Field of the Invention
The present invention relates to transistors and particularly to field effect transistors utilizing field plates.
Description of the Related Art
Improvements in the manufacturing of AlGaN/GaN semiconductor materials have helped advance the development of AlGaN/GaN transistors, such as high electron mobility transistors (HEMTs) for high frequency, high temperature and high power applications. AlGaN/GaN has large bandgaps, high peak and saturation electron velocity values [B. Gelmont, K. Kim and M. Shur, Monte Carlo Simulation of Electron Transport in Gallium Nitride, J. Appl. Phys. 74, (1993), pp. 1818-1821].
Electron trapping and the resulting difference between DC and RF characteristics have been a limiting factor in the performance of these devices. Silicon nitride (SiN) passivation has been successfully employed to alleviate this trapping problem resulting in high performance devices with power densities over 10 W/mm at 10 Ghz. For example, U.S. Pat. No. 6,586,781 which is incorporated herein by reference in its entirety discloses methods and structures for reducing the trapping effect in GaN-based transistors. However, due to the high electric fields existing in these structures, charge trapping is still an issue.
Field plates (FP) have been used to enhance the performance of GaN-based HEMTs at microwave frequencies [See S Kamalkar and U. K. Mishra, Very High Voltage AlGaN/GaN High Electron Mobility Transistors Using a Field Plate Deposited on a Stepped Insulator, Solid State Electronics 45, (2001), pp. 1645-1662]. These approaches, however, have involved a field plate connected to the gate of the transistor with the field plate on top of the drain side of the channel. This can result in a significant field plate to drain capacitance and the field plate connected to the gate adds additional gate-to-drain capacitance (Cgd) to the device. This can not only reduce gain, but can also cause instability due to poorer input-output isolation.
The present invention provides improved field effect transistors having a field plate connected to the source electrode. One embodiment of a field effect transistor according to the present invention comprises a metal semiconductor field effect transistor (MESFET) having a buffer layer on a substrate and a channel layer on the buffer layer with the buffer layer sandwiched between the channel layer and substrate. A source electrode is included in electrical contact with said plurality of the channel layer, along with a drain electrode in electrical contact with said channel layer. A gate is included in electrical contact with the channel layer and between the source and drain electrodes. A spacer layer is over at least a portion of the channel layer between the gate and the drain electrode. A field plate is formed on the spacer layer and electrically isolated from the channel layer and gate, with the field plate electrically connected to the source electrode by at least one conductive path.
Another embodiment of a field effect transistor according to the present invention comprises a buffer layer and channel layer formed successively on a substrate. A source electrode, drain electrode, and gate are all formed in electrical contact with the channel layer, with the gate between the source and drain electrodes. A spacer layer is formed on at least a portion of a surface of the channel layer between the gate and drain electrode and a field plate is separately formed on the spacer layer isolated from the gate and channel layer. The spacer layer is electrically connected by at least one conductive path to the source electrode, wherein the field plate reduces the peak operating electric field in the transistor.
Still another embodiment of a transistor according to the present invention comprises a metal semiconductor field effect transistor (MESFET) having a buffer layer and channel layer formed successively on a substrate. Source electrode, drain electrode, and gate are all formed in electrical contact with the channel layer with the gate between the source and drain electrodes. A field plate extends a distance Lf from the edge of the gate to the drain electrode with the field plate isolated from the gate and active layers. At least one conductive path electrically connects the field plate to the source electrode, with the at least one conductive path covering less than all of the topmost surface between the gate and source electrode.
Still another embodiment of a transistor according to the present invention comprises an active region having a channel, source electrode, drain electrode, gate all in electrical contact with the channel layer, with the gate between the source and drain electrodes on the active region. The embodiment further comprises a spacer layer over at least a portion of the active region between the gate and the drain electrode. The embodiment further comprises a field plate on the spacer layer isolated from the active region and gate, the field plate electrically connected to the source electrode by at least one conductive path and extending a distance Lf as measured from the edge of the gate to the drain electrode.
These and other further features and advantages of the invention would be apparent to those skilled in the art from the following detailed description, taking together with the accompanying drawings, in which:
The field plate arrangements according to the present invention can be used with many different transistor structures. Wide bandgap transistor structures generally include an active region, with metal source and drain electrodes formed in electrical contact with the active region, and a gate electrode formed between the source and drain electrodes for modulating electric fields within the active region. A spacer layer is formed above the active region. The spacer layer can comprise a dielectric layer, or a combination of multiple dielectric layers. A conductive field plate is formed on the spacer layer and extends a distance Lf from the edge of the gate electrode toward the drain electrode.
