Transistor with voltage clamp

Abstract: A power transistor takes advantage of the lower breakdown voltage capability of a spherical junction. A clamping region (40) having a spherical shape is provided in the gate region of an enclosed transistor cell (42). The clamping region (40) has a lower breakdown voltage than do the active portions of the transistor cell (42). Both a DMOSFET and an IGBT transistor may be provided with the clamping region (40) (a MOS-controlled thyristor is also disclosed). The clamping region (40) is a zener diode in the case of the DMOSFET, and is a bipolar junction transistor in the case of the insulated gate bipolar transistor. The clamping region (40) is preferably an island in the center of each cell of a closed cell structure.

Description: This invention relates to a transistor and method for making a transistor with a voltage clamp. The invention can be applied to a power switching transistor, such as a DMOS or insulated gate bipolar transistor. A DMOS transistor is disclosed in JP-A-59149058. Reference is now made to Figures 1A, 1B and 1C of the accompanying drawings, in which: Figures 1A and 1B show views of portions of a prior art power transistor, and Figure 1C shows breakdown voltage of a spherical and cylindrical junction. DMOSFET's (double diffused metal oxide silicon field effect transistors) and IGBT's (insulated gate bipolar transistors) are well-known in the art. A typical example of one cell of a DMOSFET transistor is shown in Figure 1A. The DMOSFET is a field effect transistor as shown having source regions 10a and 10b formed respectively in body regions 12a, 12b which are in turn formed in an epitaxial layer 14 (i.e., a drain region) grown on a substrate 16. A gate 18 is formed over an insulating layer 20 on the principal surface 22 of the epitaxial layer 14. A drain contact 24 is attached to the backside of the substrate 16. A gate contact 28 and source/body contact 30 are also provided. Figure 1A thus shows a conventional power DMOSFET. An insulated gate bipolar transistor (IGBT) has a somewhat similar structure as the DMOSFET of Figure 1A, except that for the IGBT substrate region 16 would be a P+ region (i.e., of opposite conductivity type to that of the epitaxial layer 14). The IGBT in effect is internally a field effect transistor (FET) with its source connected to the collector of a wide base bipolar transistor and its drain connected to the base of the wide base bipolar transistor. The emitter terminal of the wide base transistor then is referred to as the collector terminal of the IGBT; the collector terminal of the wide base transistor is referred to as the IGBT emitter terminal, and the FET gate terminal is the IGBT gate terminal. Thus for the IGBT corresponding to the structure of Figure 1A, the epitaxial layer 14 is the base region. The body regions 12a, 12b are shorted to the IGBT emitter regions 10a, 10b. The substrate 16 (which is of P+ type) is the IGBT collector region. Therefore, the chief structural difference between an insulated gate bipolar transistor and a DMOSFET is in the conductivity type of the substrate. In an insulated gate bipolar transistor the epitaxial region is an open base region, meaning there is no electrical contact of that region to any external structures. This structure is also referred to as a floating base region. Prior art power transistors typically include many (e.g., ten thousand) cells of the kind shown in Figure 1A, each cell being identical. As shown in Fig. 1B in a top view, for a DMOSFET 32 each cell 34, 36, 38, 40 is a polygon such as a square which includes a central P+ source region 34a, 36a, 38a, 40a formed in and surrounded by an N+ body region 34b, 36b, 38b, 40b. Each cell 34, 36, 38, 40 is in turn surrounded by a polycrystalline silicon (i.e., polysilicon) conductive gate region 44 which is the conductive gate region for the entire transistor. In another well known prior art cell structure (not shown), open linear cells are provided. Each cell typically includes a linear P+ source region formed in between linear N+ body regions. Between adjacent cells a polysilicon gate region is provided. It is known that in devices such as shown in Figure 1A, a diffused region such as collector region 12a (which is typically delineated by means of a window in a photo-etched oxide mask) is parallel plane in shape, with the exception of part of the region defined by the edge of the window in the oxide. At the edge of the window in the oxide, owing to diffusion effects, the region takes on a cylindrical shape in cross section. Thus the space charge lines at the window edge are distorted, resulting in an electric field that is different from the parallel plane electric field structure. Thus for a particular applied voltage, the peak electric field is higher for the cylindrical junction than for the parallel plane junction. Thus the breakdown voltage is lower for the cylindrical junction than for the parallel plane, and so breakdown tends to occur at the cylindrical junction. It