Abstract:
Edge termination for a silicon carbide Schottky rectifier is provided by including a silicon carbide epitaxial region on a voltage blocking layer of the Schottky rectifier and adjacent a Schottky contact of the silicon carbide Schottky rectifier. The silicon carbide epitaxial layer may have a thickness and a doping level so as to provide a charge in the silicon carbide epitaxial region based on the surface doping of the blocking layer. The silicon carbide epitaxial region may form a non-ohmic contact with the Schottky contact. The silicon carbide epitaxial region may have a width of from about 1.5 to about 5 times the thickness of the blocking layer. Schottky rectifiers with such edge termination and methods of fabricating such edge termination and such rectifiers are also provided. Such methods may also advantageously improve the performance of the resulting devices and may simplify the fabrication process.

Description:
FIELD OF THE INVENTION 
     The present invention relates microelectronic devices and more particularly to edge termination for silicon carbide Schottky devices. 
     BACKGROUND OF THE INVENTION 
     High voltage silicon carbide (SiC) Schottky diodes, which can handle voltages between 600 V and 2.5 kV, are expected to compete with silicon PIN diodes fabricated of similar voltage ratings. Such diodes may handle as much as 100 amps of current, depending on their active area. High voltage Schottky diodes have a number of important applications, particularly in the field of power conditioning, distribution and control. 
     An important characteristic of a SiC Schottky diode in such applications is its switching speed. Silicon-based PIN devices typically exhibit relatively poor switching speeds. A silicon PIN diode may have a maximum switching speed of approximately 20 kHz, depending on its voltage rating. In contrast, silicon carbide-based devices are theoretically capable of much higher switching speeds, for example, in excess of 100 times better than silicon. In addition, silicon carbide devices may be capable of handling a higher current density than silicon devices. 
     However, reliable fabrication of silicon carbide-based Schottky devices may be difficult. Typical edge termination in SiC Schottky diodes require ion implantation of p-type dopants into the crystal. Such implants may cause substantial damage to the crystal lattice, which may require high temperature annealing to repair such defects. This high-temperature anneal step (&gt;1500° C.) may be undesirable for a number of reasons. For example, high temperature anneals tend to degrade the surface of SiC on which the Schottky contact is to be made, as silicon tends to dissociate from exposed surfaces of the crystal under such a high-temperature anneal. Loss of silicon in this manner may result in a reduced quality Schottky contact between metal and the semiconductor surface. High temperature anneals have other drawbacks as well. Namely, they are typically time-consuming and expensive. Moreover, implantation of p-type (Al) dopants may cause substantial lattice damage, while other species (B) have poor activation rates. 
     A conventional SiC Schottky diode structure has an n-type SiC substrate on which an n −  epitaxial layer, which functions as a drift region, is formed. The device typically includes a Schottky contact formed directly on the n −  layer. Surrounding the Schottky contact is a p-type JTE (junction termination extension) region which is typically formed by ion implantation. The implants may be aluminum, boron, or any other suitable p-type dopant. The purpose of the JTE region is to prevent the electric field crowding at the edges, and to prevent the depletion region from interacting with the surface of the device. Surface effects may cause the depletion region to spread unevenly, which may adversely affect the breakdown voltage of the device. Other termination techniques include guard rings and floating field rings which are more strongly influenced by surface effects. A channel stop region may also be formed by implantation of n-type dopants such as Nitrogen or Phosphorus in order to prevent the depletion region from extending to the edge of the device. 
     Additional conventional termination of SiC Schottky diodes are described in “Planar Terminations in 4H-SiC Schottky Diodes With Low Leakage And High Yields” by Singh et al., ISPSD &#39;97, pp. 157-160. A p-type epitaxy guard ring termination for a SiC Schottky Barrier Diode is described in “The Guard-Ring Termination for High-Voltage SiC Schottky Barrier Diodes” by Ueno et al., IEEE Electron Device Letters, Vol. 16, No. 7, July, 1995, pp. 331-332. Additionally, other termination techniques are described in published PCT Application No. WO 97/08754 entitled “SiC Semiconductor Device Comprising A PN Junction With A Voltage Absorbing Edge.” 
