Conductivity-modulation metal oxide semiconductor field effect transistor

Abstract: A conductivity-modulation MOSFET employs a substrate (30) of an N type conductivity as its N base. A first source layer (34) of a heavily-doped N type conductivity is formed in a P base layer (32) formed in the N base (30). A source electrode (38) electrically conducts the P base (32) and the source (34). A first gate electrode (36) insulatively covers a channel region (CH1) defined by the N⁺ source layer (34) in the P base (32). A P drain layer (44) is formed on an opposite substrate surface. An N⁺ second source layer (46) is formed in a P type drain layer (44) by diffusion to define a second channel region (CH2). A second gate electrode (40) insulatively covers the second channel region (CH2), thus providing a voltage-controlled turn-off controlling transistor. A drain electrode (48) of the MOSFET conducts the P type drain (44) and second source (46). When the turn-off controlling transistor is rendered conductive to turn off the MOSFET a "shorted anode structure" is temporarily formed wherein the N type base (30) is short-circuited to the drain electrode (48), whereby case, the flow of carriers accumulated in the N type base (30) into the drain electrode is facilitated to accelerate dispersion of carriers upon turn-off of the transistor.

Description: The present invention relates to metal insulator semiconductor field effect transistors and, more particularly, to an improvement of a conductivity-modulation MOSFET. A conductivity-modulation MOSFET has a semiconductive drain layer, an N type conductivity base layer (N base layer) formed on a buffer layer, and a base layer (P base layer) of P type conductivity. The P base layer is formed by diffusion in an N type semiconductive layer serving as the N base layer. A heavily-doped N type layer (N + layer) is formed on the P base layer to define a channel region of the MOSFET. A gate electrode layer insulatively covers the N base layer and the channel region, and a source electrode layer electrically shorts the P base layer and the N + source layer. When a positive voltage is applied to the gate electrode, the channel region is inverted, so that carriers (electrons) are injected from the N + source layer into the N base layer. When the electrons enter the drain layer through the buffer layer, the PN junction of the MOSFET is forward-biased, and as a result, the MOSFET is turned on. When a zero or negative voltage is applied to the gate electrode, the inverted layer in the channel region disappears, and hence, the channel disappears. As a result, the MOSFET is turned off. EP-A-0 111 804 discloses a known bidirectional insulated-gate rectifier. An insulated-gate bipolar transistor (IGBT) having an anode short-circuit which is dependent on carrier-flow is described in IBEM 1986, December 1986, pp 218-221 (Gough et al). A MOS-Darlington IGBT/thyristor device which employs a buffer layer for protecting against punch-through is described in EP-A-0 118 336. In order to improve a turn-off switching speed of such a conductivity-modulation MOSFET, carriers accumulated in the N base layer thereof must disappear faster. However, with a conventional conductivity-modulation MOSFET, if the carrier lifetime in the N base layer is shortened in order to improve the turn-off speed, a voltage in the device becomes undesirably high, which leads to the difficulty in turn-on drive of the MOSFET. It is therefore an object of the present invention to provide an improved conductivity-modulation metal insulator semiconductor field effect transistor. It is another object of the present invention to provide a new and improved conductivity-modulation metal insulator semiconductor field effect transistor which can increase a turn-off switching speed while a turn-on voltage thereof is kept lowered. In accordance with the above objects, claim 1 of the present invention now provides a semiconductor device characterised by comprising: a semiconductor substrate (100, 230) of p type conductivity having a main surface; and a conductivity-modulation field effect transistor formed on said main surface of said substrate, said transistor having a first base region (84) of p type conductivity formed on one portion of said main surface of said substrate, a source region (88) of n type conductivity formed in a surface of said first base region (84), a source electrode (92) formed on said first base region and said source region for electrically connecting the same with each other, a drain region (86) of p type conductivity formed on another portion of said main surface of said substrate (100, 230), a drain electrode (94) formed on said drain region (86), a first semiconductor region (104, 236) of n type conductivity formed to entirely surround said drain region (86) except for an upper surface thereof, a second base region (106, 80) of n type conductivity formed on said main surface of said substrate (100, 230) including a region between said first base region (84) and said first semiconductor region (104, 236) an impurity concentration of said second base region being lower than that of said first semiconductor region, a first gate electrode (96) insulatively provided above said substrate on a first channel region formed between said source (88) and said second base region (106, 80) and a second semiconductor region (90), of n type conductivity, which is formed in said surface of said drain region (86), said semiconductor layer (90) being in contact with said drain electrode (94) and having an impurity concentration higher than that of said first semiconductor region. The present invention and its objects and advantages will become more apparent from the detailed description of a preferred embodiment presented below. In the detailed description of a preferred embodiment of the invention presented below, reference is made to the accompanying drawings. It is pointed out that figures 2, 5, 11, 15 and 18 below, together with the corresponding text, are examples which are useful for understanding the invention but do not form part of the present invention. Fig. 1 is a diagram showing a sectional structure of a main part of a conventional conductivity-modulation MOSFET; Fig. 2 is a diagram showing a sectional structure of a main part of a conductivity-modulation MOSFET having a vertical double-gate structure; Fig. 3 is a graph showing changes in drain voltage and drain