⁸ dopant atoms per cm³, provided by with a separate low energy implant. The well implant 214 concentration is high to improve bias coefficient of the transistor, with a concentration of about 8×10¹⁷ dopant atoms per cm³.

In contrast to the narrow screen region peak dopant concentration of FIG. 6, the dopant profile 207 of FIG. 7 has a broad peak 212. In addition to a narrow undoped channel 210, the transistor structure includes a well defined partially retrograde threshold set 211, and a distinct separate punch through suppression peak 213. The well 214 doping concentration is relatively low, less than about 5×10¹⁷ dopant atoms per cm³.

FIG. 8 is a schematic process flow diagram 300 illustrating one exemplary process for forming a transistor with a punch through suppression region and a screening region suitable for different types of FET structures, including both analog and digital transistors. The process illustrated here is intended to be general and broad in its description in order not to obscure the inventive concepts, and more detailed embodiments and examples are set forth below. These along with other process steps allow for the processing and manufacture of integrated circuits that include DDC structured devices together with legacy devices, allowing for designs to cover a full range of analog and digital devices with improved performance and lower power.

In Step 302, the process begins at the well formation, which may be one of many different processes according to different embodiments and examples. As indicated in 303, the well formation may be before or after STI (shallow trench isolation) formation 304, depending on the application and results desired. Boron (B), indium (I) or other P-type materials may be used for P-type implants, and arsenic (As) or phosphorous (P) and other N-type materials may be used for N-type implants. For the PMOS well implants, the P+ implant may be implanted within a range from 10 to 80 keV, and at NMOS well implants, the boron implant B+ implant may be within a range of 0.5 to 5 keV, and within a concentration range of 1×10¹³ to 8×10¹³/cm². A germanium implant Ge+, may be performed within a range of 10 to 60 keV, and at a concentration of 1×10¹⁴ to 5×10¹⁴/cm². To reduce dopant migration, a carbon implant, C+ may be performed at a range of 0.5 to 5 keV, and at a concentration of 1×10¹³ to 8×10¹³/cm². Well implants may include sequential implant, and/or epitaxial growth and implant, of punch through suppression regions, screen regions having a higher dopant density than the punch through suppression region, and threshold voltage set regions (which previously discussed are typically formed by implant or diffusion of dopants into a grown epitaxial layer on the screening region).

In some embodiments the well formation 302 may include a beam line implant of Ge/B (N), As (P), followed by an epitaxial (EPI) pre-clean process, and followed finally non-selective blanket EPI deposition, as shown in 302A. Alternatively, the well may be formed using a plasma implant of B (N), As (P), followed by an EPI pre-clean, then finally a non-selective (blanket) EPI deposition, 302B. The well formation may alternatively include a solid-source diffusion of B(N), As(P), followed by an EPI pre-clean, and followed finally by a non-selective (blanket) EPI deposition, 302C. The well formation may alternatively include a solid-source diffusion of B(N), As(P), followed by an EPI pre-clean, and followed finally by a non-selective (blanket) EPI deposition, 302D. As yet another alternative, well formation may simply include well implants, followed by in-situ doped selective EPI of B (N), P (P). Embodiments described herein allow for any one of a number of devices configured on a common substrate with different well structures and according to different parameters.

Shallow trench isolation (STI) formation 304, which, again, may occur before or after well formation 302, may include a low temperature trench sacrificial oxide (TSOX) liner 304A at a temperature lower than 900° C. The gate stack 306 may be formed or otherwise constructed in a number of different ways, from different materials, and of different work functions. One option is a poly/SiON gate stack 306A. Another option is a gate-first process 306B that includes SiON/Metal/Poly and/or SiON/Poly, followed by High-K/Metal Gate. Another option, a gate-last process 306C includes a high-K/metal gate stack wherein the gate stack can either be formed with “Hi-K first-Metal gate last” flow or a and “Hi-K last-Metal gate last” flow. Yet another option, 306D is a metal gate that includes a tunable range of work functions depending on the device construction, N(NMOS)/P(PMOS)/N(PMOS)/P(NMOS)/Mid-gap or anywhere in between. In one example, N has a work function (WF) of 4.05V±200 mV, and P has a WF of 5.01V±200 mV.

Next, in Step 308, Source/Drain tips may be implanted, or optionally may not be implanted depending on the application. The dimensions of the tips can be varied as required, and will depend in part on whether gate spacers (SPCR) are used. In one option, there may be no tip implant in 308A. Next, in optional steps 310 and 312, PMOS or NMOS EPI layers may be formed in the source and drain regions as performance enhancers for creating strained channels. For gate-last gate stack options, in Step 314, a Gate-last module is formed. This may be only for gate-last processes 314A.

Die supporting multiple transistor types, including those with and without a punch through suppression, those having different threshold voltages, and with and without static or dynamic biasing are contemplated. Systems on a chip (SoC), advanced microprocessors, radio frequency, memory, and other die with one or more digital and analog transistor configurations can be incorporated into a device using the methods described herein. According to the methods and processes discussed herein, a system having a variety of combinations of DDC and/or transistor devices and structures with or without punch through suppression can be produced on silicon using bulk CMOS. In different embodiments, the die may be divided into one or more areas where dynamic bias structures, static bias structures or no-bias structures exist separately or in some combination. In a dynamic bias section, for example, dynamically adjustable devices may exist along with high and low V_T devices and possibly DDC logic devices.

While certain exemplary embodiments have been described and shown in the accompanying drawings, it is to be understood that such embodiments are merely illustrative of and not restrictive on the broad invention, and that this invention not be limited to the specific constructions and arrangements shown and described, since various other modifications may occur to those ordinarily skilled in the art.

Accordingly, the specification and drawings are to be regarded in an illustrative rather than a restrictive sense.

Claims

1. A field effect transistor structure having a gate dielectric under a gate with length Lg, comprising: a substrate,a well in the substrate doped to have a first concentration of a dopant,an undoped channel under the gate dielectric and extending to a source and a drain,a screening region positioned in the well and under the gate dielectric, the screening region extending to the source and drain and having a second concentration of dopant greater than 5×1018 dopant atoms per cm3,at least one punch through suppression region having a third concentration of a dopant intermediate between the first concentration and the second concentration of dopant, with the punch through suppression region positioned in the well under the gate dielectric and beneath the screening region,a threshold voltage set region having a fourth dopant concentration intermediate between the second concentration and 5×1017 dopant atoms per cm3, with the threshold voltage set region positioned under and spaced from the gate dielectric, the threshold voltage set region extending to the source and drain.

2. The field effect transistor structure of claim 1, wherein the screening region is positioned at a depth below the gate dielectric of between about Lg/5 and about Lg/1.

3. The field effect transistor structure of claim 1, wherein the screening region is positioned at a depth below the gate dielectric of greater than Lg/2.

4. The field effect transistor structure of claim 1, wherein the channel comprises an epitaxially grown layer.

5. The field effect transistor structure of claim 1, wherein the channel is formed as a blanket epitaxial layer.

6. The field effect transistor structure of claim 1, wherein the screening region sets a depletion depth for the field effect transistor structure.

7. The field effect transistor structure of claim 1, wherein the threshold voltage set region is formed as an epitaxial layer.

8. The field effect transistor structure of claim 7, further comprising a shallow trench isolation region.