INSULATED-GATE FIELD-EFFECT TRANSISTOR EMPLOYING SMALL BAND-GAP MATERIAL

Abstract: This insulated-gate field effect transistor comprises an insulator (1) carrying a gate electrode (7) on one side thereof and drain and source electrodes (4, 5) on the other. A film (6) of a material having a small band gap at Fermi level extends on the insulator (1) between the drain and source electrodes (4, 5). A first potential (V g ) applied between the source and gate electrodes (5, 7) causes an electric field across the insulator (1), which field controls the flow of current through said film (6) as a second potential is applied between the drain and source electrodes (4, 5). The preferred small band-gap materials encompass semimetal and semiconduc­ tor materials, namely bismuth and bismuth alloys, graphite and graphite intercalation compounds, doped polymers, and organic metals.

Description: INSULATED-GATE FIELD-EFFECT TRANSISTOR EMPLOYING SMALL BAND-GAP MATERIAL This invention relates to an insulated gate fieldeffect transistor employing a small band gap material for its current channel, which may be used, for example, as an active amplifying element in electronic circuitry. A conventional field-effect transistor consists of two electrodes connected by a narrow channel the conductivity of which can be controlled by an electric field applied to a gate electrode which is insulated from the channel. Known in the art are field-effect transistor structures in which the channel is made of a semiconductor material of n-type conductivity and constricted by a p-type conductivity gate region (see e.g. K.J. Dean, Integrated Electronics, Chapman and Hall, London 1967). When a potential is applied between thy bands of the channel, called source and drain, respectively, an impurity current will flow passing through the constricted region and causing a potential gradient along its length. With a potential applied to the gate electrode, the p-n junction between the gate and the channel becomes reverse biased so that a depletion layer is formed near the junction. The width of this depletion layer is a function of the gate potential. Thus, with increasing gate potential, the channel becomes still more constricted, until the conductance of the channel approaches zero. US-A-3,500,137 discloses a cryogenic device comprising a semiconductor channel permitting superconducting carrier transport in an operation mode analogous to field-effect transistors. A first gate is provided to apply a potential for controlling the depletion/enhance ment of the conducting region. By application of a magnetic field via a second gate, the superconductor can be switched between superconducting and normal resistive states. Known from EP-A ) is a tunneling transistor with a semiconductor channel which, at low temperatures, behaves like an insulator with a low barrier through which charge carriers can tunnel under the influence of an applied drain voltage. The tunnel current is controlled by a gate voltage which modifies the barrier height between source and drain. The field-effect transistors known in the art have various limitations among which is the temperature range in which they can operate - field-effect transistors with superconductors require helium temperatures -, and/or their relatively low cutoff frequency. It is, therefore, an object of the present invention to propose an insulated-gate field-ettect transistor employing normal-conducting materials operating at room temperature as well as at low temperatures down to liquid helium temperature and yet having a relatively high cutoff frequency in the neighbourhood of 16 GHz. These goals can be achieved in accordance-with the present invention with an insulated-gate field-effect transistor employing a semimetallic channel material such as bismuth or a bismuth alloy, or a small band-gap semiconductor material. The proposal to use these materials EP Appln. 83113163.6 is based on the cognition that they #have a very high mobility of their charge carriers, also at low temperatures, and that they show a sufficiently great field dependence. This is in contrast to the classical semiconductors, viz. silicon and germanium, in which the charge carriers, even from shallow donors, are frozen out at low temperatures, in other words, their mobility becomes virtually zero. The field dependency of the resistivity of bismuth is known from Y.F. Ogrin, V.N. Lutskii and M.I. Elinson, Field Effect in Bismuth, Sov. Phys.