current upon turn-off of the MOSFET; Fig. 4 is a graph showing measurement results a change over time in electron density distribution with respect to various drain voltage applications upon turn-off of the MOSFET, wherein "Y" plotted along the abscissa represents a distance from the centre of a turn-on controlling gate electrode; Fig. 5 is a diagram showing a sectional structure of a main part of a conductivity-modulation MOSFET having a horizontal double-gate structure; Fig. 6 is a diagram showing a sectional structure of a main part of a conductivity modulation MOSFET having a horizontal double-gate structure according to an embodiment of the present invention; Fig. 7 is a diagram showing a plan view of a main part of a conductivity-modulation MOSFET having a horizontal double-gate structure; Fig. 8 is a diagram showing a sectional structure taken along a line XV - XV of the device shown in Fig. 7; Figs. 9 to 12 are diagrams showing sectional structures of main parts of conductivity-modulation MOSFETs having horizontal double-gate structures; Figs. 13 to 15 are diagrams showing sectional structures of main parts of conductivity-modulation MOSFETs having horizontal single-gate structures; Fig. 16 is a diagram showing a two-dimensional structure of a main part of another conductivity-modulation MOSFET; Figs. 17 and 18 are diagrams showing sectional structures taken along different cutting lines of the device shown in Fig. 15; Fig. 19 is a diagram showing a two-dimensional structure of a main part of another conductivity-modulation MOSFET; Figs. 20 and 21 are diagrams taken along different cutting lines of the device shown in Fig. 19; Fig. 22 is a diagram showing a sectional structure of a main part of still another conductivity-modulation MOSFET; Fig. 23 is a diagram showing a two-dimensional structure of a main part of still another conductivity-modulation MOSFET; Figs. 24 and 25 are diagrams showing sectional structures taken along different cutting lines of the device shown in Fig. 23; Fig. 26 is a diagram showing a two-dimensional structure of a main part of another conductivity-modulation MOSFET; and Figs. 27 and 28 are diagrams taken along different cutting lines of the device shown in Fig. 20. Prior to description of the embodiment of the present invention, a conductivity-modulation MOSFET (also called a "bipolar mode MOSFET") having a conventional vertical structure will be described with reference to Fig. 1, for the sake of easy understanding of the present invention. In Fig. 1, heavily-doped P type conductivity (P + type) semiconductor layer 10 serves as a drain layer. N type buffer layer 12 and N - type base layer 14 are formed on drain layer 10. P type base layer 16 is formed in N - base layer 14 by diffusion. N + type layer 18 serving as a source of the MOSFET is formed in P base layer 16, and defines, as channel region CH of the FET, a portion of P base layer 16 located between itself and N base layer 14 . Gate electrode layer 20 insulatively covers N - base layer 14 and channel CH. Source electrode layer 22 is disposed on layer 14 so as to electrically short between P base layer 16 and N + source layer 18. Drain electrode layer 24 is disposed on an opposite surface of P + drain 10. When gate electrode 20 is positively biased with respect to source electrode 22, the MOSFET is turned on. The physical mechanism of the MOSFET is as follows. When gate electrode 20 is applied with a positive voltage, channel region CH is inverted and electrons are injected from source 18 into N - base 14 through channel CH. When these electrons enter P + drain 10 through N buffer layer 12, the PN junction of the MOSFET is forward-biased. In this case, holes are injected from P + drain 10 to N base 14 through N buffer 12. Therefore, both the electrons and holes are stored or accumulated in N - base 14, thus inducing conductivity modulation. Even when the resistance of N - base 14 is set to be relatively high in order to obtain high withstand voltage characteristics, the resistance of N - base 14 is decreased upon turn-on of the MOSFET due to the conductivity modulation, so that a turn-on voltage is decreased. When gate electrode 20 is biased to zero or negative with respect to source electrode 22, the inverted layer formed in channel region CH disappears, and the MOSFET is turned off. According to the conventional conductivity-modulation MOSFET, in order to increase a turn-off speed, carriers accumulated in N - base 14 must be disappeared as fast as possible. Unless electrons accumulated in N - base 14 are rapidly moved into drain 10, a PNP transistor constituted by P + drain 10, N buffer 12, N - base 14, and P base 16 is operated, and a large tail current flows through the MOSFET. In order to achieve rapid disappearance of accumulated carriers in N - base 14, a carrier lifetime can be decreased. However, in this case, a voltage (turn-on voltage) necessary for turning on the MOSFET is undesirably increased to cause its turn-on characteristics to be degraded. In the conventional MOSFET, improvement of the turn-off speed (switching-off speed) and a decrease in turn-on voltage cannot be simultaneously realized. The aforementioned conflicting problems in the conventional conductivity-modulation MOSFET can be effectively eliminated by a conductivity-modulation MOSFET presented below. Referring to Fig. 2, a vertical conductivity-modulation MOSFET having a double-gate structure has a characteristic feature in that it has second gate electrode G2 as a turn-off controlling electrode. More specifically, P base layer 32 and N + type source layer 34 are formed in N - diffusion layer 30 in the same manner as in the prior art shown in Fig. 30. N + source layer 34 defines, as first channel region CH1, a portion of P base 32 located between itself and N - base 30. Polysilicon layer 36 serving as first gate electrode G1 is insulatively provided above N - base layer 30 to be self-aligned with N + source 34. Metal layer 38 serving as a source electrode electrically shorts P base layer 32 and N + souce layer 34. N buffer layer 42 comprises N layers 42a and 42b (if N buffer layer 42 is separately formed as layers 42a and 42b, as illustrated in Fig. 2, this structure allows effective threshold value control of channel CH2). Polysilicon layer 40 serving as a second gate electrode is insulatively provided above one surface of N buffer layer 42. The other surface of N buffer