     SUMMARY OF THE INVENTION 
     Embodiments of the present invention may provide a silicon carbide Schottky rectifier having a silicon carbide voltage blocking layer having a predefined surface doping level and a Schottky contact on the silicon carbide voltage blocking layer. A silicon carbide epitaxial region is also provided on the silicon carbide voltage blocking layer and adjacent the Schottky contact. The silicon carbide epitaxial region has a thickness and a doping level designed to provide a selected charge per unit area in the silicon carbide epitaxial region. The charge per unit area in the silicon carbide epitaxial regions, also referred to as the junction termination extension (JTE) charge, is selected based on the surface doping of the blocking layer. In particular embodiments, the JTE charge is greater than 50% of an optimal JTE charge as determined by the surface doping of the blocking layer. Furthermore, it is preferred that the JTE charge is not greater than the optimal charge value. 
     In further embodiments of the present invention, a silicon carbide Schottky rectifier is provided having a silicon carbide voltage blocking layer and a Schottky contact on the silicon carbide voltage blocking layer. A silicon carbide epitaxial termination region is provided on the voltage blocking layer and adjacent the Schottky contact. The product of the thickness and doping concentration of the silicon carbide epitaxial region is greater than about 50% of            (       ɛ   r     ×     ɛ   0     ×     E   C       )     q     ;                          
     where: 
     ε r  is the relative dielectric constant of SiC; 
     ε 0  is dielectric constant of air; 
     E C  is the critical electric field of SiC; and 
     q is the electronic charge. 
     In further embodiments, the product of the thickness and doping concentration are not greater than about 100% of            (       ɛ   r     ×     ɛ   0     ×     E   C       )     q     .                          
     In still further embodiments, the thickness and doping concentration are not less than about 75% of            (       ɛ   r     ×     ɛ   0     ×     E   C       )     q     .                          
     In still further embodiments of the present invention, the silicon carbide epitaxial region extends from the Schottky contact from about 1.5 to about 5 times the thickness of the blocking layer. Additionally, a non-ohmic contact may be provided between the silicon carbide epitaxial termination region and the Schottky contact. 
     In embodiments of the present invention where the silicon carbide epitaxial region has a first conductivity type and the voltage blocking layer has a second conductivity type opposite the first conductivity type, the edge termination may also include a region of first conductivity type silicon carbide in the voltage blocking layer having a carrier concentration higher than that of the voltage blocking layer and adjacent a periphery of the silicon carbide epitaxial region opposite the Schottky contact. 
     In additional embodiments of the present invention, the Schottky rectifier may also include a first layer of silicon carbide of a first conductivity type the same as a conductivity type of the blocking layer and disposed between the blocking layer and a silicon carbide substrate. The first layer of silicon carbide may have a carrier concentration higher than the blocking layer. A second layer of silicon carbide of the first conductivity type may also be provided on the substrate opposite the first layer of silicon carbide so as to provide a layer of silicon carbide having a carrier concentration higher than a carrier concentration of the substrate. An ohmic contact may be provided on the second layer of silicon carbide. In such embodiments, the second layer may be an implanted layer of first conductivity type silicon carbide. Furthermore, the silicon carbide epitaxial region may be of a second conductivity type opposite that of the first conductivity type. In particular, the first conductivity type may be n-type and the second conductivity type may be p-type. 
     In other embodiments of the present invention, a Schottky rectifier is provided which includes an n-type silicon carbide substrate, an n-type silicon carbide blocking layer on the silicon carbide substrate, a Schottky contact on the silicon carbide blocking layer, an epitaxial region of p-type silicon carbide on the silicon carbide blocking layer and adjacent the Schottky contact so as to form a non-ohmic contact between the p-type epitaxial region and the Schottky contact, and an ohmic contact on the substrate opposite the blocking layer. 
     In further embodiments of the present invention, a plurality of p-type silicon carbide islands on the blocking layer may be provided. In such embodiments, the Schottky contact overlaps the plurality of p-type islands. 
