Background of the Invention
The invention relates to a process for the production of a locally high, inverse current amplification (upwards current amplification) in a preferably double-diffused or implanted, inversely operated planar transistor which is arranged in a semiconductor body with an integrated circuit.
Digital circuits are known (Valvo-Reports, Volume XVIII, Edition 1/2 pages 215 to 226) which employ the so-called integrated injection logic (I.sup.2 L). The basic gate type of this technique requires only a very small crystal surface and the power loss can be kept extremely low. Bipolar, double-diffused or implanted transistors are used as switching elements. However, in contrast to a transistor of the usual planar technique in an inversely operated transistor, the emitter zone does not lie on the surface of the semiconductor body or an epitaxial layer deposited on a semiconductor substrate, but in the semiconductor body itself, that is to say beneath the surface of the epitaxially deposited layer. Thus an inversely operated npn-transistor has, for example, a n-conducting epitaxial layer, which normally forms the collector of a conventional transistor, forms the emitter, whereas the last n.sup.+ diffusion which normally forms the emitter of the conventional transistor now serves as the collector. This means that the switching element of the I.sup.2 L technique is an inversely operated bipolar npn-transistor in the conventional planar technique.
A fundamental advantage of the integrated injection logic consists in the high packing density which can be achieved on a semiconductor body for the integrated circuit. This is based on the fact that with a corresponding circuit concept, no mutual insulation is necessary. On the other hand, inversely operated transistors have a relatively small upwards current amplification, which here is referred to as upwards current amplification (B.sub.up), which corresponds to the inverse current amplification in normal operation. The upwards current amplification could in fact be improved by a correspondingly high basic doping of the epitaxial layer. However, a high doping of this type is not very effective as it reduces the efficiency of a lateral pnp-transistor as injector (see Valvo-Reports, Vol. 18, Edition 1/2, pages 216 and 217) and at the same time increases the emitter-base-capacitance of the I.sup.2 L- transistor.
Summary of the Invention
It is an object of the present invention to provide a novel inversely operated transistor which exhibits a high upward current amplification even in the case of a low-doped and high-ohmic epitaxial layer or in the case of a high-ohmic semiconductor substrate.
This object is attained in accordance with the invention in that prior to the base doping ions are implanted into the semiconductor body beneath the zone provided for the collector, and during following temperature treatments diffuse out into the adjacent zones.
The process in accordance with the invention allows the injector to be fully effective and at the same time permits a high upwards current amplification. As a result of the higher local doping introduced by ion implantation merely beneath the "active" base surface, the parasitic capacitance between the aforesaid base surface and the aforesaid emitter surface is likewise lower than with an increased basic doping of the overall epitaxial layer and of the substrate. This results in a substantial improvement in the speed-power product, which on the one hand is based on the high injector efficiency with a nevertheless adequate forwards current amplification and on the other hand on a reduction in the parasitic base-emitter-capacitance in relation to an overall increase in the doping.
Brief Description of the Drawings
A preferred embodiment of the present invention is illustrated by the drawings, in which:
FIG. 1 is a fragmentary plan view of an inversely operated transistor embodying the present invention;
FIG. 2 is an enlarged fragmentary sectional view taken along the line II--II of FIG. 1;
FIG. 3 is a graph showing the doping course in a section III--III of FIG. 2 where the penetration depth x is shown in .mu.m on the abscissa (compare arrow x in FIG. 2) and the doping concentration K in atoms-cm.sup.-3 is plotted on the ordinate; and
FIG. 4 is the doping force in a section IV--IV of FIG. 2 corresponding to FIG. 3.
Description of the Preferred Embodiments
A semiconductor body 1 consists of an n.sup.++ conducting semiconductor substrate having therein a buried layer 2. Above the layer 2 is an epitaxially deposited layer 3 of n type conductivity. The epitaxially deposited layer 3 has, for example, a layer thickness of 5 .mu.m and a specific resistance of 0.8 .OMEGA.cm corresponding to a doping of approximately 10.sup.16 atoms-cm.sup.-3. In this connection, see the horizontal line 31 in FIGS. 3 and 4. The doping course of the semiconductor substrate 2 is indicated by a curve 32 in FIGS. 3 and 4.
Using ion implantation, n.sup.+ conducting zones are introduced into the epitaxially deposited layer 3 into those zones which are later covered by the collectors. The ions are implanted for example with 100 keV. As a result of a post-diffusion, the implanted ions penetrate deeper into the epitaxially deposited layer 3, so that the zones 4 which they form assume the course shown in broken lines in FIG. 2. FIG. 4 shows in broken lines the doping course of the implanted ions following the implantation in the form of a broken line curve 41.
Then, in a known manner, the base is doped with boron by diffusion or ion implantation, so that a p-conductive zone 5 with the emitter-base junction is formed at the penetration depth x.sub.EB (see FIGS. 3 and 4). At the same time the p-conducting zone 5 is being formed, the injector zone 7 may be conveniently formed. If desired, the p-conducting zone 7 may be formed as the injector by diffusion in the n-conducting layer 3. Finally, in the zone 5, an n.sup.+ conducting zone 6 is produced as collector with the base-collector junction at the penetration depth x.sub.BC (see FIGS. 3 and 4) by means of diffusion or implantation. The zone 6 has a penetration depth of approximately 1 .mu.m. The doping course of the zone 5 and of the zone 6 is referenced 35 and 36, respectively in FIGS. 3 and 4.
During the base doping, a possible post-diffusion and the doping of the collector, the doping which has been introduced by means of ion implantation (see Curve 41 in FIG. 4) diffuses out, so that after these temperature treatments a doping course is formed as illustrated by the curve 42 in FIG. 4.
FIG. 3 shows the doping course in a section III--III of FIG. 2 without the zone 4, and FIG. 4 shows the doping course in a section IV--IV with the zone 4. Beneath the collector 6, thus at the point of the actual, inversely operated transistor, the epitaxial layer 3 has a higher doping which produces a good emitter efficiency and thus a good upwards current amplification.
It will be apparent to those skilled in the art that many modifications and variations may be effected without departing from the spirit and scope of the novel concepts of the present invention.