layer 42 is connected to N - base layer 30. N buffer layer 42 serves to prevent generation of a punch-through phenomenon, and to increase a MOSFET withstand voltage. P type drain layer 44 is formed in N buffer layer 42. N + type source diffusion layer 46 is formed in P type drain layer 44 by diffusion. N + layer 46 defines, as second channel region CH2, a portion of P drain layer 44 located between itself and N buffer 42. Metal layer 48 serving as a drain electrode electrically shorts between layers 44 and 46. As shown in Fig. 2, N + layer 46, P drain 44, and N buffer 42 are formed by diffusion to be self-aligned with an end portion of second gate electrode 40. In the following description, first gate electrode G1 is referred to as a "turn-on controlling gate electrode" or simply as an "ON gate" of the MOSFET hereinafter, and second gate electrode G2 is referred to as a "turn-off controlling gate electrode" or simply as an "OFF gate" hereinafter. The conductivity-modulation MOSFET is turned on, when turn-on controlling gate electrode G1 is positively biased with respect to source electrode S, and turn-off controlling gate electrode G2 is biased to a zero or negative potential with respect to drain electrode D. The physical mechanism associated with the turn-on of the MOSFET is substantially the same as that in the prior art shown in Fig. 1. More specifically, in a turn-on mode of the MOSFET, OFF gate G2 is biased to a zero or negative potential. Therefore, second channel region CH2 is kept nonconductive. N - buffer 30 is disconnected from drain electrode D in the same manner as in N buffer 12 shown in Fig. 1. In this state, when ON gate G1 is positively biased, first channel region CH1 is inverted, and as a result, electrons are injected from N + source 34 into N - base 30. When these electrons migrate toward the drain layer through N buffer 30, holes are injected from P drain diffusion layer 44 into N - base 30 through N buffer 42. The MOSFET is thus turned on. The turn-on operation is the same as that of the conventional MOSFET shown in Fig. 1, and conductivity modulation is performed in N base layer 30. When the MOSFET is to be turned off, turn-on controlling gate electrode G1 is biased to a zero or negative potential with respect to source electrode S, and turn-off controlling gate electrode G2 is positively biased with respect to drain electrode D. Thus, channel region CH1 is rendered nonconductive, and channel region CH2 is inverted and rendered conductive. Since channel region CH1 is rendered nonconductive, injection of electrons from N + source 34 into N base 30 is inhibited. On the other hand, since channel region CH2 is rendered conductive, N + source 46 is electrically conducted to N buffer 42, so that drain electrode D shorts between N buffer 42 and P drain 44, thereby temporarily forming a "shorted anode structure". In this case, a current gain of the PNP transistor becomes zero. Electrons accumulated in the device are rapidly discharged through N buffer 42, channel CH2, and N + source 46. Holes migrate into source electrode layer 38 through P base 32. This state is substantially equivalent to a state wherein P and N bases 32 and 30 are reverse-biased. With this conductivity-modulation MOSFET, gate G2 is activated to invert channel CH2, and N buffer layer 30 is electrically shorted with electrode layer 10 constituting drain electrode D, thereby providing the "shorted anode structure". Therefore, the turn-off speed of the MOSFET can be increased. In this case, unlike in the conventional MOSFET, since the carrier lifetime need not be shortened, the current gain of the PNP transistor in the turn-on state of the MOSFET can be increased. As a result, even if the thickness of N base diffusion layer 30 is increased, its forward voltage drop can be kept small, and the turn-on voltage of the MOSFET can be maintained low. Therefore, the conflicting problems which the conventional conductivity-modulation MOSFET suffers can be simultaneously solved. The device structure in the turn-off mode is equivalent to a diode constituted by P and N bases 16 and 14. This means that the MOSFET has a reverse-conducting diode therein (N buffer 42 serves as an N emitter to decrease a forward voltage drop of the reverse-conducting diode). When the diode is reverse-biased, a current flows through a path constituted by source electrode 38, P base 32, N base 30, N buffer 42, channel CH2, N + source 46, and drain electrode layer 48. The presence of the diode is particularly effective when applied to a high-voltage MOSFET which deals with 2,000 volts or higher. It is important that the "shorted anode structure" is temporarily formed in the device only when it is driven to be turned off. When the N buffer layer 42 is electrically shorted with drain electrode D, carriers (electrons, in this case) accumulated in N - base 30 in a turn-off mode can be rapidly disappeared, since the current gain of the above-mentioned PNP transistor is reduced to zero and hence the tail current components of the turn-off current can be very small. However, if the "shorted anode structure" is always formed in the MOSFET throughout turn-on/off control, turn-on characteristics may be impaired. If N buffer 42 is electrically shorted with drain electrode D in the turn-on mode, injection of holes from P drain 44 into N buffer 42 is suppressed, and the effect of conductivity modulation cannot be sufficiently obtained, thus undesirably increasing the turn-on voltage. In consideration of the above problem, according to the present invention, second gate electrode G2 is provided as the OFF gate, and during turn-on control of the MOSFET, N buffer 42 is forcibly disconnected from drain electrode D, thereby disappearing the "shorted anode structure". It should be noted that applications of a turn-on/off controlling voltage to gates G1 and G2 can be delayed from one another so that OFF gate G2 is turned on faster than ON gate G1. Preferably, a few microseconds before a voltage application to ON gate G1, more preferably, 1 µs or more before a voltage application to ON gate G1, OFF gate G2 is applied with a positive voltage. An application of a positive voltage for turn-off control allows a further increase in the turn-off speed of the conductivity-modulation MOSFET. The reason therefor is as follows. A few microseconds before a bias voltage to gate G1 is decreased, if gate G2 is positively biased, N channel CH2 is shunt before the MOSFET is turned off. Therefore, excess carriers inside the MOSFET device can be effectively removed, thus shortening a turn-off time (to be referred to as a "fall-time" hereinafter). Fig. 3 is a graph showing a calculated inductive turn-off waveform of the aforementioned conductivity-modulation MOSFET device. 