     In yet other embodiments of the present invention, a Schottky rectifier is provided which includes an n-type silicon carbide substrate, an n-type silicon carbide blocking layer on the silicon carbide substrate, a Schottky contact on the silicon carbide blocking layer, an epitaxial region of p-type silicon carbide on the silicon carbide blocking layer and adjacent the Schottky contact so as to form a non-ohmic contact between the p-type epitaxial region and the Schottky contact and an ohmic contact on the substrate opposite the blocking layer. The p-type silicon carbide epitaxial region extends from the Schottky from contact about 2 to about 3 times the thickness of the blocking layer. Such embodiments may also include a plurality of p-type silicon carbide islands on the blocking layer. If so, then the Schottky contact overlaps the plurality of p-type islands. 
     In method embodiments of the present invention, a method of fabricating a termination region of a silicon carbide Schottky rectifier includes forming an epitaxial layer of p-type silicon carbide having a thickness and a doping level selected so as to provide a charge in a region of p-type silicon carbide adjacent to a Schottky contact of the Schottky rectifier proportional to the surface doping of a silicon carbide blocking layer of the Schottky rectifier and patterning the epitaxial layer of p-type silicon carbide so as to provide the region of p-type silicon carbide adjacent to the Schottky contact of the Schottky rectifier. 
     In such method embodiments, the patterning the epitaxial layer of p-type silicon carbide may be provided by forming an oxide layer on the p-type epitaxial layer of silicon carbide, patterning the oxide layer so as to expose a portion of the p-type epitaxial layer corresponding to the Schottky contact, thermally oxidizing the exposed portion of the p-type epitaxial layer at a temperature and for a time sufficient to consume all of the expose portion of the p-type epitaxial layer, and etching the thermally oxidized portion of the p-type epitaxial layer so as to expose a portion of the blocking layer on which the Schottky contact is formed. Furthermore, thermally oxidizing the p-type epitaxial layer may be carried out in a dry ambient environment. Additionally, thermally oxidizing the p-type epitaxial layer may be accomplished by oxidizing the p-type epitaxial layer at a temperature of less than about 1300° C. 
     In further embodiments, etching the thermally oxidized portion of the p-type epitaxial layer may be preceded depositing an ohmic metal on a surface of a silicon carbide substrate opposite the blocking layer and annealing the ohmic metal so as to form an ohmic contact to the silicon carbide substrate. Such a deposition of an ohmic metal may also be preceded by implanting n-type dopants in the substrate so as to form a region of n-type silicon carbide having a carrier concentration higher than a carrier concentration of the substrate. In such embodiments, the ohmic metal may be deposited on the implanted region of the substrate. Furthermore, the implantation of n-type dopants may be carried out prior to thermally oxidizing the exposed portion of the p-type epitaxial layer such that thermally oxidizing the exposed portion of the p-type epitaxial layer also activates the n-type dopants. 
     In yet other embodiments of the present invention, etching the thermally oxidized portion of the p-type epitaxial layer is followed by depositing a Schottky metal on the exposed portion of the blocking layer. 
     In still other embodiments of the present invention, the good quality passivating oxide layer is patterned so as to expose a portion of the p-type epitaxial layer corresponding to the Schottky contact including a plurality of regions of exposed portions of the p-type epitaxial layer. The exposed portion of the p-type epitaxial layer including the plurality of regions is thermally oxidized at a temperature and for a time sufficient to consume all of the exposed portion of the p-type epitaxial layer. The thermally oxidized portion of the p-type epitaxial layer is etched so as to expose a portion of the blocking layer on which the Schottky contact is formed thereby providing a plurality of exposed portions of the blocking layer spaced apart by islands of p-type silicon carbide. 
     In additional embodiments of the present invention, patterning the oxide layer so as to expose a portion of the p-type epitaxial layer corresponding to the Schottky contact is preceded by patterning the oxide layer and the p-type epitaxial layer to expose a portion of the blocking layer at the periphery of the Schottky rectifier, and implanting n-type dopants in the exposed portion of the n-type blocking layer so as to provide a region of implanted n-type dopants adjacent the periphery of the p-type epitaxial layer. 