is also known in the art that at the curved region where two cylindrical junctions meet, such as at the corner of a rectangular shaped diffused region, a so-called spherical junction is formed. The electrical breakdown of a spherical junction typically occurs at an even lower breakdown voltage than is experienced with a cylindrical junction. This is because extremely small curvature radii are encountered at such sharp corner regions associated with a diffusion area which is masked through a rectangular window. Figure 1C shows that the breakdown voltage of a spherical junction is lower than the breakdown voltage of a cylindrical junction. The breakdown voltage of the spherical junction is typically about 60% of that of a cylindrical junction, where the radius of the junction divided by the thickness of the lightly-doped semiconductor is approximately 0.1. In Figure 1C, r j is the radius of the junction, and W′ is the thickness of the lightly-doped semiconductor. BV/BV pp is the breakdown voltage relative to that of a parallel plane. The prior art power DMOS and insulated gate bipolar transistor devices typically have spherical or at best cylindrical shaped PN junctions. As indicated above, the spherical junctions typically break down at lower voltage values than do the cylindrical junctions. As also indicated above, a cylindrical junction breaks down at a lower voltage value than does a planar junction. Thus the prior art power transistor devices as described above typically experience electrical breakdown at the corners of their diffused regions. This electrical breakdown is undesirable, because it can lead to heating at the breakdown region due to excessive current flowing through that spot. This is especially a problem because power transistors are intended to be subjected to high currents, and so this heating can catastrophically destroy the transistor. It is therefore desirable to have a transistor device for use in power switching which does not break down at the active part of the transistor. In U.S. Patent No. 4,779,123, issued October 18, 1988, incorporated herein by reference, Bencuya et al. disclose an improved insulated gate bipolar transistor having a high conductivity collector well surrounding the active portion of the transistor. This collector well prevents undesirable transistor latching. Latching is a phenomenon whereby a semiconductor structure "latches" into a self-perpetuating state of bipolar conduction, which cannot be turned off by removing the voltage bias on the gate to stop FET mode conduction. However, Bencuya et al. do not disclose any method of dealing with the breakdown problem. In US-A-4 819 044, a MOSFET with an integrated Zener diode is described. The Zener diode forms a clamping region having a lower breakdown voltage, than the MOSFET. The Zener diode, however, requires an additional diffusion step which complicates the manufacturing process. In accordance with the invention, a transistor comprises a plurality of cells wherein each cell comprises a semiconductor body of a first conductivity type, a substantially annular first region of a second conductivity type formed in the semiconductor body, a second region of the first conductivity type formed in the annular region, and a conductive gate region overlying a surface of the semiconductor body and having its extent defined by the interior portion of the second region, characterised by a clamping region of the second conductivity type formed in the interior portion of the first and second regions, the clamping region having a breakdown voltage lower than the breakdown voltage of the other portions of the cell, a cross-sectional shape different from that of the annular first region, and a depth of a doping level the same as that of the annular first region. Also in accordance with the invention, a method of making a cell for a transistor comprising a plurality of cells comprises the steps of forming in a semiconductor body of a first conductivity type a substantially annular first region of a second conductivity type, forming a second region of the first conductivity type in the annular region, and forming a conductive gate region overlying a surface of the semiconductor body and having its extent defined by the interior portion of the second region, characterised by forming a clamping region of the second conductivity type in the interior portion of the first and second regions, the clamping region having a breakdown voltage lower than the breakdown voltage of the other portions of the cell, a cross-sectional shape differing from that of the annular first region, and a depth and a doping level the same as that of the annular first region. The clamping region has a voltage breakdown lower than the voltage breakdown of the remainder of the transistor, thus protecting the transistor from destructive voltage breakdown and hence increasing the transistor's safe operating area (SOA). In accordance with the preferred embodiments of the invention, the transistor is either an insulated gate