0.8 µs and 0.65 µs fall-time could be obtained by adjusting the timing for causing N-channel anode short. As shown in Fig. 3, turn-off controlling gate G2 was positively biased approximately 2 µs before turning off the device or reducing the turn-on controlling gate G1 bias. By creating the N-channel shunt, a few microseconds before turning off the device, the excess carriers inside the device were effectively removed, thus realizing a short fall-time. Fig. 4 shows the electron density distribution change corresponding to Fig. 3. It is clearly seen from Fig. 4 that the excess carriers in the drain side are removed from 0 µs to 1.98 µs through the n-channel shunt. Fall-time can be further reduced by applying a positive bias voltage to gate G2 3 µs before the device is turned off as seen in Fig. 4. P source diffusion layer 44 are symmetrically formed on the opposing surfaces of N base layer 50. Similarly, N + source layers 34 and 46 are symmetrically formed, thus defining symmetrical channels CH1 and CH2. With this multilayered structure, since no N buffer layer is formed, mobility of electrons and holes inside the device can be improved due to the symmetrical element structure although the withstand voltage of the MOSFET is slightly degraded. The symmetrical device structure is also advantageous in mass production. According to the device shown in Fig. 6, deep P + diffusion layer 52 is additionally formed in P drain layer 44 located beneath drain electrode layer 48. P + layer 52 is deeper than P drain 44. As shown in Fig. 6, P + layer 52 overlaps N + layer 46. Addition of P + layer 52 improves injection efficiency of holes on the drain side of the MOSFET. Fig. 7 is a perspective view of a MOSFET having a double-gate structure, wherein an upper source electrode pattern is shifted from a lower drain electrode pattern through 90 degrees. ON-gate electrode layers (these are designated by identical numerals "36" in Fig. 7) and source electrode layers (these are denoted by identical numerals "38" in Fig. 7) are alternately arranged on the the upper surface of a wafer, i.e., the top surface of N base 30, and slit-like elongated parallel grooves are defined between these layers 36 and 38. These layers 36 and 38 extend along one direction. P base layers 32 and N + source layers 34 are elongated along the extending direction of layers 36 and 38. It is to be noted that layers 36 or 40 are covered by an insulative layer such as an SiO 2 film, and layers 38 or 48 are formed on the entire surface of the insulative layer, in practice. OFF-gate electrode layers (these are designated by identical numerals "40" in Fig. 7) and drain electrode layers (these are denoted by identical numerals "48" in Fig. 7) are alternately arranged on the rear surface of the wafer, i.e., on the surface of N buffer 42, slit-like parallel elongated grooves are defined between these layers 36 and 38. These layers 40 and 48 extend in a direction shifted from the extending direction of layers 36 and 38 by 90 degrees. P drain layers 44 and N + diffusion layers 46 formed therebelow are elongated along the extending direction of layers 40 and 48. If such an electrode pattern is adopted, local concentration of a turn-on current inside the wafer is moderated, and a current distribution can be made uniform. In Fig. 8, upper source electrode pattern extends in the same direction as that of a lower drain electrode pattern and is shifted therefrom by half an interval (pitch). Therefore, source electrodes 38 and drain electrodes 48 are inhibited from directly opposing each other, and ON-gate electrodes 36 and OFF-gate electrodes 40 are also inhibited from directly opposing each other. More specifically, as shown in Fig. 6, ON-gate electrode layer 36 faces drain electrode layer 48, and OFF-gate electrode layer 40 faces source electrode layer 38. When such an arrangement of electrode layers is employed, holes can be rapidly injected from P drain 44 into a region of N base layer 30 to which electrons are supplied from N + source 34, thus allowing efficient conductivity modulation. In Fig. 9, electrode layers are fabricated so that the relation among width Lg1 of ON-gate electrode layer 36, source width Ls, width Lg2 of OFF-gate electrode layer 40, and drain width Ld satisfies the following inequality: (Ls + Lg1) < (Lg2 + Lg) In Fig. 10, electrode layers are fabricated so that the relation among width Lg1 of ON-gate electrode layer 36, source width Ls, width Lg2 of OFF-gate electrode layer 40, and drain width Ld satisfies the following inequality: (Ls + Lg1) > (Lg2 + Lg) When the patterns of the electrode layers are set as described above, injection efficiency of holes can be improved. Fig. 12 is a cross-sectional view of a main part of a conductivity-modulation MOSFET having a horizontal double-gate structure. Unlike in the MOSFET device structures shown in Fig. 2 and Figs. 5 to 11 wherein the source and drain are formed on opposite surfaces, the source and drain of the MOSFET are formed on a single surface of N - base layer 80, according to this example. Lightly-doped N type (N - type) silicon wafer 80 is used as an N - base layer of the MOSFET. Heavily-doped N type (N + type) buffer layer 82 is formed on one surface of silicon wafer 80. Electrode layer 83 is formed on buffer layer 82. P type diffusion layers 84 and 86 are formed on the other surface (front surface) of silicon wafer 80. P type diffusion layers 84 and 86, serve as P base and P drain layers respectively. N + type layers 88 and 90 are respectively formed in P base and P drain layers 84 and 86 to define channel regions CH1 and CH2. Source electrode layer 92 is deposited on wafer 80 to render layers 84 and 88 electrically conductive to each other. Drain electrode layer 94 is deposited on wafer 80 to render layers 86 and 90 electrically conductive to each other. First gate electrode layer 96 serving as an ON-gate insulatively covers channel CH1, and constitutes a turn-on controlling transistor of the MOSFET. According to the conductivity-modulation MOSFET having the horizontal double-gate structure described