SEMICONDUCTOR LOGIC CIRCUITS

Abstract: A velocity saturated pull-up load for a compound semi­ conductor, e.g. gallium arsenide, logic element comprises a mesa 11 of active material supported on a substrate 12 and provided with a pair of closely spaced electrodes 13. The satu­ ration current corresponds to the mesa dimensions and the electrode spacing. A logic element provided with the velocity saturated load is also described.

Description: SEMICONDUCTOR LO-GIC CIRCUITS This invention relates to integrated circuits and to the fabrication of such circuits. The most commonly used semiconductor material is silicon. The technology of this material is well known and it can be used to fabricate a wide range of devices including integrated logic circuits. The speed of operation of such logic circuits is becoming an important factor as the complexity of the circuits increases. However this operating speed is limited ultimately by the carrier mobility in the semiconductor material. This mobility is of course an intrinsic property of the material itself. Attention is thus turning from silicon to those semiconductors having a higher carrier mobility. There are the compound semiconductors of which the best known example is gallium arsenide. Since the first GaAs high speed logic integrated circuit was introduced in 1974, a number of circuit approaches and device technologies have been reported with the aim to minimizing the speed power product to a level suitable for large scale integration. In recent years, enhancezent mode, normally-off MESFET logic has gained considerable attention due to its extremely low power consumpion, circuit simplicity and high speed. Enhancement mode normally-off logics reported to date utilise a linear resistance pull-up load in series with the switching FET in their basic inverter/gate design, although the linear characteristic of such a load involves certain limitations on switching characteristics. In a normally-off MESFET the thickness and the doping of the active region are tailored so that the built-in depletion of the Schottky barrier gate contact fully depletes the channel. The MESFET is switched on by the application of a positive voltage to the gate. The maximum voltage which can be applied is approximately 0.6 to 0.7V, and is limited by the forward conduction of gate diode. Since only positive voltage is required to switch the FET between the two logic states only a single rail supply is needed and the logic gates can be directly coupled which simplifies circuit design and mask layout. The low operating voltage is directly reflected in the low power consumption. According to one aspect of the present invention there is provided a field effect semiconductor logic element provided with a velocity saturated pull-up load. According to another aspect of the invention there is provided a gallium arsenide logic element having a non-linear pull-up load, characterised in that said load comprises a gallium arsenide mesa formed from active material on an undoped substrate and provided with a pair of closely spaced electrodes. We have found that velocity saturated pull-up loads can be fabricated in compound semiconductor materials and having dimensions sufficiently small that the saturation voltage is within the operating voltage range of an associated logic device. The velocity saturated pull-up load overcomes the disadvantage of the prior art resistive loads by providing a high speed switch that can operate at low power levels. The electrical characteristics of the device are determined by its dimensions and by the level to which the device is doped. Advantageously the pull-up load is formed by a photo-activated etching process. Said processes provide a high definition and accuracy thus ensuring a reproducibility of circuit parameters that has not hitherto been possible. Furthermore, the small physical size of the velocity pull-up load, as compared with prior art devices, makes it an ideal component for large scale integration. The device may be seen in the fabrication of fast logic integrated circuits for application e.g. in high speed data transmission systems. An embodiment of the invention will now be described with reference to the accompanying drawings in which: Figure 1 is a plan view of a logic circuit velocity saturated pull-up load; Figure 2 is a cross-section through the plane A-A of the load of Figure 1; Figure 3 is a schematic circuit diagram of a logic element provided with the load of Figures 1 or 2; Figure 4 shows a typical current/voltage characteristic of the pull-up load of Figures 1 and 2; and Figures 5 and 6 show typical switching characteristics of logic devices provided