SEMICONDUCTOR RECTIFIER DIODE

Abstract: In accordance with the present invention, there is provided a semiconductor rectifier diode which has low loss, quick response and soft reverse recovery properties and is composed of three consecutive layers, i. e., a p-type emitter layer (3), an n-type base layer (4) and an n-type emitter layer (5), the p-type emitter layer being composed of a first portion (31) and second portions (32) which sur­ round said first portion, have a higher impurity concentra­ tion as compared with said first portion, and extend beyond said first portion toward said n-type base layer, and said base layer being composed of a first layer portion (41) which is adjacent to said n-type emitter layer and a second layer portion (42) which is located near a p-n junction (J₁) side and has a lower impurity concentration as compared with said first layer portion.

Description: SEMICONDUCTOR RECTIFIER DIODE The present invention relates to a semiconductor device, and in particular to a semiconductor rectifier diode. In recent years, IC's and LSITs have been rapidly introduced into a computer and associated various terminal units or various system apparatuses. A low voltage stabilized DC power supply is demanded to feed such an apparatus. Among¯various methods for obtaining a low voltage stabilized DC power supply from the commercial AC power source, the switching regulator system is excellent in its small size and high efficiency. Properties demanded for a rectifier diode to be used in the above described power supply are low loss, high stability and quick response. Diodes heretofore known did not fully satisfy these requirements. For example, a Shottky barrier diode described in the Japanese Patent Application Laid-open No. 107272/80 has a large reverse leak current and a rather large thermal instability. A p-i-n junction diode does not fully satisfy the low loss requirement. It has been proposed to make the p-type layer or n-type layer of a p-i-n diode extremely thin to improve the low-loss property as described in IEEE Transactions on Electron Devices, Vol. ED-23, No. 8, August 1976, p.p. 945 to 949. Similarly to the Schottky barrier diode, however, this approach does not always facilitate production of the p-i-n diode and has often brought about a difficulty in obtaining high fabrication yield due to variation in blocking voltage. An object of the present invention is to provide a semiconductor rectifier diode wherein the above described drawbacks are obviated. In other words, the object of the present invention is to provide a semiconductor rectifier diode which meets low loss, high stability and quick response requirements and is easily produced. Another object of the present invention is to provide a semiconductor rectifier diode having a soft reverse recovery characteristic. One feature of the semiconductor rectifier diode according to the present invention for attaining the above described object is that the diode has a first emitter layer of a first conductivity type, a base layer of a second conductivity type which is adjacent to the first emitter layer, and a second emitter layer of the second conductivity type which is adjacent to the base layer, and the first emitter layer is composed of a first portion and second portions surrounding the first portion, the second portions being formed deeper than the first portion and having a higher impurity concentration as compared with the first portions. Here, the emitter layer refers to a region wherein the impurity concentration is higher than the carrier concentration at the time of its forward operation. The base layer refers to a region wherein the impurity concentration is lower than the carrier concentration at the time of its forward operation. Owing to such a structure, it becomes possible to realize a semiconductor rectifier diode which excels a p-i-n junction diode in low loss and quick response properties and excels a Schottky barrier diode in stability, high voltage blocking capability and fabrication readiness. Another feature of a semiconductor rectifier diode according to the present invention is that the distance between second portions across a first portion in the first emitter layer, i.e., the width of the first portion therebetween is set at a sufficient value for pinching off the base region under the first portion by depletion layers extending from p-n junctions between the second portions and the base when a p-n junction existing between the first emitter layer and the base layer is reverse-biased with the rated voltage of the diode. This structure brings about a blocking voltage which is equivalent to that of the p-i-n junction diode. Still another feature of a semiconductor rectifier diode according to the present invention is that the impurity concentration in the base region is made to, as a whole, increase with the increase in distance from the p-n junction. Specifically, the base layer is constituted either from a plurality of layer portions respectively having different impurity concentrations or a single layer having an impurity concentration which continuously varies therein. This structure results in a semiconductor rectifier diode having a soft reverse recovery characteristic. The present invention will be apparent from the following detailed description taken in conjunction with the accompanying drawings, in which: Fig. 1 is a schematic oblique view of an embodiment of a semiconductor