The field plate can be electrically connected to the source electrode. This field plate arrangement can reduce the peak electric field in the device, resulting in increased breakdown voltage and reduced trapping. The reduction of the electric field can also yield other benefits such as reduced leakage currents and enhanced reliability. By having the field plate electrically connected to the source electrode, the reduced gain and instability resulting from gate connected field plates is reduced. When arranged according to the present invention, the shielding effect of a source-connected field plate can reduce Cgd, which enhances input-output isolation.
One type of transistor that can utilize the field plate arrangement according to the present invention is a field effect transistor and particularly a metal semiconductor field effect transistor (MESFET), which typically includes a buffer layer and a channel layer on the buffer layer. A gate electrode is formed on the channel layer between source and drain electrodes.
According to the present invention, a spacer layer is formed on the channel layer covering at least a portion of the channel layer between the gate and drain electrode such that a field plate can be formed on the spacer layer in electric isolation from the channel layer. In other embodiments the spacer layer can also cover all or some of the gate such that the field plate can overlap the gate while remaining in electrical isolation from the gate and the channel layer. In a preferred embodiment the spacer layer covers the gate and the surface of the barrier layer between the gate and the source and drain electrodes. The spacer layer can comprise a dielectric layer, or a combination of multiple dielectric layers. Different dielectric materials can be used such as a SiN, SiO2, Si, Ge, MgOx, MgNx, ZnO, SiNx, SiOx, alloys or layer sequences thereof, or epitaxial materials as further described below.
A conductive field plate is formed on the spacer layer and extends a distance Lf as measured from the edge of the gate towards the drain electrode, with the field plate and gate electrode typically being formed during separate deposition steps. The field plate is electrically connected to the source electrode typically by conductive paths arranged in different ways.
It will be understood that when an element or layer is referred to as being “on”, “connected to”, “coupled to” or “in contact with” another element or layer, it can be directly on, connected or coupled to, or in contact with the other element or layer or intervening elements or layers may be present. In contrast, when an element is referred to as being “directly on,” “directly connected to”, “directly coupled to” or “directly in contact with” another element or layer, there are no intervening elements or layers present. Likewise, when a first element or layer is referred to as being “in electrical contact with” or “electrically coupled to” a second element or layer, there is an electrical path that permits current flow between the first element or layer and the second element or layer. The electrical path may include capacitors, coupled inductors, and/or other elements that permit current flow even without direct contact between conductive elements.
The MESFET 10 further comprises a silicon carbide buffer layer 14 formed on the substrate 12 with a silicon carbide channel layer 16 formed on the buffer, with the buffer layer 14 sandwiched between the channel layer 16 and substrate 12. The buffer and channel layers 14, 16 can be formed on the substrate 12 using known semiconductor growth techniques such as Metal Oxide Chemical Vapor Deposition (MOCVD), Hydride Vapor Phase Epitaxy (HVPE) or Molecular Beam Epitaxy (MBE).
A nucleation layer (not shown) can be included between the substrate 12 and the buffer 14 to reduce any lattice mismatch between the two. The nucleation layer can comprise many different materials, can also be formed on the substrate 12 using MOCVD, HVPE or MBE. The formation of the nucleation layer can depend on the material used for the substrate 12. For example, methods of forming a nucleation layer on various substrates are taught in U.S. Pat. Nos. 5,290,393 and 5,686,738, each of which are incorporated by reference as if fully set forth herein. Methods of forming nucleation layers on silicon carbide substrates are disclosed in U.S. Pat. Nos. 5,393,993, 5,523,589, and 5,739,554 each of which is incorporated herein by reference as if fully set forth herein.
Metal source and drain electrodes 18, 20 are formed in contact with the channel layer 16 and a gate 22 is formed on the channel layer 16 between the source and drain electrodes 18, 20. Electric current can flow between the source and drain electrodes 18, 20 through the channel layer 16 when the gate 22 is biased at the appropriate level. The source and drain contacts 18, 20 can be made of different materials including but not limited to alloys of titanium, aluminum, gold, nickel, platinum, chromium, alloys of titanium and tungsten, or platinum silicide. The gate 22 can have many different lengths, with a preferred gate length (Lg) being approximately 0.5 microns. As best shown in
As best shown in
When the spacer layer 26 is formed before device metallization the spacer layer 26 can comprise an epitaxial material such a Group III nitride material having different Group III elements such as alloys of Al, Ga, or In, with a suitable spacer layer material being AlxGa1-xN (0≦x≦1). After epitaxial growth of the channel layer 16, the spacer layer 26 can be grown using the same epitaxial growth method. The spacer layer 26 is then etched such that the gate 22, source electrode 18 and drain electrode 20 can be properly formed in contact with the channel layer 16 and the spacer layer 26. A field plate 30 can then be deposited on the spacer layer 26 between the gate 22 and drain electrode 20. In those embodiments where the field plate 30 overlaps the gate 22, an additional spacer layer 26 of dielectric material should be included at least partially over the gate 22 to isolate the gate 22 from the field plate 30.
