HIGH BREAKDOWN VOLTAGE SEMICONDUCTOR DEVICE

Abstract: A semiconductor device formed with a highly doped impurity region (16) of the same conductive type as the semiconductor substrate (10), wherein the highly doped impurity region (16) extends laterally by a prescribed amount opposite a first impurity region (12) with its center opposite the center of the first impurity region (12). The lateral width (T) of the highly doped impurity region (16) is such as to satisfy t1 < T < t1 + 2WO,where t1 is the width of the first impurity region (12) and WO is the separation in the depth direction between the first impurity region (12) and the highly doped impuirity region (16).

Description: This invention relates to planar semiconductor diode and transistor devices. It is particularly concerned with high breakdown voltage planar semiconductor diodes and transistors. Specifically, it relates to a planar semiconductor diode or transistor device having an improved breakdown voltage achieved by preventing excessive electric field concentrations at high curvature portions of the main junctions. Semiconductor devices with a high breakdown voltage were conventionally obtained by utilizing what is known as a mesa structure or a planar structure having a guard ring. The first structure has the advantage that (if the device is a diode) the PN junction, or (if the device is a transistor) the junction between base and collector are flat, so electric field concentrations do not occur. It is therefore widely used for semiconductor devices of high breakdown voltage. However, with a mesa type structure, not only is it necessary to form a mesa to obtain the high breakdown voltage, but in addition the mesa has to be covered with a protective material. This complicates the manufacturing process. Semiconductor devices of planar structure having a guard ring are therefore often used, because they can be easily obtained by a simple manufacturing process. However, also in the case of planar semiconductor devices with a guard ring, if high breakdown voltages (1KV or more, for example) are to be obtained, as many guard ring regions must be formed as possible, so as to raise the breakdown voltage by reducing the electric field concentration at the portions of high curvature of the PN junction (in the case of a diode) or the base-collector junction (in the case of a transistor). This made it difficult to reduce the element size. Moreover, particularly with recent progress in CVD techniques, forming high-resistance materials such as polysilicon has become easier, and the so-called "resistive field plate" method has attracted attention, in which a high-resistance layer is provided on top of a dielectric arranged on the peripheral surface of a PN junction. Compared with use of a guard ring, this resistive field plate method has the advantages that only a comparatively small area is needed, the breakdown voltage dependence on junction depth is small and it is not so dependent on the accuracy of the transverse spread of the junction as the guard ring method is on the accuracy of the separation from the guard ring junction. However, neither this method nor the guard ring method enable electric field concentrations at curved portions of the PN junction to be relieved as effectively as they can be with the mesa structure. United States Patent No. 3,717,515 discloses a method for fabricating a monolithic integrated circuit including at least one pedestal transistor device in order to enable the formation of transistor devices having smaller dimensions than previously without sacrificing high frequency switching performance. A planar transistor is disclosed in Solid State Technology Vol. 23, no. 3, March 1980 pages 98-105 RCA Copy, R. Denning et al "New technologies advance power semiconductor". An object of this invention is to provide a planar semiconductor device wherein an improved breakdown voltage is achieved by reducing to a great extent electric field concentrations at high curvature regions of PN junctions (in the case of diodes) or between the base and collector (in the case of transistors). The preambles of independent claims 1 and 2 correspond to a conventional planar diode and transistor respectively. According to this invention, there is provided a planar semiconductor diode device provided with: a first impurity region of a second conductivity type formed in a prescribed region of a semiconductor substrate of a first conductivity type; and a first highly doped impurity region of the first conductivity type formed in a region at the back of the said semiconductor substrate opposite said first impurity region and extending laterally by a prescribed amount; characterised in that the lateral width of said first highly doped impurity region satisfies: t1 ⋞ T ⋞ t1 + 2WO where t1 is the width of said first impurity region, T is the lateral width of said first highly doped impurity region, and WO is the separation, in the depth direction, between said first impurity region and said first highly doped impurity region. A planar semiconductor transistor device according to this invention is set out in claim 2. In this way an improved breakdown voltage is achieved by reducing to a great extent electric field concentrations at high curvature regions of the PN