     In particular embodiments, the thickness and doping level of the silicon carbide epitaxial region are selected so as to provide a charge in the region of p-type silicon carbide adjacent to a Schottky contact of the Schottky rectifier which is from about 50% to about 100% of            Q     JTE   ,   opt       =       (       ɛ   r     ×     ɛ   0     ×     E   C       )     q       ;                          
     where: 
     Q jTE,opt  is the optimum JTE charge; 
     ε r  is the relative dielectric constant of SiC; 
     ε 0  is dielectric const. of air; 
     E C  is the critical electric field of SiC; and 
     q is the electronic charge. 
     Furthermore, the thickness and doping level may be about 75% of          Q     JTE   ,   opt       =         (       ɛ   r     ×     ɛ   0     ×     E   C       )     q     .                            
     In further method embodiments of the present invention, a method of fabricating a silicon carbide Schottky rectifier is provided by forming a first n-type silicon carbide epitaxial layer on an n-type silicon carbide substrate, wherein the first n-type silicon carbide epitaxial layer has a carrier concentration less than a carrier concentration of the silicon carbide substrate. A p-type silicon carbide epitaxial layer is formed on the first n-type epitaxial layer. A passivating oxide is deposited on the p-type silicon carbide epitaxial layer and the passivating oxide patterned to expose a portion of the p-type silicon carbide corresponding to a Schottky contact of the Schottky rectifier. The exposed portion of the p-type silicon carbide is thermally oxidized to oxidize the p-type silicon carbide to the first n-type epitaxial layer. An ohmic contact metal is then deposited on the substrate opposite the first n-type epitaxial layer and annealed so as to provide an ohmic contact to the substrate. Then the oxidized p-type silicon carbide is removed to expose a portion of the first n-type epitaxial layer corresponding to the Schottky contact and a Schottky metal deposited on the exposed portion of the first n-type epitaxial layer so as to provide a Schottky contact to the first n-type epitaxial layer. 
     In further embodiments of the present invention, the p-type silicon carbide epitaxial layer has a thickness and a doping level selected so as to provide a charge in a region of p-type silicon carbide adjacent to the Schottky contact of the Schottky rectifier proportional to the surface doping of the first n-type epitaxial layer. 
     In other embodiments, the method further includes forming a second layer of n-type silicon carbide, wherein the second layer of n-type silicon carbide is disposed between the silicon carbide substrate and the first n-type epitaxial layer and has a carrier concentration higher than the carrier concentration of the silicon carbide substrate. 
     In still other embodiments, the method may also include patterning the p-type epitaxial layer to expose a portion of the first n-type epitaxial layer adjacent the periphery of the Schottky rectifier, implanting n-type dopants in the exposed portion of the first n-type epitaxial layer and thermally annealing the implanted dopants so as to activate the dopants. In such embodiments, the deposition of a passivating oxide may also include depositing a passivating oxide on the p-type epitaxial layer and the implanted region of the first n-type epitaxial layer. In particular embodiments, the thermal anneal of the implanted dopants is carried out at a temperature of less than about 1300° C. 
     Furthermore, additional method embodiments may also include implanting n-type dopants in the silicon carbide substrate opposite the first n-type epitaxial layer so as to provide a region of n-type silicon carbide having a carrier concentration higher than the carrier concentration of the silicon carbide substrate. In such embodiments, implanting n-type dopants may be followed by depositing an oxide on the implanted region of the silicon carbide substrate and the thermal oxidation step may be followed by removing the oxide from the implanted region of the silicon carbide substrate. 