above, since all the necessary layer patterns are formed on one surface of wafer 80 in addition to the aforementioned technical advantages, mounting of the device in a package (not shown) can be facilitated. In addition, internal connection wiring with terminal pins of the package can also be facilitated. According to the embodiment shown in Fig. 6, P - type silicon wafer 100 is used in place of N - type silicon wafer 80 in the example shown in Fig. 5. Heavily-doped (P + type) third semiconductor region 102 is formed on one surface of p - type silicon wafer 100. Since P - type silicon wafer 100 is used, N type diffusion layer (semiconductor region) 104 is necessary for electrically insulating P type diffusion layer 86 from wafer 100. Layer 104 can be formed in a self-aligned manner with layers 90 and 86, and serves as an N buffer, which acts as an N emitter to decrease a voltage drop generated when the device operates as a reverse conducting diode. Lightly-doped N type (N - type) diffusion layer 106 is formed shallow in the surface portion of wafer 100, and can be connected to layer 104. Shallow N - type diffusion layer 106 serves as an N base layer to which electrons are injected from first N + source diffusion layer 88. It was experimentally demonstrated by the present inventors that when shallow diffusion layer 106 had an impurity dose of about 5 × 10 11 to 4 × 10 12 /cm 2 , the withstanding voltage of the transistor structure was maximized, and a sufficiently low turn-on resistance could be obtained. According to the embodiment described above, when the source and drain of the conductivity-modulation MOSFET are formed on one surface side of a substrate, careful attention should be directed to the following two points. First, in the turn-off mode of the MOSFET, a two-dimensional pattern of the source and drain of the MOSFET should be carefully designed such that a depletion layer in a junction portion at which a reverse bias voltage is applied is uniformly expanded, and a deviated internal electric field distribution is minimized in that portion. Second, when one MOSFET is cut from a large number of MOSFETs formed on a wafer, or when element isolation is made between the MOSFETs using dielectric layers, the two-dimensional pattern of the source and drain of the MOSFET should be carefully designed so that necessity of addition of a special passivation to each element boundary portion is eliminated. Embodiments of two-dimensional patterns of conductivity-modulation MOSFETs having horizontal double-gate structure which can fully meet the requirements on device design will be presented and explained below. In Figs. 7 and 8, second semiconductor region 104 is formed on a front surface portion of wafer 100 to define island layers. In the plan view of Fig. 7, one island drain isolation diffusion layer 105 is indicated by broken line. P drain diffusion layer 86 is formed in each drain isolation diffusion layer 104 (see Fig. 8). Second N + type source layer 90 is formed in layer 86 to have an elliptical ring shape. Heavily-doped diffusion layer 110 of P type conductivity is formed deep in the central region of each P drain diffusion layer 86. Shallow N - diffusion layer 106 two-dimensionally surrounds island drain isolation diffusion layer 105. N - diffusion layer 106 is connected to each island drain isolation diffusion layer 104, as shown in Fig. 8. Drain electrode 94 is directly formed on the surface of wafer 100 to overlap p + type layer 110. Drain electrode 94 has an elliptical shape, as clearly illustrated in Fig. 7. OFF-gate electrode layer 98 is insulatively formed above wafer 100 to surround drain electrode 94. OFF-gate electrode layer 98 has an elliptical ring shape. ON-gate electrode layer 96 is insulatively formed above wafer 100 to surround OFF-gate electrode layer 98 and to have an elliptical ring shape. Conductive layer 92 serving as source electrode S two-dimensionally surrounds ON-gate electrode layers 96 formed on wafer 100 in the manner as described above, as shown in Fig. 7. P base layer 84 formed on the surface of wafer 100 two-dimensionally surrounds island diffusion layers 105 each of which includes drain layer 86 (see Fig. 7). Electrode layer 83 formed on the rear surface of the wafer 100 is, e.g. grounded. According to the above-mentioned two-dimensional pattern, P base layer 84 is designed to surround island drain regions 86. Therefore, when one MOSFET element is isolated from wafer 100, or when one element is electrically insulated from other elements formed on single wafer 100, an element boundary is formed in each P base layer 84, thus facilitating setting of passivation in each P base layer 84. Further, a junction portion which is reverse-biased in the turn-off mode of the MOSFET is formed between P - wafer 100 and a diffusion layer portion comprising N type drain isolation diffusion layer 104 surrounding P drain 86 and shallow N - layer 106 provided around layer 104. When the junction portion is reverse-biased, a depletion layer radially expands outwardly from the elliptical diffusion layer portion in wafer 100, so that local concentration of an electric field in wafer 100 can be satisfactorily suppressed. Therefore, operation reliability of the MOSFET can be improved. central flat region of corresponding island P base layer 84, and has an elliptical shape (see Fig. 16). Electrode layer 96 serving as ON gate G1 is formed on wafer 80 to surround each source electrode layer 92. Electrode layer 98 serving as OFF gate G2 surrounds ON-gate electrode layer 96. More specifically, drain electrode layer 94 is continuously formed on wafer 80 to surround OFF-gate electrode layers 98. Electrode layer 83 formed on the rear surface of wafer 80 is set at a drain potential. When the element is turned off, a depletion layer expands in wafer 80 on the side of the source region. Therefore, expansion of the depletion layer can be uniformed, and local concentration of an internal electric field can be suppressed, in the same manner as in the device shown in Figs. 14 and 15. Furthermore, since the two-dimensional pattern is employed, special passivation at boundaries of elements formed on wafer 80 can be facilitated or omitted. In Figs. 18 and 19, both source and drain regions alternately arranged on wafer 80 are formed to have an elliptical shape, as shown in Fig. 18. Each source electrode layer 92 is formed on wafer 80 to be located on the central