Low resistance gallium arsenide field effect transistor
The Government has rights to this invention pursuant to a Government contract. 
    
    
     This is a division of application Ser. No. 459,756, filed Jan. 21, 1983. 
    
    
     BACKGROUND OF THE INVENTION 
     This invention relates to semiconductor devices and the processing thereof and more particularly to III-V compound devices and a method of producing such field effect transistors. 
     With the advent of higher frequency semiconductor devices, especially in the field of gallium arsenide Field Effect Transistors (FET), there is a need for decreasing the source-to-gate resistance as well as the drain-to-gate resistance in order to more effectively operate at the higher frequency. Accordingly, the prior art methods of manufacturing gallium arsenide FET&#39;s which are to operate at these higher frequencies must be reviewed since these prior methods tend to produce devices that are frequency limited, i.e. they exhibit excessive amounts of resistance, inductance as well as capacitance. Especially in devices to be operted in the gigahertz portion of the spectrum and higher, the inductance associated with the gate, source and drain contacts must be carefully tailored in order to prevent any unnecessary frequency limiting inductance. Similarly, if the device is to be operated in the gigahertz portion of the radio frequency spectrum, the source-to-gate resistance as well as the drain-to-gate resistance must be maintained as low as possible. 
     One method of producing a gallium arsenide FET is described in my U.S. Pat. No. 4,266,333 which issued on May 12, 1981 entitled &#34;METHOD OF MAKING A SCHOTTKY BARRIER FIELD EFFECT TRANSISTOR&#34; and assigned to the same assignee as the subject application. In my prior patent, a metal layer is first formed on a layer of gallium arsenide material and is subsequently defined to form spaced source and drain contacts. The structure is then covered with a thick layer of insulating material which is then masked and subjected to an isotropic etch. Thereafter, the gate member is deposited in the opening formed by the etch. While the above mentioned patent describes a viable method for producing gallium arsenide FET&#39;s the device so produced tends to have a limited upper frequency. Accordingly, I have devised the method of the subject application for producing a structure having reduced source-to-gate resistance as well as reduced drain-to-gate resistance and has the additional advantage of providing a very short gate contact. The net effect is to lower both the inductive and capacitive reactance and thus produce a device which will operate at higher frequencies than heretofore possible. 
     SUMMARY OF THE INVENTION 
     In the subject application, the described novel device and process achieves the desired high frequency gallium arsenide FET by first forming a highly n+ doped gallium arsenide layer on a wafer of undoped, semi-insulating gallium arsenide. A mesa is then formed on the top surface of the substrate. The next steps of masking and defining a gate region will, by its very method, also define the source and drain regions. Thereafter, the channel region is regrown between the source and drain regions. By using this method, the channel dimension is minimized and thus provides a device having low resistance as well as reduced inductance and capacitance. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     FIGS. 1-10 inclusive, represent cross-sectional, elevational views of the process of one embodiment of the subject invention indicating the resultant structures during the processing of forming a high frequency gallium arsenide FET. 
     FIGS. 11 and 12 inclusive represent cross-sectional, elevational views of a variation in the processing steps of the subject invention for forming another embodiment of my novel device. 
    