     The advantages and features of the invention, and the manner in which the same are accomplished, will become more readily apparent upon consideration of the following detailed description of the invention taken in conjunction with the accompanying drawings, which illustrate preferred and exemplary embodiments, and wherein: 
    
    
     DESCRIPTION OF THE DRAWINGS 
     FIG. 1 is a cross-sectional view of one embodiment of a Schottky rectifier having edge termination according to embodiments of the present invention; 
     FIGS. 2A through 2I illustrate processing steps for fabricating silicon carbide Schottky rectifiers having edge termination according to embodiments of the present invention; 
     FIG. 3A is a graph illustrating a relationship between the charge in the epitaxial edge termination and the surface doping of a voltage blocking layer on which the epitaxial edge termination is formed; 
     FIG. 3B is a graph illustrating an exemplary relationship of the “ideal” blocking voltage V B  to surface doping N D  in the voltage blocking layer for a range of given thickness w D  of the voltage blocking layer; 
     FIG. 3C is a graph illustrating the blocking voltage to JTE charge (Q JTE ); and 
     FIG. 4 is a cross-sectional view of a Schottky rectifier according to alternative embodiments of the present invention. 
    
    
     DETAILED DESCRIPTION 
     The present invention will now be described with reference to the Figures which illustrate various embodiment of the present invention. As illustrated in the Figures, the sizes of layers or regions are exaggerated for illustrative purposes and, thus, are provided to illustrate the general structures or the present invention. Furthermore, various aspects of the present invention are described with reference to a layer being formed on a substrate or other layer. As will be appreciated by those of skill in the art, references to a layer being formed on another layer or substrate contemplates that additional layers may intervene. References to a layer being formed on another layer or substrate without an intervening layer are described herein as being formed “directly” on the layer or substrate. Like numbers refer to like elements throughout. 
     As is described in more detail below, embodiments of the present invention may provide improved Schottky rectifiers by providing p-type edge termination without the need for a p-type implant. The avoidance of a p-type implant may also avoid the need for a high temperature anneal which may adversely effect the characteristics of the device. As certain embodiments of the present invention utilize only n-type implants of, for example, Phosphorous which may be annealed at less than 1300° C., for example, 1200° C., or Nitrogen which may be annealed at about 1500° C., the higher temperatures needed to activate p-type implants may be avoided. 
     Furthermore, as is described in further detail below, because the p-type termination region is formed in an epitaxial process, its doping and thickness may be closely controlled. Thus, the use of an epitaxial p-type edge termination may allow for selecting a charge in the edge termination based on the surface charge of the voltage blocking layer which may provide improved edge termination performance over, for example, relatively uncontrolled epitaxial edge termination or implanted edge termination techniques. 
     In embodiments of the present invention it may also be possible to form the Schottky contact on a region of SiC which has not been exposed to ambient when a high temperature (e.g.&gt;1500° C.) anneal is performed and, thus, loss of Si during the anneal may be reduced or avoided. Accordingly, a higher quality Schottky contact may be provided. 
     FIG. 1 illustrates a first embodiment of a Schottky rectifier having epitaxial edge termination according to the present invention. A first (optional) epitaxial layer  12  of n-type conductivity is grown on a single crystal bulk silicon carbide substrate  10  of n-type conductivity and may act as a buffer layer. The first epitaxial layer of silicon carbide  12  is disposed between the substrate  10  and an n-type epitaxial layer  14  which may provide a voltage blocking layer. The silicon carbide substrate  10  may be an n +  SiC substrate, the first epitaxial layer  12  may be a highly doped n-type SiC epitaxial layer and the n-type epitaxial layer  14  may be a lightly doped n-type SiC epitaxial layer. Thus, the first epitaxial layer  12  may have a carrier concentration comparable to the silicon carbide substrate  10  and the n-type epitaxial layer  14  may have a lower carrier concentration than the silicon carbide substrate  10 . A Schottky contact  18  is also provided on the n-type epitaxial layer  14 . 
     A p-type silicon carbide epitaxial termination region  16  is also provided. The p-type epitaxial termination region  16  is provided on the n-type epitaxial layer  14  and is adjacent the Schottky contact  18 . A passivating oxide  20  may also be provided. The passivating oxide  20  may cover exposed areas of the Schottky rectifier other than the Schottky contact  18 . Furthermore, an ohmic contact  22  may also be provided on the substrate  10  opposite the Schottky contact  18 . The ohmic contact  22  may be provided on an optional n +  region of silicon carbide  26  which may be provided by implantation in the substrate  10  and/or as an epitaxial layer formed on the substrate  10 . Preferably, the p-type epitaxial termination region  16  extends from the Schottky contact  18  a distance from about 2 to about 3 times the thickness of the n-type epitaxial layer  14 . The silicon carbide substrate and epitaxial layers may be 4H SiC. 