bipolar transistor (IGBT) or a double diffused metal oxide semiconductor field effect transistor (DMOSFET). Preferably the clamping region has a spherical cross sectional shape so as to achieve a relatively low breakdown voltage. In accordance with one embodiment of the invention, the clamping region is formed in the center of a substantially annular (ring-shaped) active region of the transistor cell. In one alternative embodiment, multiple clamping regions are provided in each cell, with the multiple clamping regions arranged symmetrically. The gate region of the cell surrounds the clamping region. The active regions of the cell (i.e., the source and body for the DMOSFET or emitter and body for the IGBT) define a closed cell structure surrounding the gate region. These various embodiments of the invention take advantage of the existence of a lower breakdown voltage capability of spherical and cylindrical junctions compared to planar junctions. In accordance with one embodiment of the invention, the annular shaped active device cell encloses an island semiconductor region which acts as a voltage clamp. Since the active device cell is annular in shape, it has a higher breakdown voltage than would a cylindrical junction. On the other hand, the clamping region has a spherical cross-sectional shape, so breakdown will always occur around the clamping region junction rather than around the active device region junction. The clamping region in the case of the DMOSFET preferably forms a high voltage zener diode. As is known in the art, discrete zener diodes are conventionally used because they always break down at a particular voltage and can break down repeatedly without being damaged. Therefore, provision of a zener diode in the substrate in accordance with the invention ensures that the breakdown phenomena occurs in the bulk of the epitaxial layer and protects the active device. In the case of N-channel IGBT, the clamping region preferably forms a portion of a PNP-bipolar junction transistor. Both of these embodiments of the invention improve the safe operating area (SOA) of the power transistor, because a zener diode has a superior safe operating area than does a DMOSFET, and similarly a PNP-BJT has a superior safe operating area than does an insulated gate bipolar transistor. Thus for a given voltage, a transistor in accordance with the invention can carry a higher current than does a prior art transistor. The above described embodiments of the invention also beneficially prevent latching for the same reasons as does the transistor disclosed by Bencuya et al. in U.S. Patent No. 4,779,123 as described above. The invention is further described below, by way of example, with reference to the remaining Figures of the accompanying drawings, in which: Figure 2 shows a top view of one embodiment of a transistor cell of the present invention, Figures 3A and 3B show two embodiments of the present invention, Figure 4 shows a top view of another embodiment of the present invention, Figure 5 shows the safe operating area curve for one embodiment of the present invention, and Figures 6a - 6f show process steps to fabricate one embodiment of the invention. Identical reference numbers in different figures denote similar or identical structures. Figure 2 shows a top view of one embodiment of the present invention. Figure 2 shows only a small portion of the transistor; it is understood that the pattern shown in Figure 2 is replicated many times for the entire transistor. P+ region 40 is the clamping region which is at the center of a preferably substantially radially symmetric i.e., square) active cell 42 of the device. The active cell 42 includes the N+ source (for a DMOSFET) or emitter for an IGBT) region 44a, 44b which in this embodiment is square in shape. The polysilicon gate region 46 for cell 42 is shown. Shown adjacent to the cell 42 are portions of the adjacent cells 50, 52, 54, 56, 58. The polysilicon gate region 46 of cell 42 is connected by polysilicon "bridges" 46a, 46b, 46c (which overlie the body regions 48a, 48b) to respectively the polysilicon gates 52b, 54b, 58b of adjacent cells 52, 54, and 58. Thus the gate region in each cell is ultimately connected by the polysilicon bridges to the gate region in each of the other cells in the transistor. The polysilicon bridges advantageously eliminate the need for a topside contact to each cell's gate region, thus simplifying fabrication and reducing the surface area of each cell. Underneath the polysilicon bridges 46a, 46b, 46c the P+ regions 48a, 48b are continuous and thus cell 42 is fully enclosed. The top side electrical contacts to the various regions are not shown in this view for simplicity. The clamping region 40 of cell 42 is electrically connected by conventional metallization (not shown) to the source or emitter region 44a, 44b and to body regions 48a, 48b. The cell structure geometry as shown on Figure 2 is used for both DMOS and IGBT transistors in accordance with the invention. These two types of transistors would