respectively with a conventional resistive pull-up load and the velocity saturated pull-up load of Figures 1 and 2. The following description relates to semiconductor fabrication techniques with pa#ticular reference to gallium arsenide. It will however be clear to those skilled in the art that the technique described herein can also be applied to other compound semsconductors. Referring now to Figures 1 and 2 the non-linear velocity saturated pull-up load comprises a substantially rectangular mesa 11 of semiconductor material disposed on a substrate 12 of either the same or an associated semiconductor material. Advantageously the mesa 11 is formed by a photo-activated anodic etching process such as is described in our co-pending UK application No. 8033486 (J.Mun-J.A.Phillips 4-1). Typically the mesa 0.5 to 1.5 microns in height comprises a layer of material doped to 0.5 to 1.0 x 1017/cc on an undoped buffer layer 3 microns thick. The active layer may be provided by a variety of techniques including doping, ion implantation and epitaxial growth. The mesa 11 is provided with closely spaced electrodes 13 which may be e.g. 1 micron apart. When a voltage is applied across these electrodes a current flows therebetween, this current being limited above a critical voltage dependent on the mesa dimensions and the electrode geometry. The current is in fact limited by the carrier velocity and is thus substantially constant above this critical voltage. For a non-linear pull-up load to be effective in a low voltage swing logic, the knee in the load IV characteristic has to occur at a voltage smaller than the logic swing. This can be achieved by a length of GaAs mesa with very closely spaced ohmic contacts. One micron separation, for example, will give a knee at approximately 0.5V. The power dissipation in an inverter gate is determined by the current limiting effect in the load due to electron velocity saturation in GaAs. The value of this current is primarily a function of the cross section of the mesa, and, secondly, of surface effects and substrate leakage current. A few hundred micro amps of constant current, for example, can be obtained with a mesa of a few microns wide assuming an active layer thickness of 0.12 micron doped to 0.8 x 1017 /cm3. Figure 3 shows a typical logic element in incorporating the velocity saturated pull-up load of Figures 1 and 2. The logic element includes one or more field effect mode transistors 31, 31A coupled in parallel and arranged in series with a velocity saturated pullup load 32. We prefer to employ enhancement mode transistors (MESFET's), but depletion mode transistors could also be used. When the circuit input, IP, is low (i.e. logic 0) the MESFET 31 (31A) is off and the circuit output OP is high (i.e. logic 1). If the circuit input now goes high (i.e. logic 1) the MESFET 31 (31A) turns on causing the output signal at (OP) to go low (i.e. logic 0). Because the load 32 is velocity saturated during the switching process the speed of switching is enhanced compared to that of a circuit employing a conventional resistive load where the switching time is limited by the saturation of the transistor. Figure 4 shows a typical experimentally obtained IV characteristic of a normally-off MESFET with resistive and velocity saturation load lines in an inverter gate arrangement. Computer simulation of such normally-off inverter circuits with both linear and the present non-linear pull-up loads indicate that up to 40% increase in switching speed can be obtained with the latter. The primary effect of replacing a resistive with a velocity saturation pull-up load is the improvement in gain of the logic gate at its switching point. This occurs as the result of a significantly lower output conductance at the drain of the FET together with a higher current drive capability from the load. Apart from the improvement in propagation delay, a significant property of this load is the ability of maint#ining a good noise zergin for quasi normally-off FETs, i.e. FETs which require small negative voltages to fully pinch-off, making it more tolerant to processing variations. An additional feature of this non-linear velocity saturated load is its extremely small size which makes it an ideal component for large scale integration. The use of small mesa surface area but relatively thick active layer also minimises surface effects compared with a larger resistive load. Compared with depletion mode FET loads commonly used in normally-on logic, it has the additional advantage of a smaller parasitic node capacitance. Inverter, NOR, NAND and R/S latch gates in normallyoff logic using both types of pull-up loads have been fabricated