HEMT Structure

Abstract: A high electron mobility transistor includes a donor layer of aluminum gallium arsenide (AlGaAs) for forming a two-­ dimensional electron gas (2DEG) in a proximate buffer layer of gallium arsenide. The donor layer has a composition profile including a relatively high concentration of aluminum over a first thickness portion proximate the buffer layer, a low and constant concentration of aluminum over a second thickness portion distal from the buffer layer and a graded concentration of aluminum in a third thickness portion of the donor layer between the first and second thickness portions, transitioning between the high and the low concentrations of aluminum. The donor layer has a doping profile including a high level doping spike in the first thickness portion and a low doping level over the second and third thickness portions.

Description: The present invention relates to field effect transistors (FET's) and more particularly to high electron mobility transistors (HEMT's) utilizing gallium arsenide technology. Such a transistor is a heterostructure of two materials: gallium arsenide (GaAs) and aluminum gallium arsenide (AlGaAs). The heterojunction between them separates electrons from their donor ions and confines conduction path electrons to a potential well in an undoped gallium arsenide layer known as the buffer layer, where they exhibit high mobility. The conduction path electrons form what is known as a two-dimensional electron gas (2DEG), typically about 100 Å (10 Å = 1nm) thick. Electrons forming the 2DEG are supplied from donor ions in a donor layer of AlGaAs formed over the buffer layer, but also sometimes separated from the buffer layer by a thin, undoped AlGaAs layer typically 15-25 Å (10Å = 1 nm) thick, known as the spacer layer. Typically, in conventional devices, the AlGaAs layer is of a constant composition. It is herein recognized and understood that a 2DEG is also typically formed in indium gallium arsenide (InGaAs), sandwitched in between the barrier layer and the buffer layer. A layer of n-doped GaAs, sometimes referred to as a cap layer, is generally formed over the AlGaAs donor layer and a recess in this n-doped GaAs layer has a gate electrode formed therein for controlling conduction by the 2DEG between source and drain electrodes which typically reach through the n-doped GaAs layer into the donor layer and thereby approach the location of the 2DEG so as to provide low-resistance paths thereto. As a result of the band structure in GaAs, electrons provided by donors are not always freely available for conduction. Depending on the aluminum content, donors can appear at a deep energy level in the band-gap and the capture and emission of electrons from such donors, or "DX-centers", is a complex phenomenon which involves relatively slow time-constants and which leads to instabilities in device electrical characteristics. Such instabilities manifest themselves primarily as a change in transconductance with time. Thus, for example, a step change in a gate-source voltage of a transistor exhibiting such effects causes an initial resulting change in drain current which, however, is not sustained with the passage of time, so that the final, resulting change in drain current is smaller than the initial change. Another form of instability relates to temperature behavior, so that the threshold voltage of such a transistor drops drastically when the transistor is cooled below a given temperature, typically 150 degrees Kelvin. When energy level is plotted against aluminum content in AlGaAs, it is found that the lower edge of the conduction band rises as the aluminum content is increased from zero, peaking at a mole fraction of about 0,4. Thereafter, the lower edge of the conduction band drops from this peak with increasing aluminum content. In forming the 2DEG, it is desirable to have a large difference between the conduction band level edges of the GaAs and AlGaAs forming the heterojunction, since it is this difference that constitutes the potential well containing the 2DEG. It has been recognized that problems posed by DX-center instabilities are avoidable by ensuring that DX-center levels are within, or close to, the conduction band. This is because donor electrons in that situation will tend to fall to the lower edge of the conduction band and the effects of electron capture and emission are then no longer appreciably relevant to conduction and therefore are not important causes of instability. However, it is found that the DX-centers are within the conduction band for AlGaAs only when the aluminum mole fraction is less than about 0.2 or greater than 0.7 or so Accordingly, it has generally been the practice to utilize mole fractions of 0.2 or less in making stable devices. However, this limits the available difference between the conduction band levels across the heterojunction, so that the available potential well capacity for forming the 2DEG is limited. The mutual conductance and current-carrying capacity of a device are limited