     FIG. 1 also illustrates an optional n +  region of silicon carbide  24  in the n-type voltage blocking layer  14  at the periphery of the p-type epitaxial termination region  16 . The n +  region of silicon carbide  24  may provide a “channel stop” region for the Schottky rectifier. An optional metal overlayer  28  on the Schottky metal  18  is also illustrated in FIG.  1 . 
     In particular embodiments of the present invention, the p-type epitaxial termination region  16  has a controlled doping and thickness so as to provide a predefined charge in the p-type epitaxial termination region  16  based on the surface doping of the n-type voltage blocking layer  14 . Preferably, the charge in the p-type epitaxial termination region  16  is selected based on a theoretical optimum junction termination extension (JTE) charge given the surface doping concentration of the epitaxial layer used to make this structure: 
     
       
           Q   JTE,act   =αQ   JTE,opt , 
       
     
     where            Q     JTE   ,   opt       =       (       ɛ   r     ×     ɛ   0     ×     E   C       )     q       ;                          
     where: 
     α is a proportionality value between 0.5 and 1.0; 
     Q JTE,opt  is the theoretical optimum JTE charge; 
     ε r  is the relative dielectric constant of SiC (which is about 9.7); 
     ε 0  is dielectric constant of air which is 8.854×10 −14  C-cm/V; 
     E C  is the critical electric field of SiC, which is dependent on the doping by the formula given below; 
     q is the electronic charge which is 1.602×10 −19  C; and 
     Q JTE,act  is the actual selected JTE charge. 
     The critical electric field of SiC is given by the following equation:            E   C     =         2.49   ×     10   6         (     1   -     0.25   ×   ln                   (     N   /     10   16       )                           V        /        cm       ;                          
     where N is the doping of the n-type blocking layer. See “Ionization rates and critical fields in 4H-SiC,” by A. O Konstantinov, Q. Wahab, N. Nordell and U. Lindefelt, Applied Physics Letters, vol. 72, No. 1, July 1997. 
     An illustration of the relationship of JTE charge to surface doping is seen in FIG.  3 A. The line identified as “theoretical” corresponds to an α of 1.0 and the “75% theoretical” line corresponds to an α of 0.75. FIG. 3B shows an exemplary illustration of the relationship of the “ideal” blocking voltage V B  to surface doping N D  in the voltage blocking layer  14  for a range of given thickness w D  of the voltage blocking layer  14 . In this context “ideal” refers to the best blocking voltage obtainable for a given layer thickness and doping without regard to surface or other effects. FIG. 3B shows that, as the surface doping N D  in the voltage blocking layer  14  increases, the ideal blocking voltage generally decreases. In general, the ideal blocking voltage V B  may be calculated using the following equation:          V   B     =       β                   (       w   D     ×   Ec     )       2                            
     where 0.75≦β≦1 and Ec is given by the equation set forth above. A doping level in the range of 1×10 15  to 2×10 16  may yield a blocking voltage from approximately 2.5 kV at w D =30 μm to 400 V at w D =4 μm, provided the doping is selected to be as high as possible while keeping the device in the punch-through regime. 
     As those of skill in the art will recognize, a diode epitaxial design is said to be in the punch-through regime when the breakdown voltage is primarily a function of the epitaxial thickness of the voltage blocking layer. In contrast, in the non-punch-through regime, the breakdown voltage is primarily a function of doping. For a given epitaxial thickness, whether a diode design is in the punch-through regime or non-punch-through regime depends on the doping of the voltage blocking layer. In general, an empirical relation describing the boundary between the punch-through regime and the non-punch-through regime may be: 
     
       
           BV =5.73×10 14   N   D   −0.73 . 