rectifier diode according to the present invention; Fig. 2 is a plan view of a semiconductor substrate of the device illustrated in Fig. 1; Fig. 3 is an enlarged view of the principal part of the device illustrated in Fig. 1; Fig. 4 shows the distribution of the impurity concentration within the device illustrated in Fig. 1; Fig. 5 shows characteristic curves illustrating the relationship between the width of the first portion of the p-type emitter layer and the forward voltage drop in the device illustrated in Fig. I; Fig. 6 shows characteristic curves illustrating the relationship between the width of the first portion of the p-type emitter layer and the blocking voltage in the device illustrated in Fig. 1; Fig. 7 shows characteristic curves illustrating the relationship between the surface impurity concentration of the first portion of the p-type emitter layer and the forward voltage drop in the device illustrated in Fig. 1; Fig. 8 shows a characteristic curve illustrating the relationship between the surface impurity concentration of the first portion of the p-type emitter layer and the reverse recovery time in the device illustrated in Fig. 1; Fig. 9 shows characteris#tic curves illustrating the relationship between the surface impurity concentration of the first portion of the p-type emitter layer and the reduction rate of the reverse recovery current in the device illustrated in Fig. 1; ; Fig. 10 is a schematic sectional view of another embodiment of a semiconductor rectifier diode according to the present invention; Figs. lla and llb respectively illustrate the structure and the impurity concentration profile of still another embodiment of a semiconductor rectifier diode according to the present invention; and Figs. 12a and 12b respectively illustrate the structure and the impurity concentration profile of still another embodiment of a semiconductor rectifier diode according to the present invention. Hereafter, embodiments of the present invention will be described in detail by referring to drawings. In Fig. 1, Fig. 2 and Fig. 3, a semiconductor substrate 100 has a pair of main surfaces 101 and 102. Between the pair of main surfaces 101 and 102, there are an n-type emitter layer 5 composed of an n++-type layer portion 51 which is adjacent to the main surface 102 and an n+-type layer portion 52 which is adjacent to the layer portion 51 and is lower than that layer portion 51 in concentration, an n-type base layer 4 which is adjacent to the layer 5 and is lower than the layer 5 in concentration, and a p-type emitter layer 3 which is adjacent to the main surface 101 and is adjacent to the layer 4 to form a p-n junction J1 Thus, the semiconductor substrate 100 has a structure composed of consecutive layers. The n-type base layer 4 is composed of a first layer portion 41 which is adjacent to the layer 5 and a second layer portion 42 which is placed between the layer portion 41 and the layer 3 and is lower than the portion 41 in concentration. The p-type emitter layer 3 is composed of a first portion 31 which is thin in thickness and low in concentration and second portions 32 which have a higher concentration than the first portion 31 and is formed more deeply than the first portion 31. The first portion 31 and the second portions 32 and formed in stripe-shape and are alternately arranged so that they face one another lengthwise. On the main surface 101, the first portion 31 is surrounded by the second portions 32 as illustrated in Fig. 2. Fig. 1 and Fig. 3 are sectional views viewed from the direction perpendicular to the length of the stripes. Thus, the p-n junction J1 is composed of a first portion J11 formed between the portions 31 and 42 and a second portion J12 formed between the portions 32 and 42. In Fig. 3, symbol I denotes a first laminated structure, each layer of which overlaps with the junction J11 when projected onto the main surface 102. Symbol II denotes a second laminated structure, each layer of which overlaps with the junction J12 when projected onto the main surface 102. On a portion of the main surface 101 whereon the p-n junction is exposed, an SiO2 film 10 is formed. On the exposed portion of the p-type emitter layer 3, an anode electrode 1 which is in ohmic contact with the p-type emitter layer 3 is formed. On the main surface 102, a cathode electrode 2 which is in ohmic contact with the n-type emitter layer is formed. On the SiO2 film, the anode electrode 1 is extended outward from the end of the exposed portion of the p-n junction J1 to serve as a field plate. A solid line in Fig. 4 illustrates the distribution of impurity concentrations within the second laminated structure II of the semiconductor substrate taken in a direction which is denoted by x in Fig. 3. In Fig. 4, the distribution of impurity concentrations within the first laminated structure I taken in a direction which is denoted by y in Fig. 3 is also illustrated. For the first laminated structure I, however, only a portion of the distribution which differs from that of the second laminated structure II is illustrated in Fig. 4 by with a broken line. A diode of this embodiment may be fabricated by using a well known semiconductor fabrication technique. An example of the fabrication is described in the following. At first, on one face of an n -type monocrystalline silicon wafer, an n-type layer and an n -type layer are successively formed by epitaxial growth technique to yield a silicon