therefore have the same appearance in a top view as shown in Figure 2. Figure 3A shows a cross section of an insulated gate bipolar transistor in accordance with the invention. The view of Figure 3A is taken through the line X - X in Figure 2. Shown in Figure 3A is the P+ type substrate 60. Overlying the substrate region 60 is N type region 62. Overlying the N type region 62 is an N- type epitaxial layer 64 which is the base region. The active device is formed in the N- type region 64. The active device as shown includes the conventional P+ type deep body regions 48a, 48b flanked by P type body regions 68a, 68b, 68c, 68d. It is understood that regions 48a, 48b are actually one region joined outside the plane of the drawing to form an annular structure. N+ type emitter region 44a is formed in P type body region 68a. N+ type emitter region 44b is formed in P type body region 68b. In the center of the active part of the device is the P+ clamping region 40. Overlying the N- type base region 64 is an insulating oxide layer 74. Conductive gate layer 46 overlies insulating oxide layer 74. As shown, the oxide layer 74 and gate layer 46 are opened to provide contacts to the N+ type emitter 44a, 44b and P+ type deep body regions 48a, 48b and to the P+ type clamping region 40. Also shown are N+ emitter regions 78, 80 which are respectively part of adjoining cells 52, 54. Figure 3B shows a similar device as shown in Figure 3 except that Figure 3B shows a DMOS device. The structural difference between the DMOS device of Figure 3B and the IGBT of Figure 3A is that in the DMOS device the substrate layer 82 is an N+ type region. For the IGBT (of Figure 3A) the emitter electrical contacts (not shown) conventionally contact the P+ type deep body regions 48a, 48b and the N+ type emitter regions 44a, 44b. The gate layer 46 is electrically contacted by the polysilicon bridges (not appearing in this view) as described above. A collector contact (not shown) is conventionally provided at the back side of the device in contact with the P+ type substrate region 60. As shown, the base region 64 is a conventional floating (or open base) which does not have its own electrical contacts. The electrical contacts for the DMOS devices are identical to those for the IGBT device. For both the IGBT and DMOS devices as shown in respectively Figures 3A and 3B, all of the conductivity types of the regions may be reversed. Thus in the reversed version of the IGBT device, the base region (epitaxial layer) is P type, the collector region is N+ type, and the emitter region is P+ type. For the reversed polarity version of the DMOS device, the drain region is a P- type region. Thus the reversed polarity version of the DMOS device is a P channel DMOSFET device instead of the N channel (i.e., channel region 64) device shown in Figure 3B. As shown in Figure 2, the active device cell 42 is delineated by the N+ type regions 44a, 44b which enclose a P+ type island 40 which is the voltage clamp region. Since the active device cell 42 is preferably annular in shape in the plane defined by the principal surface of the substrate, the active device cell (i.e., regions 68a, 68b, 68c of Fig. 3A) has a higher breakdown voltage than would a cylindrical junction. Since the clamping P+ type region 40 preferably has a spherical shape in cross section as shown in Figures 3A and 3B, the breakdown of the device will always occur around the P+ type clamp junction region 40 rather than at the active device cell region 42. For the IGBT version of the device as shown in Figure 3A, the P+ type clamping region together with the N-type region 64 and the P+ type substrate 60 form a PNP bipolar junction transistor. Thus the safe operating area (SOA) of the device is improved because a PNP-bipolar junction transistor has a larger safe operating area than does an ordinary prior art insulated gate bipolar transistor. For the DMOS embodiment of the invention shown in Figure 3B, a zener diode which breaks down at high voltage is formed by the junction between P+ type clamping region 40 and the N- type region 64 in which the P+ type clamping region 40 is formed. This PN junction high voltage zener diode improves the safe operating area (SOA) of the device. With reference to the safe operating area, in accordance with the invention the provision of a breakdown device (a zener diode or transistor) by means of a clamping region provides the benefit of allowing the device including the clamping region to break down at a much lower voltage. Thus even though a particular current is still passing through the device, the clamping region will break down at a a voltage lower than that at which the active portion of the device will break down, and so the clamping region will carry most of the current which thus bypasses the active device area. Thus, the normal operation of the device will still be within the safe operating area current curve. In accordance with the invention, the shape of the active area cells 42, 50, 52, 54, 56 and 58 as shown in Figure 2 