junction. Embodiments of this invention will now be described, by way of example, with reference to the accompanying drawings in which:- Fig. 1 is a cross-sectional view of a first preferred embodiment of this invention; Fig. 2 is a cross-sectional view of a second preferred embodiment of this invention. Fig. 3 is a cross-section showing the position where the highly doped impurity region of this invention is formed. Fig. 4 is a plan view corresponding to Fig. 3 seen from the side of the main face. Fig. 5 is a doping concentration profile of the various impurity regions of the cross-section shown in Fig. 2. Fig. 6 is a characteristic showing the relationship between the breakdown voltage and the sheet resistance of the collector region, taking the separation Wo between the first impurity region and the highly doped impurity region (in the case of a flat junction) as a parameter. Fig. 7 is a characteristic of the relationship between the electric field distribution of this invention and position in the transverse direction of the semiconductor substrate. Fig. 8 is a cross-sectional view showing a third preferred embodiment of this invention. Fig. 9 is a cross-sectional view given in explanation of the third embodiment, shown in Fig. 8. Fig. 10 is a view showing the relationship between the separation Wg between the first impurity region and the lightly doped impurity region and the breakdown voltage. Fig. 11 is a view showing the relationship between the specific resistance and the width of the depletion layer. Fig. 12 is a cross-sectional view showing a fourth embodiment of this invention. Fig. 13 is a cross-sectional view showing a fifth embodiment of this invention. Fig. 14 is a cross-sectional view showing a sixth embodiment of this invention. Fig. 15 is a cross-sectional view given in explanation of the fifth embodiment of this invention, shown in Fig. 13. Fig. 16 is a view showing the relationship between the width of the resistive field plate layer and the breakdown voltage. Fig. 1 is a cross-sectional view showing a first preferred embodiment of this invention. The case where the semiconductor substrate is an N type diode will be described. As shown in Fig. 1, a doping level of an N type semiconductor substrate 10 is about 10¹³⁻¹⁴ cm⁻³. An anode region 12 of P type conductivity, with surface impurity concentration 10¹⁹⁻²⁰ cm⁻³ and constituting a first impurity region is formed in a prescribed region of the main face of the semiconductor substrate. A guard ring region 14 is formed in a prescribed region of the main face of the semiconductor substrate 10 so as to surround the anode region 12. Fig. 1 shows a single guard ring, but two or more guard rings could be used. A resistive field plate structure could also be used. An N+ type highly doped impurity region 16 of surface impurity concentration 10²⁰ cm⁻³ is formed facing the anode region 12 on the back face of the semiconductor substrate 10. It is preferred to farm the highly doped impurity region 16 such that its middle region is in the same position as the anode region 12. The side face portion of the highly doped impurity region 16 is formed by introducing the impurity up to a position defined by adding a width WO, or rather less than this, to the width of the anode region 12. WO is the separation in the depth direction between the anode region and highly doped impurity region. A description will now be given for the case of the NPN transistor of breakdown voltage 1500 V and maximum collector current 3.5 A shown in Fig. 2. The substrate of the transistor of Fig. 2 is an N-type semiconductor substrate of doping concentration 10¹³⁻¹⁴ cm⁻³, and of thickness for example 300 micrometers. A base region 22 of P-type conductivity of surface impurity concentration 10¹⁸⁻¹⁹ cm⁻³. constituting a first impurity region, is formed in a prescribed region of the main face of the semiconductor substrate 21. The diffusion depth of this region is for example 50 micrometers. An N+ conductivity type emitter region 23 of surface impurity concentration 10²¹ cm⁻³, of prescribed depth of diffusion and constituting a second impurity region is formed within the base region 22. A guard ring region 24 is formed in a prescribed region of the main face of the semiconductor substrate 21 so as to surround the base region 22, leaving a prescribed separation. Fig. 2 shows a single guard ring, but two or more could be provided. An N+ type highly doped impurity region 25 of surface impurity concentration 10²⁰ cm⁻³ is formed on the back face of the semiconductor substrate 21 opposite to, and with its center in the same position as, the base region 22. However, it is not essential for the centers of these regions to be in the same position; suitable modifications can be made in accordance with design requirements. The diffusion depth of this region is for example 150 micrometers. The side face of the highly doped impurity region 25 is formed so as to be positioned at a location specified from the width of the emitter region by adding WO, which is the separation in the depth direction between this base region and the highly doped impurity region, to the width of the base region 22. Fig. 3 is a cross-sectional view given to explain how the position of formation of the highly doped impurity region of