flat region of corresponding island P base layer 84 and to have an elliptical shape (see Fig. 16). ON-gate electrode layer 96 surrounds source electrode layer 92. Each drain electrode layer 94 is formed on wafer 80, located on the central flat region of corresponding island P drain diffusion layer 86, and has an elliptical shape (see Fig. 16). OFF-gate electrode layer 98 surrounds drain electrode layer 94. N + diffusion layer 114 is continuously formed on the surface portion of wafer 80 to surround the source and drain regions. A drain potential is applied to N type wafer 80 through P drain 86 and P + layer 110 which are forward-biased. Therefore, continuous N + diffusion layer 114 is formed so that a necessary potential can be applied to the junction portion of each island P base layer 84 without a drain electrode porvided on one entire surface of wafer 80 in the embodiment shown in Figs. 16 and 18. With this structure, the effects of facilitating element isolation can also provided. Fig. 32 is a cross-sectional view of a main part of a conductivity-modulation MOSFET having a horizontal double-gate structure. According to this device, the source and drain of the MOSFET are formed on the front surface of P - type wafer substrate 200 and adjacent to each other. Wafer 200 is used as a P base layer of the MOSFET. P + type layer 202 is formed on the rear surface portion of wafer 200. Electrode layer 203 is formed on layer 202. P type diffusion layers 204 and 206 are formed on the front surface of silicon wafer 200. P type diffusion layers 204 and 206 respectively serve as P base and P drain layers. Layer 204 consists of P type diffusion layer 204a and relatively deep P + type diffusion layer 204b. N + type diffusion layer 208 is formed in P base diffusion layer 204. Layer 208 defines channel region CH1 in layer 204a. N + type diffusion layer 210 is formed in P drain layer 206, and defines channel region CH2 in layer 206. Source electrode layer 212 is deposited on wafer 200 to render layers 204b and 208 electrically conductive to each other, and drain electrode layer 214 is deposited on wafer 200 to render layers 206 and 210 electrically conductive to each other. First gate electrode layer 216 serving as an ON-gate insulatively covers channel CH1 and constitutes a turn-on controlling transistor of the MOSFET. Second gate electrode layer 218 serving as an OFF-gate insulatively covers channel CH2 and constitutes a turn-off controlling transistor of the MOSFET. It is to be noted that N type diffusion layer 220 is formed on the front surface portion of wafer 200 to include P drain layer 206 therein. N - type diffusion layer 220 serves as an N buffer. N type diffusion layer 222 which is connected to buffer 220 and extends immediately below gate G1 is formed on the front surface portion of wafer 200. Layer 222 serves as an N base. Furthermore, N type impurity ions are implanted in channel region CH2 which is defined on the surface portion of wafer 200 so as to be located below second gate electrode 218 which serves as OFF gate G2, as clearly illustrated in Fig. 22. In other words, N + drain 210 is conducted to N - type isolation layer 220 through N - type diffusion section (to be referred to as an "N bypass layer" hereinafter) 224 of channel region CH2. Since the impurity dose of the N - type diffusion section is relatively very low (e.g., about 1 x 10 11 to 1 x 10 13 /cm 2 ), a conductance between N + drain 210 and N - type isolation layer 220 is relatively low, and a lateral resistance therebetween is relatively high. In this sense, N + drain 210 is half-conducted to N base 220 through N bypass layer 224 of channel region CH2. Alternatively, a turn-off controlling switch section having OFF gate G2 is normally rendered half-conductive. The turn-off controlling switch section having OFF gate G2 which is rendered conductive in the turn-off mode of the conductivity-modulation MOSFET is rendered half-conductive in other operation modes. For example, when a positive voltage is applied to source electrode 212 in in order to turn on the MOSFET, electrons are injected from N + source 208 into N base 222. These electrons flow into N + layer 210 through N bypass layer 224. In this case, a potential difference is generated by the lateral resistance of N bypass layer 224. The lateral potential difference forward-biases the PN junction portion between P drain 206 and N buffer 220. Upon forward-biasing, holes are injected from P drain 206 into N base 222. N base 222 is thus subjected to conductivity modulation, and the MOSFET can be turned on at a relatively low turn-on controlling voltage. When a zero or negative voltage is applied to ON gate G1, and OFF gate G2 is positively biased so as to turn off the MOSFET, injection of electrons from the source is interrupted. Electrons accumulated in N base 222 are discharged into N + layer 210 through N bypass layer 224. Holes accumulated in N base 222 are discharged into source electrode 212 through P base 204. N bypass layer 224 for half-conducting N + drain 210 and N base 220 is provided to channel region CH2. The potential difference for forward-biasing the PN junction portion of P drain 206 in the turn-on mode of the MOSFET is generated in N bypass layer 224. The lateral resistance of N bypass layer 224 can be desirably increased by controlling the concentration of impurities injected into channel region CH2. Therefore, even if the impurity concentration of N buffer 220 is increased to relatively high, a desired high withstand voltage of the element can be maintained. This contributes to realization of a conductivity-modulation MOSFET having good turn-off characteristics (capable of high-speed turn-off switching) and a high withstand voltage. In Fig. 10, formation position of drain electrode 214 and OFF gate electrode 218 on wafer 200 are reversed to those in the embodiment shown in Fig. 22. More specifically, gate electrode 218 of a turn-off controlling switch section is formed outside N + layer 210 and separated from N base 222. Therefore, channel region CH2, which is located below electrode layer 218 serving as OFF gate G2 and in which N bypass layer 224 is formed, is also defined outside N + layer 210, as shown in Fig. 23. With this structure, the same effects as described above can be provided. In the device shown in Fig. 5, the impurity concentration of channel region CH2 defined in P drain layer 86 cannot exceed 5 × 