need not be square in the top view. Preferably the shape of each of the cells is approximately radially symmetric, i.e., a circle, square, hexagon, octagon or similar shape. An advantage of radial symmetry is increasing the active cell breakdown voltage by using the third dimension, that is the thickness of the semiconductor material, to ensure that depletion takes place uniformly. If the cells are not contiguous, i.e., as with circular cells, the area between the cells is preferably a "dead" (inactive) region having the same doping as the outer (i.e., body) region of each cell. In another embodiment, the cells are square, circular, or are elongated closed rectangles each enclosing a gate region, and multiple clamping regions are provided in the gate region between the two channel regions of each rectangle. A transistor cell in accordance with this embodiment is shown in top view in Figure 4, and has a similar structure to that shown in Figure 2, except that multiple P+ clamping regions 40a, 40b, 40c, 40d are provided in gate region 46, and only two bridges 46a, 46b are provided. N+ regions 44a, 44b and P+ body regions 48a, 48b enclose the cell, which is an elongated rectangle in shape. In one embodiment of the invention, the transistor is for use at a 600 volt typical ordinary operating level. Such a device rated at 600 volts typically would have an actual breakdown in excess of 700 volts to provide a safe operating margin. The typical dimensions for one cell for such a device are described hereinafter with reference to Figure 2. The spacing between the P+ type diffusions 40 and 44b, that is the width of the cell 42, is typically 15 microns to 20 microns. This spacing is an edge of the voltage clamp region 40 to the nearest edge of the N+ type regions 44a or 44b. This distance is the spacing when the P+ type diffusions are masked during fabrication. The actual spacing when the device is completed will typically be less due to the lateral diffusion effect when the device is fabricated. The typical width of the P+ type clamping region 40 is about 10 microns. This width is defined to accommodate a minimum sized electrical contact to the P+ type clamping region 40. The width of the cell 42 is typically about 30 to 40 microns. This includes the N+ type region 44a, the gate region 46, the P+ type region 40 and the other N+ type region 44b as defined when the diffusions are masked. In other embodiments which use for instance circular, or hexagonal shaped cells, the dimensions are preferably approximately the same. The polysilicon bridges 46a, 46b, 46c are each preferably about 7 microns wide (i.e., the dimension of bridge 46a in a direction perpendicular to line X-X). In a typical power transistor device there are approximately 10,000 such cells 42 to switch a current of about 50 amps. The safe operating area curve for the above described IGBT device is as shown in Figure 5 which shows collector-emitter current I CE plotted against collector-emitter voltage V CE . The maximum current is at I 1 . The SOA I of the IGBT embodiment of the present invention (solid line) lies within the SOA WB of a prior art wide base PNP transistor. The SOA I of the present invention is generally superior, as shown, to the SOA P of a prior art IGBT (dotted line). As shown, the breakdown voltage of one embodiment of the present invention is at about 750 volts, which corresponds to the avalanche voltage V A of a prior art wide base PNP transistor. A wide base PNP transistor has an SOA WB (interrupted line) approaching the ideal; however, such a structure as is well known is not suitable for a power transistor. The SOA for the transistor cell in accordance with the IGBT embodiment of the present invention is effectively a combination of the SOA of a bipolar transistor and the SOA of the active device of each cell. The transistor in accordance with the invention is formed by conventional masking, implantation, and diffusing processes as is known in the art. The process steps in accordance with the invention in the preferred embodiment are as follows for the IGBT device shown in Figure 3A. Substrate 60 (see Figure 6a) is preferably silicon having a conductivity of about .005 to .01 Ω-cm and a <100> crystal orientation, but semiconductor materials other than silicon having other conductance, conductivity type, and crystal orientation are also appropriate. Substrate P+ type region 60 is conventionally doped to a level of about 5 x 10 18 ions per cm 3 . For the IGBT embodiment of the invention, the P+ doping is achieved using boron. For the DMOS embodiment of the invention, the substrate N+ doping level is preferably approximately 10 19 ions per cm 3 and is achieved using arsenic or phosphorus. The N type region 62 is then grown epitaxially to approximately 5-10 microns thick and provided with a arsenic or phosphorus doping of about 1 x 10 16 to 5 x 10 17 atoms per cm 3 . Grown conventionally on top of the N type region is the N- type epitaxial layer 64, which is grown to approximately 60 microns