this invention is specified. Portions which are the same as in Fig. 2 are given the same reference numerals. As shown in Fig. 3, the lateral width T of the highly doped impurity region 25 is formed so as to satisfy t2 < T⋞ t1 + 2WO and with its center in the same position as the center of the base region; t2 is the width of the second impurity region; and WO is the separation in the depth direction between the first impurity region and the highly doped impurity region. Fig. 4 is a plan view seen from the main face of Fig. 3. As shown in Fig. 4, the widths of the various regions described above represents the spread of the diffusion region on the surface of the semiconductor substrate. This also applies to the collector region. Fig. 5 shows the doping profile of the various regions with depth from the semiconductor surface. The reason why the projection width T of the highly doped impurity region 25 of the semiconductor device of this invention is chosen within the range t2 < T ⋞ t1 +2WO is as follows. In the semiconductor device shown in this invention in order to make the internal resistance of the collector small, the lateral width T of the highly doped impurity region 25 should be made large. However, to increase the breakdown voltage of the semiconductor device, the lateral width T should be small. However, the main factor that determines this breakdown voltage is the electric field concentration due to the depletion layer extending from the base region 22. This electric field concentration is most marked in curved regions of the main junction (boundary region between the base region 22 and collector region 21). In general if the diffusion depth of the base region is about 40 to 50 micrometers, the electric field concentration is most marked in the approximately ϑ=45° direction of the curved portion 6, but, even if the diffusion depth is not so great as this electric field concentration at curved portions is believed to occur to about the same degree, not being much affected by small changes in the vertical direction. The extension of the depletion layer increases with increased applied voltage. That is, the breakdown voltage is adversely affected if the width T of the region 25 is made greater than the width t1 of the base region 22 and twice the separation WO between the base region 22 and the highly doped impurity region 25. In contrast, if, with the aim of increasing the breakdown voltage, the lateral width T of the region 25 is made less than the width t2 of the emitter region 23, sufficient collector current cannot be obtained, since the internal resistance of the device becomes large. The projecting portion should therefore desirably be in the range of ϑ=45° of the emitter junction. In other words, sufficient collector current can be obtained if the lateral width T of the region 25 is made to satisfy the inequality: t2 < T ⋞ t1 + 2WO. Furthermore, satisfactory reduction of electric field concentrations at curved portions of the base-collector junction formed between the base region 22 and collector region 21 can also be obtained, and the breakdown voltage increased. Additionally, the highly doped impurity region 25 is easy to form, and enables elements of small size to be produced since only the minimum necessary number of guard rings need to be formed. In the above description, the lateral width T of the highly doped impurity region 25 has been chosen within the range: t2 < T ⋞ t1 + 2WO. However, if, depending on the requirements imposed on the semiconductor device, the internal resistance of the collector has to be made small, it can be chosen such that: t1 ⋞ T ⋞ t1 + 2WO. The reason why the breakdown voltage can be increased by the formation of such a highly doped impurity region 25 can easily be understood from the characteristics (A...D) of the relationship, shown in Fig. 6, between the breakdown voltage and the collector region sheet resistance. In this Figure, the characteristic A corresponds to the variation of the breakdown voltage of a semiconductor device [diffusion depth Xj of the base region = 50 micrometers] which is essentially of mesa structure. Characteristics B to D show the variation in breakdown voltage in the case of a semiconductor device of guard ring planar structure with a highly doped impurity region with a flat junction. In the case of characteristic B, the separation between the highly doped impurity region 25 and the base region 22 is 200 micrometers; in the case of characteristic C, the separation between the highly doped impurity region 25 and the base region 22 is 130 micrometers; in the case of characteristic D, the separation between the highly doped impurity region 25 and the base region 22 is 80 micrometers. Consequently, since, in the case of the semiconductor devices to which this invention relates, there are very marked concentrations of electric field at the curved portions of the PN junction in the case of a diode or the base-collector junction in the case of a transistor, the breakdown voltage is increased for increased separation, in the depth direction, at these portions i.e. between the highly doped impurity region and the anode region or base region. In other words, as is clear from the electric field concentration curve 1 of Fig. 7, the breakdown voltage can be