substrate. Phosphor is diffused selectively from one main surface and entirely from the other main surface. Thus, an -type layer 6 which is exposed to a periphery of one main surface 101 at the chip end and an n -type layer 51 which is exposed to the other main surface 102 are formed. Subsequently, boron is selectively diffused from the main surface 101 by using an oxide film as a mask, the second portions 32 being formed. From the main surface 101, boron is ion-implanted and subjected to heat treatment to form the first portion 31. Onto predetermined portions of main surfaces 101 and 102 of the silicon substrate, laminated films made of AlSi, Cr-Ni-Ag or the like are evaporated to form the anode electrode 1 and the cathode electrode 2. The SiO2 film 10 is deposited during the above described diffusion process or by the CVD method or the like. The function and effect of the above described diode will now be described. Under a so-called forward bias state wherein a positive voltage is applied to the anode electrode 1 with respect to the cathode electrode 2, the impurity concentration in the first portion 31 in the p-type emitter layer 3 is lower than that in the second portion 32 thereof. As a result, the diffusion potential of the first portion Jli within the p-n junction J1 becomes lower than that of the second portion J12 Accordingly, the main current flows mainly through the first laminated structure I wherein the first portion 31 serves as one of the emitters. When the first laminated structure I thus becomes the main current path, minority carriers contribute to operation between the first portion 31 and the anode electrode 1 because the diffusion potential is low and the first portion 31 is thin. And the barrier between the first portion 31 and the anode electrode is not an obstacle to the carrier movement. As a result, the forward voltage may be made smaller than that in the case where the second laminated structure II is the main current path. In addition, the total amount of impurities included in the first portion 31 of the p-type emitter layer 3 is less than that included in the second portions 32 since the first portion 31 of the p-type emitter layer 3 is thinner than the second portions 32 thereof and the former has a lower impurity concentration as compared with the latter. Under the forward bias state, therefore, the amount of carriers injected from the p-type emitter layer 3 into the n-type base layer 4 is small. Thus, it becomes possible to reduce the reverse recovery time required for transition from the forward bias state to the reverse bias state. Under a so-called reverse bias state wherein a negative voltage is applied to the anode electrode 1 with respect to the cathode electrode 2, a depletion layer formed near the p-n junction J1 extends mainly in the n-type base layer 4 in the vicinity of the second portion J12 due to the difference between the impurity concentration in the second portion 32 within the p-type emitter layer 3 and that in the n-type base layer 4. Therefore, the second layer portion 42 of the n-type base layer 4 located between the second portiions 32 and under the first portion 31 is pinched off by the depletion layer extending from the second portion J12 of the p-n junction. Accordingly, the strength of the electric field in the first portion Jll of the p-n junction is weakened. Since the first portion 31 is thin and has a low impurity concentration, the first portion J11 of the p-n junction tends to be easily punched through to the surface by the depletion layer extending in the p-type emitter layer side and therefore has a low blocking voltage. Owing to the depletion layer caused by the existence of the second portions 32, however, the voltage is blocked and the first portion J11 is prevented from being punched through. As a result, it becomes possible to obtain a blocking voltage which is equivalent to that obtained when the p-type emitter layer is composed of only the second portions 32. At this time, the depletion layer extending from the second portion J12 of the p-n junction J1 toward the other main surface 102 is prevented from further widening beyond the vicinity of the boundary between the first layer portion 41 and the second layer portion 42 included in the n-type base layer 4 or beyond the first layer portion 41. When the diode is switched from the forward conduction state to the reverse blocking state, the first layer portion 41 which is filled with injected carriers remains as a neutral region within the n-type base layer 4 even after the depletion layer has been formed. From the time when the reverse current reaches its peak value until the time when the carriers in the neutral region disappear, the reverse current flows while decreasing gradually, whereby the reverse recovery characteristic being softened. The "soft" reverse recovery characteristic means that the reduction rate diR/dt of the reverse current #R after it has reached its peak value is rather small. Should the reverse current decrease rapidly, a large voltage L di R/dt is induced by the inductance L included in the circuit comprising the diode, noises being incurred. As described above, embodiments of the present invention illustrated in Figs. 1, 2, and 3 yield a semiconductor rectifier diode which excels a conventional junction diode in low loss, quick response and soft recovery properties and excels a Schottky barrier diode in stability and high breakdown