thick. The doping level of the epitaxial layer 64 is about 1 x 10 14 per cm 3 . Field oxide layer 140 is conventionally grown over epitaxial layer 69. As shown in Figure 8b, by means of a first mask the field oxide layer 140 is conventionally patterned using photoresist. In areas exposed by the mask, field oxide 140 is removed to form openings for passage of impurities for formation of P+ regions 48a, 40. P+ type deep body region 48a and clamping region 40 are conventionally formed, preferably in one step. This is done preferably by subjecting the wafer to an ion implantation process using boron, a dosage of about 10 16 ions per cm 2 , and an implant energy of about 120 KeV. Alternatively, regions 48a, 40 are formed by a boron nitride injection which is used as a P+ diffusion source. The wafer is then subjected to a diffusing process. Regions 48a and 40 preferably are each about 3 to 6 microns deep and have a doping level of about 5 x 10 19 to 10 20 atoms/cm 3 . Then a layer of silicon dioxide 142 about 500 nm in thickness is regrown over the openings in field oxide layer 140. Then as shown in Figure 6c, a second mask is used to conventionally pattern and remove portions of field oxide 140 and regrown oxide 142, leaving portions 144 of the two combined oxide layers 140, 142 over P+ regions 48a, 40, and also over the high voltage termination regions at the edge (not shown) of each die of the wafer. Silicon dioxide layer 74 (see Figure 6d) is formed on epitaxial layer 64. Silicon dioxide layer 74 is thermally grown to a thickness of about 100 nm and serves as the gate insulating layer. Polycrystalline silicon layer 46 is the gate layer and is formed over silicon dioxide layer 74 typically by chemical vapor deposition, to a thickness of about 500 nm. Other conductive materials can be used as the gate layer. Silicon dioxide layer 74 and polycrystalline silicon layer 46 are then conventionally patterned (see Figure.6e) using a photoresist layer and a third mask (not shown). Then the exposed portions of gate layer 46, and the portions of silicon dioxide layer 74 lying thereunder are removed. Figure 8f shows the configuration of a portion of the polysilicon gate layer 46 after patterning in a top view, showing polysilicon gate layer "bridges" 46a, 46b, and 46c respectively to adjacent gate regions 52b, 54b, and 58b of respectively cells 52, 54, and 58, as discussed above in connection with Figure 2. Figure 6f illustrates the repetitive pattern of polysilicon gate layer 46 after it is patterned. The opening 40b in gate layer 46 is for electrical contact to clamping region 40 in the underlying epitaxial layer (not shown). P type body regions 68a, 68b, (see Figure 6e) are formed conventionally by ion implantation using polycrystalline silicon layer 46 as a mask. In one embodiment, dopants such as boron or aluminum are implanted into the wafer with a dosage of about 10 14 per cm 2 and an implant energy of about 40 to 100 KeV. The wafer is then subject to a diffusion process so that regions 68a, 68b, are each about 3 to 4 microns deep and have a surface doping level of about 1 x 10 17 to 10 18 ions per cm 3 . A thin silicon dioxide layer (not shown) is thermally grown over the entire wafer surface to a thickness of about 200 nm during the diffusion process. The N+ type source regions 78, 44a, are then conventionally formed preferably by ion implantation using arsenic or phosphorus at a dosage of about 8 x 10 15 per cm 2 and an implant energy of about 60 KeV. The wafer is then subjected to a diffusion process. The N+ type regions 78, 44a, each preferably are less than one micron deep and have a doping level of about 5 x 10 19 to 10 20 ions per cm 3 . Thus polysilicon layer 46 serves as the mask for both the P type body regions 68a, 68b and N+ type source regions 78, 44a. Then a fourth mask (not shown) is used to form an N+ type body region block implant (not shown) at the edge of each die only. This block implant prevents the P type body regions from going into the high voltage termination region at the die edge. Then conventionally an insulating layer of PSG or BPSG or silicon dioxide or silicon nitride (not shown) is formed over the surface of the transistor. This insulating layer is conventionally patterned using a fifth mask, to open contacts to the polysilicon layer 46 and to the various semiconductor regions at the principal surface of the epitaxial layer 64. A layer of conductive material such as aluminum (not shown) is then formed over the wafer and conventionally patterned by a sixth mask (not shown) to provide electrical contacts to the emitter/body regions, the gate layer, and the clamping region. A second layer of conductive material (not shown) is conventionally formed on the backside of the wafer to electrically contact the substrate 60. A passivation layer is then conventionally formed (not shown) and openings conventionally formed through the passivation layer by a seventh mask for the bonding pads. The above description of the fabrication of the transistor is