substantially raised by making the separation between the anode region or base region and highly doped impurity region directly below the anode region or base region and guard ring region, which have the largest effect on the breakdown voltage, as large as possible (subject to consideration regarding increase in the resistance of the cathode region or collector region). In the case of the breakdown voltage of 1500 V shown in the embodiment of Fig. 2, this separation WO may be taken as 100 micrometers. A third embodiment will now be described, with reference to Fig. 8. The third embodiment is a structure in which a highly doped impurity region 28 is formed that is shallower than a projection 27 thereof which corresponds to the region 25 in the second embodiment. The effect of this invention can be satisfactorily obtained with this third embodiment also. Furthermore, since the highly doped impurity region 28 is shallow, there is the advantage that more current can flow since the internal resistance is less than in the case of the second embodiment. Fig. 9 is a cross-sectional view given in explanation of the third embodiment. The device is formed such that WO < Wg, where the separation between the first impurity region 22 and the highly doped impurity region 28 is taken as Wg. The separation Wg is determined by the extension of the depletion layer from the first impurity region 22. Fig. 10 is a view showing the relationship between the breakdown voltage and the separation Wg when the specific resistance ρp of the first impurity region 22 is 0.06 Ω -cm, and the specific resistance ρp of the semiconductor substrate 21 is 60 Ω -cm. In Fig. 10, the values in the case of a conventional mesa construction are shown for purposes of comparison. The symbol O in Fig. 10 indicates the mesa structure, while the symbol Δ indicates the case where the separation Wo is 110 µm and the symbol X the case where the separation Wo is 90 µm. A breakdown voltage of 1.7 KV can be obtained when the separation Wo is 100 µm and the separation Wg is 150 µm. This corresponds to the case where the thickness tn of the collector region of the mesa structure is 110 µm. In Fig. 11, the specific resistance ρn Ω -cm of the semiconductor substrate 1 is taken along the vertical axis, while the width of the depletion layer when a reverse bias voltage is applied is taken along the horizontal axis. In Fig. 11, the width of the depletion layer when ρn is 60 Ω -cm is about 150 µm. This invention is therefore effective when setting the separation Wg between the first impurity region and the shallow highly doped impurity region shown in Fig. 9 such that the width of this depletion layer is not exceeded for each respective ρn. This embodiment has been described with reference to a transistor, but clearly it could be applied to a diode as in the first embodiment. Also, though the above description has been given with reference to a planar construction having a guard ring, the invention is not restricted to this and could also be applied to the resistive field plate construction shown in Fig. 12. Fig. 12 is a cross-section showing an embodiment of this invention applied to the case of a power transistor employing a resistive field plate configuration. Fig. 13 is a cross-section for the case of a diode. Since the effect of these embodiments is the same, for this embodiment we shall describe as an example the case of a power transistor. In Fig. 12, a silicon dioxide layer of thickness 3 microns is formed by heat treatment in a steam atmosphere of for example an N-type substrate. If the thickness of this SiO2 layer is insufficient, a further layer of SiO2 or Si3N4 etc. may be deposited by the CVD method. Next this silicon dioxide layer is partially removed by photolithography, and phosphorus atoms are diffused into it to form an N+ highly doped impurity projecting portion 122. The main face is formed by mechanically lapping the opposite face of the substrate by a prescribed amount, leaving a high resistance layer 121. The main face of this N type high resistance layer 121 is then again subjected to heat treatment in a steam atmosphere, to form a SiO2 layer of thickness 1.5 micrometer. This SiO2 layer is then partially removed by once more carrying out photolithography. Boron atoms are then diffused into it to form a p-type base layer 123 (Xb = 10 micrometer. The central position of this base layer 123 corresponds to the center position of the N+ highly doped impurity projecting portion. An N+ type emitter layer 124 (Xe = 5 micrometer and N+ layer 125 are then formed in the same way. Next, a resistive field plate layer 127 is provided. The main face is then provided with an A1 electrode 128 and the back face with a Ni or the like electrode 129 to complete the transistor. In a semiconductor device having such a construction, the relationship between the width (t2) of the N+ type emitter layer 124 in the p type base layer 123, and the width (T) of the N+ type highly doped impurity region 122 is specified by t2 < T ⋞ t1 + 2WO (in the case of separation (WO) in the depth direction of the high resistance layer 121). Or, for a diode, in the case of the width (t1) of the p type anode layer 123, is set such that t1 ⋞ T ⋞ t1 + 2WO. The spread of the depletion layer into the N type