voltage properties. The p-type emitter layer 3 is divided into the first portion 31 and the second portions 32, and design objectives which are incompatible with each other such as a lowered loss and a raised breakdown voltage are separately achieved by the first and second portions, respectively. Accordingly, the design of the p-type emitter becomes easy. In addition, the blocking voltage is not lowered even if a defect such as a pinhole exists in the first portion 31. Thus, the fabrication yield may also be improved. Fig. 5 shows the dependence of the forward voltage drop upon the width Wch of the first portion 31 within the diode illustrated in Figs. 1, 2 and 3. Fig. 6 shows the dependence of the blocking voltage upon the width Wch. In these cases, the current density is approximately 60 A/cm2, the thickness L of the p first portion 31 is approximately 2 Vm, the thickness of the second portion 32 is approximately 5 Vm, the thickness of the second layer portion 42 existing between the bottom portion of the first portion 31 and the first layer portion 41 is approximately 6 pm, the thickness of the first layer portion 41 is approximately 12 pm, the impurity concentration in the first layer 15 -3 portion 41 is approximately 3 x 10 cm , and the surface impurity concentration in the-first portion 31 taken on the main surface 101 is approximately 5 x 1015 -3 cm . Symbols ¯ and 0 in Fig. 5 and Fig. 6 correspond to impurity concentrations of approximately 3 x 1013 -3 14 -# cm and approximately 1 x 10 cm - in the second layer portion 42, respectively. As seen from Fig. 5 and Fig. 6, reducing th#e width of the first portion 31 from 10 pm to 2 pm raises the blocking voltage by approximately 70 V only at a cost of increase in the forward voltage drop of approximately 0.02 V even when the surface impurity concentration in the first portion 31 is as low as 15 -3 approximately 5 x 10 cm and the thickness thereof is as thin as approximately 2 pm. The effect of the surface impurity concentration in the first portion 31 upon the characteristics of the diode in this embodiment will now be described. Fig. 7 and Fig. 8 respectively illustrate the forward voltage drop and reverse recovery time t rr when the thickness L of the first portion 31 is p chosen to be 1 pm (represented by Ipl) or 2 pm (represented by Lp2). The forward current density was conditioned to be approximately 60 A/cm2. The reduction rate of the forward current during reverse recovery was conditioned to be approximately 30 A/#s. Fig. 7 and Fig. 8 indicate that it becomes possible to lower the forward voltage and quicken the reverse recovery by decreasing the thickness of the first portion 31 to 1 to 2 ijm and lowering the surface impurity concentration thereof. For example, when the thickness of the first-portion 31 is 1 to 2 Vm and the surface impurity concentration is below 1 x 1016 cm 3, the forward voltage drop is approximately 0.7 V and the reverse recovery time trr is as low as 50 to 60 ns, a diode presenting a low loss and fast response being obtained. As the impurity concentration in the first portion 31 is lowered, reverse recovery is quickened because holes injected from the first portion 31 into the n-type base layer 4 under the forward bias state are decreased and whereby the amount of stored carriers is decreased. When the impurity concentration in the first portion 31 is lowered, the forward voltage is also lowered because the diffusion potential at the p-n junction J11 is lowered. Fig. 9 shows the reduction rate di /dt of R the reverse recovery current when the thickness L of p the first portion 31 is chosen to be approximately 2 um. The impurity concentration in the second layer portion 42 is chosen to be approximately 3 x 1013 cm 3. In Fig. 9, curve A represents the reduction rate when the impurity concentration in the first layer portion 41 is approximately 3 x 10 cm . In case of curve B, the impurity concentration in the first layer -3 portion 41 is approximately 3 x 1013 cm 3 which is equal to that of the second layer portion 42. In this case, the impurity concentration in the n-type base layer 4 is chosen to be uniform in the layer-stacking direction. As the surface impurity concentration in the first portion 31 is decreased, the reduction rate diR/dt is lowered as illustrated in Fig. 9, resulting in a soft reverse recovery characteristic. If the impurity concentrations in the n-type base layer 4 are made to distribute over the layer so that a portion located near the n+ -type emitter layer 5 will have a higher concentration, the reduction rate di R/dt is further decreased as represented by the curve A instead of the curve B. As illustrated in Fig. 6 as well, the lower the impurity concentration in a portion of the n-type base layer 4, which is located near the p-n junction J11 is, the higher the resulting blocking voltage is. Thus, it is possible to obtain the soft reverse recovery and high blocking voltage properties simultaneously by establishing the impurity concentration distribution in the n-type base 4 wherein a portion located near the p-n junction J1 has a lower impurity concentration and another portion located far from the p-n junction J1 has a higher concentration. The effect of the present invention will now be described referring to a numerical example. Table 1 shows measured values of forward voltage drop, blocking voltage, reverse recovery time and reduction rate of the reverse recovery current both