       
     
     An exemplary illustration of the blocking voltage to JTE charge (Q JTE ) is shown in FIG.  3 C. As seen in FIG. 3C, as charge in the JTE increases for a given surface doping of the blocking layer, the breakdown voltage of the device generally increases. However, if surface doping of the blocking layer remains constant and charge increases beyond a threshold value (identified in FIG. 3C as Q JTE,opt ), the blocking voltage of the device decreases. Furthermore, the absolute value of the slope of the curve of blocking voltage versus JTE charge is substantially greater above the threshold value than below. This maximum point in the blocking voltage versus JTE charge curve is the “theoretical optimum” charge as it is the charge which theoretically provides the maximum breakdown voltage of a device for a give voltage blocking layer surface doping. Because the slope is steeper above the theoretical optimum value, it may be preferable to avoid exceeding the theoretical optimum value. Thus, it is preferable the α value not be substantially greater than 1.0. Furthermore, if α is too small, then the JTE may have only limited effect on the performance of the device. Thus, it is preferred that α be greater than about 0.5. Additionally, because exceeding the optimum charge value may substantially decrease the blocking voltage of the device, it is preferred that variations in the manufacturing process(es) be taken into account in establishing the charge for the JTE. Thus, it may be preferable to utilize an α value of about 0.75 or from about 0.75 to about 1.0. However, as will be appreciated by those of skill in the art in light of the present disclosure, the selection of an α value may depend on the degree of variation in the final products, the acceptable failure rate or other manufacturing concerns. 
     FIGS. 2A through 2I illustrate processing steps which may be utilized in producing Schottky rectifiers having edge termination according to various embodiments of the present invention. As seen in FIG. 2A, a layer of n +  silicon carbide  12  may optionally be formed on a single crystal silicon carbide substrate  10  by epitaxial growth, ion implantation or other such techniques known to those of skill in the art. An n −  pitaxial layer of silicon carbide  14  is formed on the n +  silicon carbide layer  12  if present, or the substrate  10 . The n −  epitaxial layer  14  may also be formed utilizing techniques known to those of skill in the art. 
     As illustrated in FIG. 2B, a p-type epitaxial layer is formed on the n −  epitaxial layer  14  with a doping and depth which are controlled so as to provide the predetermined charge proportional to the surface charge of the n −  epitaxial layer  14  as described above. Such a doping and depth may also take into account any loss in the p-type epitaxial layer during subsequent processing so that the final p-type termination region has the proper final total charge. 
     FIG. 2C and 2D illustrate optional processing steps for providing channel stop implants. As seen in FIG. 2C, a masking oxide  42  is formed on the p-type epitaxial layer  40 . Such a masking oxide may be formed, for example, utilizing Plasma Enhanced Chemical Vapor Deposition (PECVD) of SiO 2 . The p-type epitaxial layer  40  and the masking oxide  42  are then patterned so as to provide an oxide mask  42 ′ and a patterned p-type layer  40 ′ for implantation of the channel stop  24 . Furthermore, the opposite surface of the substrate  10  may also be implanted with n-type dopants so as to provide an optional n +  layer  26 ′ suitable n-type dopants may include Nitrogen and Phosphorous. The structure of FIG. 2D may then be annealed to activate the n-type implants. Optionally, such an anneal may be delayed and performed simultaneously with the thermal oxidation of the p-type layer  40 ′ as described below. Techniques for implantation and activation of n-type dopants in SiC are known to those of skill in the art. In the event that one or more of the n-type implants are not incorporated in the device, then the implant and/or annealing step(s) may be omitted. However, it is preferred that the patterning of the p-type layer  40  still be carried out so as to define the outer periphery of the p-type epitaxial termination region  16 . 
     As is seen in FIG. 2E, after removal of the oxide mask  42 ′, a passivating oxide layer  44  is formed on the exposed surface of at least the patterned p-type epitaxial layer  40 ′, the n-type implanted region  24  (if present) and/or the n-type voltage blocking layer  14 . If an n-type implant is also provided in the opposite face of the substrate, then an oxide layer  50  may also be deposited on the opposite side of the substrate  10  over the implanted region  26 ′. Such oxide layers may help to prevent loss of ion implanted regions during subsequent thermal oxidation steps. Preferably, the oxide layers  44  and  50  are deposited oxide layers and more preferably are Low Pressure Chemical Vapor Deposition (LPCVD) layers of SiO 2 , however, high quality Plasma Enhanced Chemical Vapor Deposition 9PECVD) may also be used. 