resistance layer 121 is shown in Fig. 15 for the case when a reverse bias voltage V is applied to the PN junction for an internal field model of a semiconductor device, for example. In this Figure, the electric field represented by the vector (εO, εM, εR) is clearly a maximum. There is a substantial improvement in the breakdown voltage under the conditions approximately represented by WO < Wd since the structure is such that the electric field (εM) at the curved portion of the PN junction is not impeded by the N+ type highly doped impurity region 122. In this inequality, Wd is the width of the depletion layer shown in Fig. 15. As shown in Fig. 11, the width of the depletion layer is altered by the resistance of the semiconductor substrate. Fig. 16 gives the data for a conventional device which is not provided with a projecting N+ type highly doped impurity region. When Wo = ∞, the breakdown voltage of the flat junction is VB = 1.6 KV, and when Wo = 100 micrometer, it is VB = 1.4 KV. Thus, the structure of this invention shifts the breakdown voltage for Wo = 100 micrometer onto the level of that for Wo = ∞. The effectiveness of this invention has in fact been ascertained in enabling a breakdown voltage of about VB = 1.5 KV to be obtained for WR = 350 micrometer. The situation t2 <T and t1 ⋞ T are determined from the current characteristic. The above conditions are found, in the case of a transistor, by consideration of the spreading resistance in a collector layer of emitter layer width (t1), and, in the case of diode, by consideration of the spreading resistance in a cathode layer of p-type anode width (t1). Fig. 14 is a cross-sectional view showing a sixth embodiment of this invention. The embodiment of Fig. 14 is an embodiment in which a highly doped impurity region 130 is formed, which is shallower than the projecting portion 122 in the fourth embodiment shown in Fig. 12. This corresponds to the embodiment shown in Fig. 8. Because this highly doped impurity region 130 is shallow, the internal resistance can be made smaller than in the case of the fourth embodiment. This gives the advantage that the current can be made larger. As explained above, with a semiconductor device according to this invention, the breakdown voltage can be increased since the electric field concentration at curved portions of the junctions (PN junction in the case of a diode and base-collector junction in the case of a transistor) can be reduced.

Claims: A planar conductor diode device comprising: a first impurity region (12) of a second conductivity type formed in a prescribed region of a semiconductor substrate (10) of a first conductivity type; and a first highly doped impurity region (16) of the first conductivity type formed in a region at the back of the said semiconductor substrate opposite said first impurity region (12) and extending laterally by a prescribed amount; characterised in that the lateral width T of said first highly doped impurity region (16) satisfies: t1 ⋞ T ⋞ t1+ 2WO where t1 is the width of said first impurity region (12) and WO is the separation, in the depth direction, between said first impurity region (12) and said first highly doped impurity region (16). A planar semiconductor transistor device comprising: a first impurity region (22) of a second conductivity type formed in a prescribed region of a semiconductor substrate (10) of a first conductivity type; a second impurity region (23) of said first conductivity type is formed within the said first impurity region (22); and a first highly doped impurity region (25) of the first conductivity type formed in a region at the back of the said semiconductor substrate opposite said first impurity region (22) and extending laterally by a prescribed amount; characterised in that the lateral width T of said first highly doped impurity region (25) satisfies t2 < T ⋞ t1 + 2WO where t2 is the width of said second impurity region (23), t1 is the width of said first impurity region (22) and WO is the separation , in the depth direction, between said first impurity region (22) and said first highly doped impurity region (25). A planar conductor device as claimed in either of claims 1 or 2 including a second highly doped impurity region (28) of the first conductivity type adjacent said first highly doped impurity region (27) at the back of said semiconductor substrate (21) and formed to be shallower than said first highly doped impurity region (27). A planar semiconductor device as claimed in any of claims 1 to 3, characterised in that said first highly doped impurity region (16,25,27) is formed with its center in the same position as that of said first impurity region (12,22). A planar semiconductor device as claimed in any of claims 1 to 4, characterised by a guard ring region (14,24) of the second conductivity type surrounding said first impurity region (12,22). A planar semiconductor device as claimed in any one of claims 1 to 4, characterised by a resistive field plate (127) formed so as to surround said first impurity region (12,123), with the provision of a prescribed separation.

Inventors: EMOTO, TAKAO C/O PATENT DIVISION, SHIOMI, TAKEO C/O PATENT DIVISION
Applicants: KABUSHIKI KAISHA TOSHIBA
Application year: 1985
Main classification: H01L29
IPC codes: H01L29, H01L21