- Solid State 9 (1968) 2547; C. Reale, Field Effect in Vacuum-Deposited Bismuth Films, Phys. Lett. 35A (1971) 437; and D.A. Glocker and M.J. Skove, Field Effect and Magnetoresistance in Small Bismuth Wires, Phys. Rev B 15 (1977) 608. Of particular importance in connection with the present invention is the observation of the field-effect in thin bismuth films. In addition to pure bismuth, the invention contemplates the use of bismuth alloys for the current channel, with a preference placed on bismuth-antimony alloys. Alloying antimony to bismuth yields a continuous transition from semimetallic bismuth to a semiconductor. The overlap of valence and conduction bands, typical for semimetals, disappears at 5% antimony in the alloy. The activation energy has a maximum value of 14 meV at 12% antimony. Accordingly, the present invention relates to an insulated-gate field-effect transistor having gate, source and drain electrodes and an insulator separating said gate electrode from said source and drain electrode es, with the characteristic that a film of a material having a band-gap between +0,3 eV and -0,3 eV at the Fermi level extends on said insulator on its side oppo site from the gate electrode and between said drain and source electrodes, and that said source and drain elec trodes are i#n ohmic contact with said film, such that with a first potential applied between said gate and source electrodes, an electric field exists across said insulator, said field controlling the flow of current between said source and drain electrodes as a second potential is applied therebetween. Details of an embodiment of the invention will hereafter be described by way of example with reference to the attached drawings in which Fig. 1 is a schematic representation of the field-effect transistor in accordance with the invention; Fig. 2 is a diagram showing the ratio of the electrical conductivity of bismuth films to the conductivity of bulk material as a function of the electric field E for various film thicknesses d. x Referring to Fig. 1, there is shown a field-effect transistor structure comprising an insulator 1 carrying on one side a drain region 4 and a source region 5, respectively fitted with electrodes 2 and 3. Extending on insulator 1 between drain region 4 and source region 5 is a thin film .6 consisting of a semimetal, viz. bismuth. On the other side' of insulator 1 opposite bismuth film 6 is a gate region 7 carrying an electrode 8. Drain region 4 and source region 5 form ohmic contacts with bismuth film 6. In view of the fact that in a semimetal conduction and valence bands overlap, the current flowing in bismuth film 6 is not necessarily unipolar since both electrons and holes may contribute. Accordingly, the configuration in accordance with the invention is an alternative to the known unipolar fieldeffect transistors. In contrast to the known MESFET, no Schottky barrier is used for altering the geometry of the channel; in contrast to the known MOSFET, no p-n junctions at source and drain and no induced channel in an inversion layer under the gate are formed. Evidently, these differences account for advantages in the fabrication and operation. In particular, parasitic resistances in the source and drain regions can be kept low. The gate region 7 may in principle consist of a metal or a semiconductor. Of course, for applications of the field-effect transistor in accordance with this invention at low temperatures, the semiconductor material will not be suitable. In the following, the characteristics of a fieldeffect transistor constructed in accordance with this description will be reviewed. Fig. 2 shows the ratio of the electrical conductivities of bismuth films and bulk material (a/ab) as a function of the electric field Ex for various film thicknesses d, using experimental data of C. Reale, published in his Phys. Lett. article mentioned above. In agreement with Fig. 2, the conductivity a of bismuth films of 10 to 50 nm thickness can well be approximated by EMI5.1 where a (d) is the conductivity in the absence of an electric field, d is the thickness of the bismuth film, Ex is the transverse electric field, and E (d) is the critical electric field. Using Fig. 2, the value a for a d=10 nm thick 0 bismuth film is #o = 1 x 105 A/Vm and the critical electric 0 field is Eo = - 2 ¯ 10 V/m. In the configuration shown in Fig. 1, the gate field is Ex r - Vg/di and the drain field Ez = - Vd/L < < IEX . The drain current per width w results to EMI6.1 and the transconductance EMI6.2 For a bismuth film with the material parameters given above and with a gate length L = 1 pm, for an insulator thickness of d. = 50 nm, a drain voltage of Vd = 1 V, the transconductance per width becomes EMI6.3 Introducing the gate capacitance per width EMI6.4 the cutoff frequency of the field-effect transistor of Fig. 1 becomes EMI7.1 If the insulator is chosen as A1203, #i P 9. The cutoff frequency thus is fco = 109s-1 at room temperature. (7) By inserting a, P Neyeff (8) with N being the carrier concentration, and e the charge of an electron, and EMI7.2 into equation (6), we get the standard expression for the cutoff frequency of MOSFET's for the case of drain voltages below saturation: EMI7.3 Using again equations (8) and (9), the effective mobility follows as: EMI7.4 For the bismuth film under consideration, for room temperature, one gets EMI7.5 and the carrier concentration EMI8.1 The parameters chosen for the foregoing calculation on the basis of the work by C. Reale yield a good transistor performance at room temperature. It is known to those skilled in the art that with falling temperature the carrier mobility in bismuth increases while the carrier concentration decreases. In accordance with A.L. Jain, Temperature Dependence of the Electrical Properties -of Bismuth-Antimony Alloys, Phys. Rev. 