    
     DETAILED DESCRIPTION OF THE INVENTION 
     In the following description, it should be noted that similar elements, in the various FIGURES, will be similarly numbered. 
     Referring now to FIG. 1 there is shown a substrate 10 of, for example, semi-insulating gallium arsenide having an undoped buffer layer 12, which may be formed from the vapor phase, that is then capped with a highly doped n+ layer of gallium arsenide 14. It should be noted that the buffer layer 12 may be formed using a chemical vapor deposition technique, as is well known in the art, and has a thickness of about 2-5 μm (microns) deep. The gallium arsenide layer 14 has an n+ dopant concentration of about 10 18  /cm 3  and a thickness of about 0.2-0.5 micron. The layer 14 has been doped with, for example, silicon to provide the required n+ concentration. Thereafter, the upper surface of the layer 14 is provided with a layer of photoresist material 16, which photoresist will define the area wherein a gallium arsenide mesa is to be formed. As shown in FIG. 2, the structure is then subjected to either an isotropic chemical etch or to an ion milling etch to form a mesa 18. Thereafter, as shown in FIG. 3, the device is provided with a layer of silicon dioxide (SiO 2 ) 20 which, for example, may be formed by a chemical vapor deposition technique, as is well known in the art. 
     As shown in FIG. 4, the mesa 18 is now provided with an apertured masking layer 22 which is utilized to subsequently define the channel region. Thereafter, as shown in FIG. 5, the structure is subjected to either a chemical or plasma etch wherein the exposed portion of the SiO 2  layer 20 is etched down to the layer 14 and the now exposed portion of the doped layer 14 is etched down to the buffer layer 12, effectively forming a source region 14.1 and a drain region 14.2. 
     As shown in FIG. 6, the mesa 18 is now subjected to a gallium arsenide regrowth step in order to produce a channel region 24. Sufficient n+ dopant (such as silicon) is introduced during the regrowth step in order to provide the channel region 24 with a doping density of the order to about 10 17  /cm 3 . This regrowth processing has been detailed in an article by C. O. Bozler et al. entitled &#34;SINGLE-CRYSTAL GaAs FILMS ON AMORPHOUS SUBSTRATES BY THE CLEFT PROCESS&#34;, J. Vac. Sci. Technol., 20 (3), March, 1982. In this article, the authors describe a process for regrowing gallium arsenide crystals from a surface orientation in the [110] crystallographic plane and, by utilizing the teachings of the article, the regrown crystals will grow laterally over the top of the SiO 2  layer 20 to form a &#34;T&#34; shaped channel region. The lateral regrowth of the gallium arsenide crystal, as compared to vertical regrowth of the crystals, controls the proximity of the channel region to the source and drain regions. This growth is dependent on the crystallographic orientation of the top surface of the mesa 18 where the aperture in which the crystal is regrown is defined as being oriented about 20° to the single [110] cleavage plane of the underlying crystal. 
     Having formed channel region 24 it should now become obvious that current will now normally flow through the n+/n/n+ regions 14.1, 24 and 14.2 and, that when the channel region 24 is appropriately biased, current will be entirely pinched-off. 
     Contact is now made to the source and drain regions 14.1 and 14.2 and this is done, as shown in FIG. 7, by applying an apertured layer of a photoresist mask 26 to the top surface of the SiO 2  layer 20 in order to define the source and drain contacts. The openings in the photoresist mask 26 are used to etch corresponding openings in the SiO 2  layer 20 to expose the source and drain regions 14.1 and 14.2 while maintaining the channel region 24 masked. Thereafter, as shown in FIG. 8, ohmic contacts are formed by depositing a standard AuGe/Ni/Au layered alloy 28. In this situation the entire wafer is covered with the deposited metal alloy 28 and the well-known lift off technique is utilized whereby when the photoresist mask 26 is removed all of the desired metal deposited thereon is also removed leaving only contacts 28.1 and 28.2 in ohmic contact with the source region 14.1 and the drain region 14.2 respectively. It should be understood that these contacts may also be extended to contact pads shown here symbolically as pads 30 and 32 respectively. 
     Having formed the source and drain contacts 28.1 and 28.2, the structure is again provided with an apertured layer of photoresist material 34 as shown in FIG. 9 wherein the aperture is aligned with the channel region 24. A Schottky contact metal is then deposited over the entire structure, using the same lift off technique as previously described, to produce a contact 36 in Schottky contact with the channel region 24, as shown in FIG. 10. To complete the device, as with the source and drain contacts, the Schottky contact metal may be run out to a pad member positioned at the edge of the chip and is shown here symbolically as pad 38. 
     Referring now to FIGS. 11 and 12 there is shown another embodiment which may be produced by my novel method, that also may be used to produce similar results. Insofar as this latter embodiment is concerned, the processing is identical with the first embodiment, through FIGS. 1-5. Thereafter, as shown in FIG. 11, the channel region 24 is formed without the lateral overgrowth described in the C. O. Bozler et al. article. The processing is continued through FIGS. 7 and 8 and the photoresist material 34 is deposited as in FIG. 9. Thereafter, when the Schottky contact is made using the well-known lift off technique the contact 36 shown in FIG. 12 will be produced. 
     Thus, I have described a method which may be employed to produce the required Schottky metal contact on the top surface of the channel region. Current can now be made to flow through the pad 30, the source contact 28.1, through the n+ source region 14.1, through the regrowth n channel region 24, and into the n+ drain region 14.2, the drain contact 28.2 and into the pad 32. The Schottky contact/channel 36/24, with the proper bias applied to the pad 38 will pinch-off in the area of the channel region overgrowth 24 and thus, prevent current flow in the device. 
     As will be seen by those skilled in the art, the source and drain resistance has been appreciably lowered by the close proximity of the contacts 28.1 and 28.2 to the channel contact 36. Further, by making the contacts as small as possible with my novel process the inductance in the resultant structure has also been reduced significantly, thereby allowing the device to operate at higher frequencies than heretofore possible. 
     Additionally, while I have described a process and the resultant structure in terms of a gallium arsenide device, it should now be obvious to those skilled in the art that various other III-V compounds may also be used without departing from the inventive concept.