10 16 to 1 × 10 17 /cm 3 in consideration of threshold voltage level Vth of the turn-off controlling switch section. In this case, effective conductivity modulation of the MOSFET cannot always be performed, since it cannot be expected that holes are effectively injected from P drain 86. Modifications suitable for a case wherein injection efficiency of holes from the P drain layer must be improved in the conductivity-modulation MOSFET having the horizontal double-gate structure will be presented below. According to a modification shown in Fig. 11, P - type diffusion layer 230 and P + type diffusion layer 232 are formed on the rear surface portion of N type wafer 80. Second N + diffusion layer 90 and shallow P + type diffusion layer 234 are formed in P drain layer 86 formed on the front surface portion of N type wafer 80. P + layer 234 overlaps N + diffusion layer 90 and is adjacent to channel region CH2, as illustrated in Fig. 11. Deep N type diffusion layer 236 is formed in wafer 80 to surround P drain layer 86. Shallow P + type diffusion layer 234 is additionally formed in P drain layer 86, the injection efficiency of holes from the P drain can be effectively improved without increasing the impurity concentration of channel region CH2. According to a modification shown in Fig. 12, in order to improve the injection efficiency of holes from P drain 86, electrode layer 98 serving as OFF gate G2 is insulatively provided above p - type wafer 100 so as to be distant from the source region of the device. Shallow P + type diffusion layer 240 is formed in P drain layer 86 on the side of the source region. Drain electrode layer 242 is formed on wafer 100 to be in electrical contact with N + layer 90 and P + layer 240 in P drain layer 86, as shown in Fig. 12. During manufacture of the device with the above structure, N buffer layer 104, P drain 86, and N + layer 90 can be easily fabricated in wafer 100 by a triple diffusion technique using the edge portion of one end of OFF gate electrode layer 98 as one end of a window opening of a diffusion mask. High-speed turn off controlling technique in conductivity-modulation MOSFETs can also be realised in a shorted anode MOSFET having a single-gate structure. Such conductivity-modulation MOSFETs will be described below. A conductivity-modulation MOSFET shown in Fig. 13 is substantially the same multilayered structure as that shown in Fig. 9, except that turn-off controlling gate G2 is omitted from the MOSFET shown in Fig. 13. Thus, the same reference numerals in Fig. 13 denote the same portions as in Fig. 9, and a detailed description thereof will be omitted. With this structure, N buffer layer 220 is constantly half-connected to drain electrode layer 214 through channel region CH2 in both turn-on and turn-off modes of the conductivity-modulation MOSFET. When a positive voltage is applied to source electrode 212, electrons are injected from source layer 208 into N base 222. These electrons flow from N base 222 into N + layer 210 through N bypass layer 224. In this case, a potential difference occurs by the lateral resistance of the N bypass layer. The potential difference serves to forward-bias the PN junction between P drain 206 and N buffer 220. Thus, holes are injected from P drain 206 into N base 222, so that N base 222 is subjected to conductivity modulation, and the MOSFET is turned on. When the gate voltage is set to be zero or a negative voltage, injection of electrons from source 208 is interrupted. Electrons accumulated in N base 222 are discharged into N + layer 210 through N bypass layer 224, and holes accumulated in N base 222 are discharged into source electrode 212 through P base 204. Thus, the conductivity-modulation MOSFET is turned off. The potential difference for forward-biasing the PN junction occurs in N bypass layer 224, and the lateral resistance for causing the potential difference can be easily controlled by adjusting the impurity concentration of the N bypass layer. Therefore, even if the concentration of the N buffer is desirably increased, a withstanding voltage of the element can be increased without increasing the width of the N bypass layer. According to an element structure shown in Fig. 14, N bypass layer 224 is formed outside drain electrode 214. In this case, the same effects as described above can be obtained. According to a conductivity-modulation MOSFET shown in Fig. 15, dielectric element isolation film 250 is formed on supporting substrate 254, and buried isolation layer 252 is formed on film 250, as shown in Fig. 15. Although the invention has been described with reference to a specific embodiment, it shall be understood by those skilled in the art that numerous modifications may be made that are within the scope of the invention as defined by the appended claims. The device of Fig. 16 has the same basic structure as that shown in Fig. 6, wherein N drain layer 104 is formed in P - type silicon wafer 100, and P drain diffusion layer 86 and second N + source 90 are formed in layer 105. For the sake of easy visual understanding in Fig. 16, electrodes provided to respective portions are omitted, and only a diffusion layer pattern is visible. Fig. 17 shows a sectional structure taken along a line XXXI-XXXI in Fig. 16, and Fig. 18 shows a sectional structure taken along a line XXXII - XXXII in Fig. 16. In these figures, the same reference numerals denote the same portions as in Fig. 6 or 11 and a detailed description thereof will be omitted. As shown in Fig. 16, second N + source diffusion layer 90 in such a manner that it is divided into a plurality of layers by P type diffusion layers 300. P + layers 300 serve as part of a drain diffusion layer. In other words, second channel region CH2 below OFF controlling gate electrode 98 is divided into substantially channels CH2-1 (see Fig. 17) which contribute to a transistor operation, and sub-channels CH2-2 (see Fig. 18) which do not contribute to the transistor operation. These sub-channels CH2-1 and CH2-2 are alternately arranged when viewed from the top. Since second N + source diffusion layer 90 is divided as described above, injection efficiency of holes from P drain 86 when the MOSFET is rendered conductive can be improved, and hence, the ON voltage of the MOSFET can be decreased. It should be noted that high resistance layer 302 is insulatively provided above a substrate to connect first and second gate electrodes 96 and 98 to each