and results compared. In each type of load, six resistor values and six current limit values have been examined. All current limit pull-up loads had 1 micron ohmic contact spacing. The MESFET geometry was of 1.5 micron gate length in 4.5 micron source drain spacing. All FETs had 50 micron gate width. The material used was vapour phase epitaxial GaAs grown by the Ass13 process. The grown material had an active layer 0.12 micron thick, doped to 0.8 to 1.0 x 1017/cc and grown on an undoped buffer layer, nominally 3 micron thick. To reduce the active channel region to normallyoff thickness, only material under the gate was removed. The pull-up loads were therefore fabricated on as-grown material. A light stimulated anodic oxidationgetch process was used to accurately remove a known amount of active material. The oxidationgetch process has a further advantageous self-limiting property in that the thickness of material left in the channel after the etch is determined by the amount of light used during the oxidation process. A calibration chart can thus be# made by plotting the light intensity against pinch-off voltages of MESFETs so obtained. Repeatability of the process is obtained by careful control of light intensity for a given required pinch-off voltage, in this case zero volts. Normally-off MESPETS with a recessed gate structure made by this process have high transconductances, typically 35 mmho/mm, compared to 20 mmho/mm from uniformly thinned material. This is due to the reduction of parasitic series gate to ohmic resistances. The self limiting property of the anodic oxidation/etch process helps to improve the uniformity in pinch-off voltage across a slice. Typical standard deviation in pinch-off voltage is 90 mV for slices approximately 2 cm square, with the best slice giving 60 mV, which is comparable to data for ion implanted material. Comparison of typical transfer characteristics measured from the inverter gates using two types of pull-up loads is illustrated in Figures 5 and 6. The resistor pull-up in Figure 5 is 13 which is the optimum value for the particular FET geometry used. Smaller load values generally give smaller gains at the switching points and less noise margin. Higher load values give slightly higher gains, but require higher rail voltages to operate. The velocity saturation load in Figure 6 has a current limit of approximately 40 microamp. The switching-characteris tics are relatively insensitive to larger current limit values. Smaller current limits reduce power consumption but also reduce the noise margin and gain. This is due to the difficulty in obtaining true constant current in the load at extremely low current values, i.e. a few tens of microamps, as the result of substrate leakage currents. The performance of the two types of loads are summarised in the table below: Resistive Velocity- Pull-up Saturation Pull- up Power dissipation (#W) (at VDD = 1.OV) 50 40 Output voltage swing (V) (fanout = 1) 0.42 0.56 Noise margin (mV) (high/low) 60/110 250/150 Switching-point gain 1.3 3.0

Claims: CLAIMS: 1. A field effect semiconductor logic element provided with a velocity saturated pull-up load, 2. A gallium arsenide logic element having a non-linear pull-up load, characterised in that said load comprises a gallium arsenide mesa formed from active material on an undoped substrate and provided with a pair of closely spaced electrodes. 3. An element as claimed in claim 2, characterised in that the mesa height is between 0.5 and 1.5 microns. 4. An element as claimed in claim 2 or 3, characterised in that the mesa material is doped to a level of 0.5 to 1.0 x 1017 /cc. 5. An element as claimed in any one of claims 2 to 4, characterised in that the logic element includes an enhancement mode field effect transistor. 6. An integrated circuit including a plurality of logic elements as claimed in any one of the preceding claims. 7. A gallium arsenide integrated logic circuit including a plurality of enhancement or depletion mode field effect transistors characterised in that at least one of said transistors is provided with a pullup load comprising a mesa formed from active material and provided with a pair of spaced electrodes, and that the electrode spacing is such that the pull-up load is velocity saturated at an applied voltage less than the operating voltage of the transistor. 8. A high speed data transmission system incorporating a plurality of integrated circuits as claimed in claim 6 or 7.

Inventors: MUN, JOSEPH, PHILLIPS, JOHN ALEXANDER
Applicants: DEUTSCHE ITT INDUSTRIES GMBH, ITT INDUSTRIES INC.
Application year: 1981
Main classification: H01L27
IPC codes: H01L29, H01L47, H01L27, H01L21