in this manner and high frequency performance is thereby limited. Further HEMTs are disclosed in JP-A-62264672 and FR-A-2620268. JP-A-62264672 features a HEMT with GaAlAs having an extended region of high Al. conc. with uniform doping only. FR-A-2620268 discloses HEMTs with constant Al. conc. and with spike doping at the interface to reduce DX centre influence. Alternative structures have been proposed for avoiding DX-center related problems including a "Superlattice Gate Structure" and a "SISFET". Nevertheless, the present invention is primarily directed to an improved depletion-mode structure of the type having a high aspect ratio and a recessed gate configuration. This object is achieved by a semiconductor device as claimed in claim 1. In the drawing, Figure 1 shows in diagrammatic form a cross-sectional view, not to scale, of a device in accordance with the invention; Figure 2 shows a diagram helpful to an understanding the composition of a device in accordance with the invention; Figure 3 shows a diagram helpful to an understanding the doping profile of a device in accordance with the invention; and Figures 4 and 5 show diagrams helpful to an understanding of the operation of a device in accordance with the invention. In the HEMT structure shown in Figure 1, generally indicated as 10, semi-insulating gallium arsenide (GaAs) substrate 12 has formed over it an undoped GaAs buffer layer 14. A relatively thin spacer layer 16 is formed over buffer layer 14 and over this in turn is a donor layer 18 of aluminum gallium arsenide (AlGaAs), relatively heavily doped, typically with an n-type dopant (n + ). A layer 20 of n + doped GaAs is formed over the n + AlGaAs layer and has a recess 22 formed in it, in which a metallic gate electrode 24 is formed so as to form a Schottky barrier junction with layer 20. A source electrode 26 and a drain electrode 28 are formed to reach through layer 22 into layer 18 so as to provide low resistance connections to a main conduction path. Layer 18 is made with a varying aluminum content, in the form Al x G 1-x As, where x is a variable. The aluminum content is shown in Figure 2, in which the vertical dimension of layer 18 is more conveniently represented by the horizontal axis of Figure 2. The vertical axis represents aluminum content. At the righthand side of Figure 2, a portion of GaAs buffer layer 14 is shown in which the aluminum content is essentially zero. Proceeding to the left, the aluminum content rises abruptly to a level 210 which is above the level below which DX-centers occur in the bandgap region. This level of aluminum content is maintained substantially constant over a region 212, typically 100 Å wide or so. Thereafter, proceeding to the left in Figure 2, the aluminum content drops rapidly with distance, in accordance with a higher order curve 214, for example, a parabola. At a level 216, corresponding to the level referred to in the introductory portion of the specification below which the DX-centers are within the conduction band, that ist, when the aluminum mole fraction is 0.2 or so, the aluminum content thereafter remains relatively constant, until it decreases to zero in the vicinity of layer 20 and gate electrode 24. Figure 3 shows the doping profile in layer 18. Beginning at the right-hand side of Figure 3, the region corresponding to spacer layer 16 is left substantially undoped. A high level of doping 310, in a so-called doping "spike" 311 ist formed in a relatively narrow region 314, slightly narrower and included within region 312, corresponding to region 212. Thereby, abrupt changes in doping are made not to coincide with abrupt changes in aluminum content composition. To the left of doping spike 311, the doping level is maintained relatively constant at a level 316 which is preferably between from one-third to one-fifth (1/3-1/5) the doping level 310 of spike 312. Typically, the distance between spike 311 and gate electrode 24 is in the order of 200 A. Doping spike 311 is in the order of 60 A wide. Region 212 of high aluminum content typically extends 3 to 4 monolayers beyond doping spike 311 on the right-hand side and on the left-hand side. The peak level 310 of doping in spike 311 is in the order of 5 x 10 18 to 8 x 10 18 cm -3 . In operation, electrons tunnelling from layer 18 form a two-dimensional electron gas (2DEG) in the potential well at heterojunction 17 between layer 16 and layer 18, resulting from the disparity in their conduction band levels. Since the aluminum concentration is high in region 212, DX-centers appear there within the bandgap level. However, because of the proximity to the 2DEG potential well, electrons resulting from such DX-centers in this region will gravitate into the potential well leaving the DX-centers ionized and therefore not able to pose problems of instability. An abrupt drop of aluminum content on the gate side of region 212, i.e. the left side in Figure 2, would give rise to the possibility of a bandgap discontinuity on that side and would lead to the presence of another 