other. When the MOSFET is turned off, a very small current flows through layer 302, and an electric field inside N - buffer layer 106 is moderated, thus preventing local concentration of an internal electric field. As illustrated on the right portion of Fig. 16, first N + source layer 88 is formed on a side opposite to channel region CH1 to have a three-dimensional pattern. Therefore, electrical contact characteristics of source electrode 92 with respect to first N + source layer 88 can be improved. In Figs. 19 to 21, second N + source diffusion layer 90 is integrally formed, and P + type layer 300 serving as a part of a drain diffusion layer has a three-dimensional pattern. More specifically, P + type layer 300 has recess portion 300a whose end portion is located inside N + source diffusion layer 90, and projection portion 300b whose end portion extends to channel region CH2 below second gate electrode 98, as shown in Fig. 20. These rectangular edge portions 300a and 300b are alternately arranged, as clearly illustrated in Fig. 19. With this structure, second channel region CH2 can be divided into sub-channels CH2-1 and CH2-2. Therefore, injection efficiency of holes from the P drain in the ON MOSFET can be improved, and a low ON voltage can be obtained. In Fig. 22, second N + source diffusion layer 90 is formed on an end portion (of P drain diffusion layer 86) farther from P base diffusion layer 84a in P drain diffusion layer 86. P + layer 300 is formed on an end portion of P drain diffusion layer 86 closer to P base diffusion layer 84a. With this structure, holes can be efficiently injected from P + layer 300 into N drain isolation diffusion layer 104 and N - buffer 106 when the MOSFET is turned on. In Figs. 23 to 25, high-resistance N diffusion layers 304 are formed in N drain isolation layer 104 to partially overlap P + type layers 300. These N type layers 304 are linearly arranged at equal intervals on an a portion opposite to channel region CH2, thus electrically shorting second N + source diffusion layer 90 to N drain isolation layer 104. With this structure, electrons are discharged through channel CH2, and are also discharged through high-resistance N diffusion layers 304 when the MOSFET is turned off. Therefore, the switching speed of the device can be increased. Since P + layers 300 are located on the side opposite to channel CH2 and closer to N - buffer layer 106, injection efficiency of holes from P drain 86 upon turn-on of the MOSFET can be improved, and hence, the turn-on voltage can be decreased. In Figs. 26 to 28, N + diffusion layer 306 is provided to electrically short together first end portions of high-resistance layers 304. N + diffusion layer 306 is formed in N drain isolation layer 104 and parallel to second N + source diffusion layer 90, as best illustrated in Fig. 40. High-resistance layers 304 for shorting second N + source diffusion layer 90 and N drain isolation layer 104 are connected to each other by N + diffusion layer 306, so that electrons can be uniformly discharged into drain electrode 94 when the MOSFET is turned off. Therefore, the switching speed of the element can be increased. Since N type layers 304 has a high resistance, passing of electrons through N type layers 304 can be suppressed. In this case, most electrons pass through P drain layer 86. Therefore, holes equivalent to passing electrons are injected, thus providing good conductivity-modulation action.

Claims: A semiconductor device characterised by comprising: a semiconductor substrate (100, 230) of p type conductivity having a main surface; and a conductivity-modulation field effect transistor formed on said main surface of said substrate, said transistor having a first base region (84) of p type conductivity formed on one portion of said main surface of said substrate, a source region (88) of n type conductivity formed in a surface of said first base region (84), a source electrode (92) formed on said first base region and said source region for electrically connecting the same with each other, a drain region (86) of p type conductivity formed on another portion of said main surface of said substrate (100, 230), a drain electrode (94) formed on said drain region (86), a first semiconductor region (104, 236) of n type conductivity formed to entirely surround said drain region (86) except for an upper surface thereof, a second base region (106, 80) of n type conductivity formed in said main surface of said substrate (100, 230) including a region between said first base region (84) and said first semiconductor region (104, 236), an impurity concentration of said second base region being lower than that of said first semiconductor region, a first gate electrode (96) insulatively provided above said substrate and located on a first channel region formed between said source (88) and said second base region (106, 80), and a second semiconductor region (90), of n type conductivity, which is formed in said surface of said drain region (86), said semiconductor layer (90) being in contact with said drain electrode (94) and having an impurity concentration higher than that of said first semiconductor region. The device according to claim 1, characterised by further comprising a second gate electrode (98) insulatively provided above said substrate and located on a second channel region formed between said second semiconductor region (90) and said first semiconductor region (104, 236). The device according to claim 1, characterised by further comprising a third semiconductor region (102, 232) of p-type conductivity formed on a back surface of said substrate (100, 230) which is a reverse side of said main surface an impurity concentration of said third semiconductor region being higher than that of said substrate. The device according to claim 3, characterised by further comprising a back electrode (83) formed on said third semiconductor region (102, 232). The device according to claim 1, characterised in that said second base layer (106, 80) has an n-type impurity dose of 5 x 10 11 to 4 x 10 12 /cm 2 .

Inventors: NAKAGAWA AKIO, WATANABE KIMINORI, YAMAGUCHI YOSHIHIRO, NAKAGAWA, AKIO, WATANABE, KIMINORI, YAMAGUCHI, YOSHIHIRO, NAKAGAWA, AKIO C/O PATENT DIVISION, WATANABE, KIMINORI C/O PATENT OFFICE, YAMAGUCHI, YOSHIHIRO C/O PATENT OFFICE
Applicants: TOSHIBA KK, KABUSHIKI KAISHA TOSHIBA
Application year: 1988
Main classification: H01L29
IPC codes: H01L29, H01L27