for a conventional junction diode and a diode fabricated according to the present invention. The conventional junction diode used for the measurement is composed of p-type emitter layer having an impurity 19 - concentration of 1 x 10 cm and a thickness of 5 m, an n-type base layer having an impurity concentration 14 -3 of 5 x 10 cm and a thickness of 7 m, and an n- type emitter layer having an impurity concentration of 18 -3 5 x 10 cm 10and a thickness of 300 m. And the diode fabricated according to the present invention is composed of a p-type emitter layer which includes the first portion having an impurity concentration of 15 - 5 x 10 cm , a thickness of 2 m and a with of 4 m and the second portion having an impurity concentration of 1 x 1018 cm and a thickness of 5 pm, the n-type base layer which includes the first layer portion 15 - having an impurity concentration of 3 x 10 cm 10and a thickness of 10 pm and the second layer portion 13 - having an impurity concentration of 3 x 10 cm 10and a thickness measured between the second portion of the p-type emitter layer and the first layer portion of 3 pm, and an n-type emitter layer which includes ++ the n -type layer portion having an impurity concen 21 -3 tration of 1 x 10 cm and a thickness of 5 pm and the n -type layer portion having an impurity concentra 18 - tion of 5 x 10 cm 10and a thickness of 295 m. Table 1 EMI17.1 <tb> <SEP> Diode <tb> <SEP> Conventional <SEP> fabricated <tb> <SEP> diode <SEP> according <SEP> to <tb> <SEP> the <SEP> present <tb> <SEP> invention <tb> Forward <SEP> voltage <SEP> 0.95 <SEP> V <SEP> 0.73 <SEP> V <tb> Blocking <SEP> 150 <SEP> V <SEP> 180 <SEP> V <tb> voltage <tb> Reverse <SEP> 500 <SEP> nsec <SEP> 60 <SEP> nsec <tb> recovery <SEP> time <tb> Reduction <SEP> rate <SEP> 300 <SEP> A/p <SEP> sec <SEP> <SEP> 10 <SEP> A/sec <SEP> <tb> of <SEP> reverse <tb> recovery <tb> current <tb> As evident from Table 1, the diode fabricated according to the present invention excels the conventional junction diode in all properties of forward voltage, blocking voltage, reverse recovery time and reduction rate of reverse recovery current. Fig. 10 shows another embodiment of a semiconductor rectifier diode according to the present invention. The diode illustrated in Fig. 10 differs from the embodiment illustrated in Fig. 1 to Fig. 3 in the fact that the second portions 32 of the p-type emitter layer 3 is in contact with the first layer portion 41 of the n-type base layer 4 and the second layer portion 42 is not provided between each of the second portions 32 and the first layer portion 41. Although the blocking voltage of the diode thus constructed is slightly lowered as compared with the diode illustrated in Fig. 1 to Fig. 3, other properties are slightly improved. Figs. lla and Ilb show still another embodiment of a semiconductor rectifier diode according to the present invention. The semiconductor illustrated in Figs. lla and llb differs from the embodiment illustrated in Fig. 1 to Fig. 3 in the fact that the n-type base layer 4 is composed of a single region wherein the impurity concentration therein is continuously increased with the increase in the distance from the p-n junction J1 The diode thus constructed has characteristics which lie between those of the embodiment illustrated in Fig. 1 to Fig. 3 and those of the embodiment illustrated in Fig. 10. Figs. 12a and 12b illustrate still another embodiment of a semiconductor rectifier diode according to the present invention. The diode illustrated in Figs. 12a and 12b differs from the embodiment illustrated in Fig. 1 to Fig. 3 in the fact that a third layer portion 43 having an impurity concentration which is lower than that in the first layer portion 41 is provided between the first layer portion 41 of the n-type base layer 4 and the n -type layer portion of the n-type emitter layer 5. In such a structure, the the first layer portion 41 and the n -type layer portion 52 which are adjacent to the third layer portion 43 and have high impurity concentrations serve as potential barriers for carriers existing in the third layer portion 43. When the diode is switched from the forward conduction state to the reverse blocking state, therefore, carriers are trapped in the third layer portion 43 and can not disappear quickly. Thus, the reverse recovery characteristic is softened as compared with the embodiment illustrated in Fig. 1 to Fig. 3. The important condition of this embodiment is that the impurity concentration in the n-type base layer 4 is, as a whole, increased with the increase in the distance from the p-n junction J1 In Fig. 12, the above described condition has been satisfied by choosing the thickness of the third layer portion 43 to be smaller than that of the second layer portion 42. When the thickness of the second layer portion 42 is set to be equal to that of the third layer portion 43, the above described condition may be satisfied by making the impurity concentration of the third layer portion 43 higher than that of the second layer portion 42. Typical embodiments of the present invention have heretofore been described. However, the present invention is not restricted to those embodiments and various modifications may be applied to them. For example, the conductivity types of illustrated devices may be inverted. In addition, the first portion of the p-type emitter may also be formed in a shape other than the stripe, such as a circle, square or curve.