114 (1959) 1518, the following table gives orders of magnitude of this dependence for pure bulk bismuth: EMI8.2 <tb> T <SEP> peff <tb> [ <SEP> K1 <SEP> im2/Vs ] <SEP> [ m'3 ] <tb> 300 <SEP> > <SEP> 10-2 <SEP> 1026 <tb> <SEP> 77 <SEP> 10 <SEP> 1024 <tb> <SEP> 4,2 <SEP> 103 <tb> Straightforward application of equation (10) leads to surprisingly high cutoff frequencies at low tempera tures, viz. fco X 1012 Hz at 77 K and even ¯ 1014 ltz at co 4,2 K. However, the use of bismuth alloys and thin films rather than pure bulk bismuth certainly requires the modification of Jain's data, yet there is a remarkable tendency toward high cutoff frequencies at low temperatures. Also, the critical field Eo will be considerably reduced. At low drain voltages, the drift velocity of the carriers is EMI9.1 If we rewrite equation (10) accordingly, we get EMI9.2 At high drain voltages, a non-linear behavior of Vdrift as a function of Vd leading to saturation might be expected. Apparently, saturation drift velocities V5 in semimetals like bismuth and bismuth alloys have so far not been reported in the literature. However, it does not seem to be too far-fetched if one speculates that the drift velocity in semimetals is in the same order of magnitude as in semi- conductors, viz. Vs > 105 m/s. Accordingly, the cutoff frequency in the saturation regime for the field-effect transistor with the beforementioned specification would be fco < 16 . 109 Hz. Insulated-gate field-effect transistors employing semimetals appear to become competitive with other devices at 77 K, and certainly below this temperature, because of their advantageous carrier mobility versus temperature characteristics. Besides bismuth and its alloys, other semimetals may be employed in the fieldeffect transistor of the present invention. The high carrier mobilities in the basal planes of quasi-twodimensional structures of graphite and graphite inter calation compounds as described by S.A. Solin, The Nature and Structural Properties of Graphite Intercalation Compounds, Adv. Chem. Phys. 49 (1962) 455 may be used, whereby the controlling electric field Ex (Fig. 1) should preferably be perpendicular to the basal plane. Also, quasi-one-dimensional structures like doped polymeres, such as polyacetylene and others, show high initial drift velocities, as was reported by B. Movaghar and N. Cade, Spontaneous Localization of Excitations in Polydiaethylenes, J. Phys. C15 (1982) L807. Another example for an organic substance with high carrier mobility which may be employed in the field-effect transistor of the present invention is the organic metal (TMTSF)2PF6 as described by P.M. Chaikin, Mu-Yong Choi, P. Haen, E.M. Engler and R.L. Green, Magnetotransport and Non-Linear Effects in (TMTSF)2PF6 Semiconducting Organic Compounds, Mol. Cryst. Liq. Cryst., Vol. 79, Nr. 1-4, Jan. 1982, Proc. of the.Int. Cont. on Low-Dimens. Conduct, Part. B, Boulder Colo, Aug. 9-14, 1981, p. 79-94.

Claims: CLAIMS 1. Insulated-gate field-effect transistor having gate, source and drain electrodes and an insulator separating said gate electrode from said source and drain electrodes, characterized in that a film (6) of a mate rial having a band gap between +0,3 eV and -0,3 eV at the Fermi level extends on said insulator (1) on its side opposite from said gate electrode (7) and between said drain electrode (4) and said source electrode (5), that said drain and source electrodes (4, 5) are in ohmic contact with said film (6), such that with a first potential (Vg) applied between said gate electrode (7) and said source electrode (4) an electric field exists across said insulator (1), said field controlling the flow of current between said drain and source electrodes (4, 5) as a second potential (Vd) is applied therebetween. 2. Field-effect transistor in accordance -with claim 1, characterized in that said film (6) consists of a semiconductor material having a band gap between +0,3 and 0 eV. 3. Field-effect transistor in accordance with claim 1, characterized in that said film (6) consists of a semimetal material having a band gap of < 0eV up to -0,3 eV. 4. Field-effect transistor in accordance with claim 3, characterized in that said film (6) consists of bismuth. 5. Field-effect transistor in accordance with claim 3, characterized in that said film (6) consists of a bismuth alloy. 6. Field-effect transistor in accordance with claim 3, characterized in that said film (6) consists of graphite. 7. Field-effect transistor in accordance with claim 3, characterized in that said film (6) consists of a graphite intercalation compound. 8. Field-effect transistor in accordance with claim 3, characterized in that said film (6) consists of a doped polymer. 9. Field-effect transistor in accordance with claim 3, characterized in that said film (6) consists of an organic metal. 10. Field-effect transistor in accordance with claim 5, characterized in that said film (6) consists of a bismuth-antimony alloy.

Inventors: JAGGI, RUDOLF, DR., MUELLER, CARL ALEXANDER, PROF. DR.
Applicants: INTERNATIONAL BUSINESS MACHINES CORPORATION
Application year: 1984
Main classification: H01L29
IPC codes: H01L29, H01L51