2DEG where it is not desired. In accordance with the present invention, this drop is made gradual, as has been explained, so that no appreciable bandgap discontinuity occurs. The doping level to the left of doping spike 311 in Figure 3 is maintained at a fractional level 316 of the peak level 310 in part to reduce any tendency to drift into this region of electrons which are otherwise available for contribution to the 2DEG to the right of spike 311. Figure 4 shows an energy band diagram for a device in accordance with the present invention, the abscissa representing layer 18 with a portion of layer 14 to the right. In Figure 4, conditions for zero gate bias are shown, the 2DEG being indicated by reference numeral 415. DX-centers shown as crosses in Figures 4 and 5, in the region immediately to the left of the discontinuity are ionized and generate the 2DEG and are in a region of positive slope. The potential minimum is on the left side, towards the gate. Figure 5 shows conditions with positive gate bias. Since the aluminum concentration is sufficiently low (less than 0.2) over the center region, DX-centers do not occur below the conduction band edge. While the invention has been described by way of an exemplary embodiment, the invention is not limited thereto. Various modifications in the composition profile, doping concentration, layer thicknesses and the like will be apparent to one of skill in the art. Such changes are contemplated to be within the scope of the invention as defined by the claims following. In the region 212 in Figure 2, the aluminum concentration is substantially constant. In the region 212, the aluminum concentration is preferably between 0,2 and 0,4 or between 0,7 and 1. In the range between 0,2 and 0,4, an aluminum concentration between 0,25 and 0,35, especially around 0,3, is even more preferred. A HEMT according to the invention makes possible a high doping concentration near the buffer layer and resulting therefrom a high electron concentration of the two-dimensional electron gas (2DEG) in the buffer layer. This is even true for an aluminum concentration of 1 (x=1), i.e. for pure AlAs, in the region 212. Thus, doping of even pure AlAs in the region 212 makes possible a high electron concentration of the two-dimensional electron gas (2DEG) in the buffer layer.

Claims: A high electron mobility transistor (10), including a first 1ayer (14) of substantially undoped gallium arsenide and a second layer (18) of doped aluminium gallium arsenide, reprensentable as Al x Ga 1-x As, proximate to said first layer, wherein said second layer comprises: proximate to said first layer, an aluminum content of a first value (212) at which DX-centers occur below a conduction-band edge of said second layer; said aluminum content remaining substantially at said first value across a first portion of a thickness dimension of said second layer, thence decreasing (214) to a second value over a second portion df said thickness dimension and thence remaining substantially at said second value (216) across a third portion of said thickness dimension; at said second value DX-centers occur within or close to the conduction band of said second layer; said first portion and said second portion being relatively thin compared with said third portion; a high doping concentration spike (314) being substantially contained within said first portion of said thickness dimension; and a low and constant doping concentration (316) over said second and third portion of said thickness dimension. A high electron mobility transistor as recited in claim 1, wherein said aluminium content decreases monotonically over said second portion of said thickness dimension to said second value. A high electron mobility transistor as recited in claim 2, wherein said aluminium content decreases in a generally parabolic manner. A high electron mobility transistor, as recited in any one of claims 1 to 3, wherein said first portion is in the order of less than 100 Å (10Å = 1nm) thick and said third portion is in the order of 200 Å (10Å = 1nm) thick. A high electron mobility transistor as recited in any one of claims 1 to 4, wherein said high doping concentration is in the order of from three times to five times said low doping concentration. A high electron mobility transistor as recited in any one of claims 1 to 5, wherein said second value of aluminum content is not greater than a mole fraction in the order of 0.2. A high electron mobility transistor as recited in any one of claims 1 to 6, including an undoped spacer layer between said first layer and said second layer. A high electron mobility transistor as recited in any one of claims 1 to 7, wherein said high doping concentration spike associated with said first portion and said low and constant doping concentration over said second and third portions are in a ratio exceeding 2.

Inventors: KOHN ERHARD PROF DR, KOHN, ERHARD, PROF, DR.
Applicants: SIEMENS AG, SIEMENS AKTIENGESELLSCHAFT
Application year: 1990
Main classification: H01L29
IPC codes: H01L29