Claims: WHAT IS CLAIMED IS: 1. A semiconductor rectifier diode composed of a semiconductor substrate (100) having a pair of main surfaces (101, 102) thereon and a pair of main electrodes (1,2) provided on both of said main surfaces of said semiconductor substrate, said semiconductor rectifier diode comprising: said semiconductor substrate including a first emitter layer (3) of a first conductivity type which is adjacent to one (101) of said main surfaces and in contact with one (1) of said main electrodes, a base layer (4) of a second conductivity type being adjacent to said first emitter layer and forming a p-n junction (J1) between said first emitter layer and said base layer, and a second emitter (5) of the second conductivity type being adjacent to said base layer and to the other one (102) of said main surface and being in contact with the other one (2) of said main electrodes; and said first emitter layer including a first portion (31) and second portions (32) which together surround said first portion on said one main surface, extend further than said first portion in a direction perpendicular to said one main surface, and have a higher impurity concentration as compared with said first portion, a width (Wch) of said first portion of said first emitter layer, when viewed in a direction parallel to said main surfaces, having a sufficient value so that said base layer are pinched off at a portion thereof lying under said first portion and between said second portions of said first emitter layer by a depletion layer produced when the p-n junction is reverse-biased with the rated voltage of said diode, and the impurity concentration in said base layer being increased with increase in the distance from said p-n junction. 2. A semiconductor rectifier diode according to Claim 1, wherein said base layer comprises a first layer portion (41) which is adjacent to said second emitter layer and a second layer portion (42) which is adjacent to said p-n junction and has a lower impurity concentration as compared with said first layer portion. 3. A semiconductor rectifier diode according to Claim 2, wherein the impurity concentration in said first layer portion of said base layer is lower than the carrier concentration in the forward conductive state of the device and is sufficient to prevent the depletion layer from widening beyond said first layer portion under the reverse blocking state. 4. A semiconductor rectifier diode according to Claim 2, wherein said first portion of said first emitter layer is composed of a plurality of regions formed in a stripe form. 5. A semiconductor rectifier diode according to Claim 1, wherein said base layer is composed of a single region in which the impurity concentration is continuously increased with increase in the distance from said p-n junction. 6. A semiconductor rectifier diode according to Claim 5, wherein the impurity concentration in a portion of said base layer which is located near said second emitter layer is lower than the carrier concentration in the forward conductive state of the device and is sufficient to prevent said depletion layer from widening beyond said portion under the reverse blocking state. 7. A semiconductor rectifier diode according to Claim 5, wherein said first portion of said first emitter layer is composed of a plurality of regions arranged in a stripe form. 8. A semiconductor rectifier diode according to Claim 2, wherein a third layer portion (43) of the other conductivity type having an impurity concentration which is lower than that in said first layer portion of said base layer is put between said first layer portion of said base layer and said second emitter layer.

Inventors: MURAKAMI, SUSUMU, NAITO, MASAYOSHI, SHIMIZU, YOSHITERU, TERASAWA, YOSHIO
Applicants: HITACHI, LTD.
Application year: 1983
Main classification: H01L29
IPC codes: H01L29