     As illustrated in FIG. 2F, the oxide passivating layer  44  may be patterned to expose the p-type layer  40 ′. Such a patterning may be accomplished by photolithography and reactive ion etching, selective growth or other such techniques known to those of skill in the art. The oxide passivating layer  44  is preferably patterned so as to provide a window for formation of the Schottky contact so as to provide a passivating layer  20  on exposed portions of the final device other than the Schottky contact  18 . The structure of FIG. 2F is thermally oxidized for a time sufficient to completely oxidize the exposed portion of the p-type layer  40 ′ so as to provide a region of oxidized p-type SiC  46  corresponding to the Schottky contact location and the termination region  16  as is seen in FIG.  2 G. Such a thermal oxidation is preferably carried out in a dry ambient of preferably less than about 1500° C. and more preferably about 1300° C. or less for a time sufficient to completely oxidize the p-type epitaxial layer  40 ′. The duration of such a thermal oxidation may vary depending on the temperature utilized and the thickness of the p-type epitaxial layer  40 ′. As described above, such thermal oxidation step may also be utilized to activate the n-type implants. 
     After the thermal oxidation is complete, the oxide layer  50  is removed from the opposite side of the substrate by, for example, reactive ion etching, and a metal layer deposited to provide an ohmic contact  22 . Suitable materials for such an ohmic contact include Nickel or other such materials known to those of skill in the art. The metal layer is also annealed to form the ohmic contact  22 . The anneal may be accomplished by a rapid thermal anneal process. Such operations are illustrated by FIG.  2 H. After forming the ohmic contact  22 , a photoresist pattern is deposited to provide a window for making the Schottky contact  18  and the thermal oxide etched through to the n-type epitaxial layer  14  so as to provide the window for forming the Schottky contact  18 . Such an etch of the oxide  46  may be accomplished by a buffered oxide etch. As seen in FIG. 2I, the Schottky metal is deposited in the window formed by the etching of the oxide region  46  and may slightly overlap the p-type termination region  16 . The Schottky metal may be any suitable Schottky metal, such as Nickel, Chromium, Titanium or Platinum. Also, an optional metal overlayer  28  of, for example, gold, may be formed on the Schottky contact  18 . 
     As illustrated in FIG. 2I, the Schottky contact  18  and the p-type edge termination region  16  form a non-ohmic contact. Such a non-ohmic contact may be characterized by a non-linear voltage/current relationship of the contact. In particular, the contact has a finite turn-on voltage and a reverse leakage current which is at least 10 3  times smaller than the rated on-state current. A reverse blocking voltage is also exhibited which is primarily determined by the epitaxial layer ( 14 ) properties. In addition, this junction follows closely the thermionic current transport physics at room temperature. 
     FIG. 4 illustrates a further embodiment of the present invention where a Junction Barrier Schottky (JBS)/Merged P-I-N Schottky (MPS) grid  17  is provided in the Schottky gate region. A Schottky contact  18 ′ and metal overlayer  28 ′ may be provided over the JBS/MPS grid  17 . Such a grid may be provided by modifying the patterning of the passivating layer  44  so as to provide a mask for oxidation of the p-type epitaxial layer  40 ′ which provides the “bumps” or “islands” of the JBS/MPS gate structure illustrated in FIG.  4 . The oxide on the grid  17  may be removed by mask and reactive ion etching. Additionally, the grid  17  may be masked when the thermally oxidized regions are etched away to provide the Schottky contact window. 
     In the drawings and specification, there have been disclosed typical preferred embodiments of the invention and, although specific terms are employed, they are used in a generic and descriptive sense only and not for purposes of limitation, the scope of the invention being set forth in the following claims.