illustrative and not limiting. Other embodiments of the invention will have other process parameters. The fabrication of power transistors is well-known in the art and is described in texts such as Semiconductor Power Devices by Sorab Gandhi, John Wiley & Sons, 1977, and Modern Semiconductor Fabrication Technology, Peter Gise and Richard Blanchard, Prentice-Hall, 1986. The intermediate N type layer region 62 shown in Figures 3A and 38 advantageously stops semiconductor depletion to that point and prevents undesirable punch through from the P+ type body region to the top of the substrate layer 60. The device would function therefore in an alternative embodiment without the N type layer region 62. The epitaxial N- type layer 64 would in this case preferably be almost double the thickness compared to a transistor with the N- type layer 62, 110 included. The N type region 62, 110 thus provides the benefit of a thinner epitaxial layer. Note that as is known in the art, depletion starts from the top and extends from the surface towards the substrate. If the N- type layer region 62, 110 is removed, then depletion tends to reach through to the P+ type substrate region 60 of Figure 3A. This may disadvantageously cause injection from the substrate P+ type region 60 in the IGBT device of Figure 3A, which will therefore undesirably cause a low breakdown voltage. In other embodiments of the device, the invention is applicable to high voltage integrated circuits as well as to discrete power transistors as described above. In the high voltage integrated circuit, the active portion of each cell is preferably protected through a zener diode clamp in accordance with the invention. The above description of the device is illustrative and not limiting. Other embodiments of the invention will be apparent in light of the invention to one of ordinary skill in the art.

Claims: A transistor comprising a plurality of cells wherein each cell comprises: a semiconductor body (64) of a first conductivity type; a substantially annular first region (48) of a second conductivity type formed in the semiconductor body; a second region (44) of the first conductivity type formed in the annular region; and a conductive gate region (46) overlying a surface of the semiconductor body and having its extent defined by the interior portion of the second region; characterised by: a clamping region (40) of the second conductivity type formed in the interior portion of the first and second regions, the clamping region having a breakdown voltage lower than the breakdown voltage of the other portions of the cell, a cross-sectional shape different from that of the annular first region (48), and a depth and a doping level the same as that of the annular first region. A transistor as claimed in claim 1 wherein the annular region (48) and second region (44) are substantially square in shape in a plane defined by a principal surface of the semiconductor body. A transistor as claimed in claim 1 or 2 wherein the clamping region (40) is of a spherical shape in a plane perpendicular to a plane defined by a principal surface of the semiconductor body. A transistor as claimed in claim 1 or 2 wherein the transistor is an insulated gate bipolar transistor, and the clamping region (40) and semiconductor body (60,64) form portions of a bipolar junction transistor. A transistor as claimed in claim 1 or 2 wherein the transistor is a field effect transistor and the clamping region (40) and semiconductor body (64) form a zener diode. A transistor as claimed in any preceding claim wherein the conductive gate region (40) comprises an extended portion which is the conductive gate region of an adjacent cell. A transistor as claimed in claim 6 wherein the conductive gate region of a first cell comprises a layer of polycrystalline silicon connected to the conductive gate region of at least one adjoining cell by an extension of the layer of polycrystalline silicon. A method of making a cell for a transistor comprising a plurality of cells, the method comprising the steps of: forming in a semiconductor body (64) of a first conductivity type a substantially annular first region (48) of a second conductivity type; forming a second region (44) of the first conductivity type in the annular region; and forming a conductive gate region (46) overlying a surface of the semiconductor body and having its extent defined by the interior portion of the second region; characterized by forming a clamping region (40) of the second conductivity type in the interior portion of the first and second regions, the clamping region having a breakdown voltage lower than the breakdown voltage of the other portions of the cell, a cross-sectional shape differing from that of the annular first region (48), and a depth and a doping level the same as that of the annular first region.

Inventors: BENCUYA IZAK, YILMAZ HAMZA, BENCUYA, IZAK, YILMAZ, HAMZA
Applicants: SILICONIX INC, SILICONIX, INC.
Application year: 1990
Main classification: H01L29
IPC codes: H01L21, H01L29, H01L27