A field plate 30 is formed on the spacer layer 26 between the gate 22 and the drain electrode 20, with the field plate 30 being in close proximity to the gate 22 but not overlapping it. A space between the gate 22 and field plate (Lgf) remains and should be wide enough to isolate from the field plate 30, while being small enough to maximize the field effect provided by the field plate 30. If Lgf is too wide the field effect can be reduced. In one embodiment according to the present invention Lgf can be approximately 0.4 microns or less, although larger and smaller spaces can also be used.
The field plate 30 can extend different distances Lf from the edge of the gate 22, with a suitable range of distances being approximately 0.1 to 2 microns. The field plate 30 can comprise many different conductive materials with a suitable material being a metal, or combinations of metals, deposited using standard metallization methods. In some embodiments according to the present invention the field plate 30 comprises titanium/gold or nickel/gold.
The field plate 30 is electrically connected to the source contact 18 and
Alternatively, the spacer layer 26 can cover only the surface of the channel layer in strips (not shown) between the gate and source electrode, with the strips having a width sufficient to support the conductive busses 32. The busses 32 would then extend from the field plate 30 over those spacer layer areas that cover the channel layer.
The field plate 30 can also be electrically connected to the source contact 20 through a conductive path 34 that runs outside of the active regions and spacer layer 26 of the MESFET 10 and is coupled to the source contact 20. This arrangement can be used in other embodiments but it is particularly adapted for use in embodiments where the spacer layer 26 does not cover the channel layer 16 between the gate 22 and the source 18. As shown in
After deposition of the field plate 30 and its connection to the source electrode 18, the active structure can be covered by a dielectric passivation layer (not shown), such as silicon nitride. The passivation layer can be formed using known growth methods.
The MESFET 40 is preferably silicon carbide based and comprises a silicon carbide substrate 12, silicon carbide buffer layer 14, silicon carbide channel layer 16, source contact 18, drain contact 20, gate 22, gate contact 24 and spacer layer 26. The MESFET 40 also comprises a field plate 42 that is formed on the spacer layer 26 primarily between the gate 22 and the drain contact 20, but also overlapping a portion of the gate 22. For the MESFET 10 in
The source connected field plate arrangement according to the present invention can be used in many different MESFETs beyond those described above. For example,
The gamma gate 52 provides for low gate resistance and allows for controlled definition of the gate footprint. A spacer layer 54 is included that covers the gamma gate 52 and the surface of barrier layer 16 between the gamma gate 52 and the source and drain electrodes 18, 20. A space can remain between the horizontal portion of the gamma gate 52 and the top of the spacer layer 54 between the gate 52 and the source electrode. The MESFET 50 also includes a field plate 56 on the spacer layer 54 that overlaps that gamma gate 52, with the field plate 56 preferably deposited on the side of the gamma gate 52 not having a horizontal overhanging section. This arrangement allows for tight placement and effective coupling between the field plate 56 and the active layers below it. In other gamma gate embodiments the field plate can be similarly arranged to field plate 56, but instead of overlapping the gate, there can be a space between the edge of the gate and the field plate similar to space Lgf shown in
The field plate 56 can be electrically connected to the source electrode 18 in many different ways. Because of the space between the lower surface of the horizontal section of the gate 52 and the spacer layer 54, it can be difficult to provide a conductive path directly between the field plate 56 and the source electrode 18. Instead, a conductive path can be included between the field plate 56 and the source electrode 18 that runs outside the active area of the MESFET 50. Alternatively, the gamma gate 52 can be completely covered by the spacer layer 54 with the space under the gate's horizontal section filled. Conductive paths can then run directly from the field plate 56 to the source electrode over the spacer layer 54. The active structure can then be covered by a dielectric passivation layer (not shown).
The embodiments above provide wide bandgap transistors, particularly MESFETs, with improved power at microwave and millimeter wave frequencies. The MESFETs exhibit simultaneous high gain, high power, and more stable operation due to higher input-output isolation. The structure could be extended to larger dimensions for high voltage applications at lower frequencies.
Although the present invention has been described in considerable detail with reference to certain preferred configurations thereof, other versions are possible. The field plate arrangement can be used in many different devices. The field plates can also have many different shapes and can be connected to the source contact in many different ways. The spirit and scope of the invention should not be limited to the preferred versions of the invention described above.
This application claims the benefit of provisional application Ser. No. 60/571,342 to Wu et al., which was filed on May 13, 2004.
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Number | Date | Country | |
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20050253167 A1 | Nov 2005 | US |
Number | Date | Country | |
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60571342 | May 2004 | US |