Logic device using ceramic superconducting element

Abstract: A logic device includes a ceramic superconducting element (4) having magneto-resistive characteristics, and three electrodes (12, 14, 16) provided adjacent the ceramic superconducting element, and constructed in such a manner that a current is applied to one of the three electrode so that a magnetic field greater than a threshold magnetic field (H0) is normally applied to the ceramic superconducting element (4), and the other electrodes (14, 16) are used for increasing and decreasing the magnetic field. A memory device includes a superconducting loop (46, 48) at least one portion thereof being formed by a ceramic superconducting element (46) having grain boundaries, and an electrode (44) provided in approximation to said ceramic superconducting element (46), whereby a current flowing through a portion (48) of said superconducting loop which is other than said ceramic superconducting element (46) can be captured in said superconducting loop by a control of a magnetic field generated by the current flowing through said electrode (44).

Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to logic devices employing a superconducting element. 2. Description of the Prior Art It is known to use the Josephson effect to theoretically form a logic circuit such as an AND gate. Josephson device is one of well-known logic devices which use the characteristics of superconductors. The logic device utilizing the Josephson effect, herein referred to as a Josephson device, according to prior art has such a structure that an extremely thin insulation film is sandwiched between layers made of superconducting materials, such as niobium, lead, or their alloys. The insulation film in a Josephson device of the above type requires a thickness of the order of ten angstroms. Production of such a thin insulation film, however, requires advanced thin film manufacturing technologies, and actual production is difficult. In addition, although one technical advantage of the Josephson device is its extremely fast operating speed, the output level change is very small. Thus, the Josephson device is not applicable to logic circuits from a practical viewpoint. In view of the above, a ceramic superconducting element's new phenomenon has been found and is disclosed in detail in prior Japanese patent applications No. 62-233369 et seq (corresponding to U.S. application serial No. 226,067 filed July 29, 1988, and to EP-A-0 301 902, which are assigned to SHARP KABUSHIKI KAISHA, one of the co-applicants of the present application. When the ceramic superconducting element utilizing the new phenomenon is employed in a logic circuit, such as in an AND, OR, XOR (exclusive or), or NOT (inverter) gate, such a logic circuit shows a stable operation and can be manufactured at a high yield rate, as disclosed in Japanese patent application No. 63-117472 (corresponding to U.S. application serial No. 289,312 filed December 23, 1988, to EP-A-0 323 187, and to Chinese application No. 88109265.7 filed December 24, 1988), and in Japanese patent application No. 63-29526 (corresponding to U.S. application serial No. 309,228 filed February 10, 1989, to EP-A-0 328 398, and to Chinese application No. 89101727.5 filed February 10, 1989), which are assigned to SHARP KABUSHIKI KAISHA, one of the co-applicants of the present application. Although these applications teach the use of the ceramic superconducting element in a logic circuit, such as in an AND, OR, XOR (exclusive or), or NOT (inverter) gate, none of these teaches or suggests the use of the same in a logic circuit which can perform the IMPLICATION or EQUIVALENCE gate operation. The following Tables A and B show the IMPLICATION and EQUIVALENCE logics when they are expressed by the truth table. Also, these applications do not teach or suggest the use of the ceramic superconducting element in a memory device. Furthermore, Josephson devices have been conventionally used for storing data by utilizing the characteristics of superconductivity. In such devices, the presence or absence of fluxoid quantum travelling through a loop connected to the Josephson device was correlated to storage states "1" and "0." However, the structure of Josephson devices such as those used in conventional superconducting memory devices is typically layered, specifically one in which a thin film insulation layer is sandwiched between superconductor layers of niobium, lead, alloys thereof, or other materials. In a Josephson device as described above, the interposed insulation film must be formed of the order of ten angstroms in order to achieve the tunnel effect enabling superconductivity. That production of such a thin insulation film, however, requires advanced thin film manufacturing technologies and actual production is difficult, that the output level is low, and that use is only possible at very low temperatures has prevented the practical application of such devices. For additional background art, reference may be made to the following publications: (1) Proceedings of the IEEE, Vol.70, No.1, January 1982, pages 26-34; T. Gheewala: "The Josephson Technology" (2) FR-A-1 381 497. The present invention has been developed in consideration of the above described points. The object of the present invention is to provide an improved logic device employing a ceramic superconducting element which can perform the IMPLICATION or EQUIVALENCE gate operation. In a first aspect, the present invention, as defined by claim 1, provides a logic device comprising: a superconducting element having magneto-resistive characteristics, provided on a substrate; electrode means arranged adjacent to said superconducting element; and means for supplying current to said electrode means so as to apply to said element a selected magnetic field to determine the conductive state of the element, characterised in that: said superconducting element comprises ceramic superconductive material; said electrode means is provided on said substrate co-planar with said element; and said means for supplying current comprises: a first current source which supplies a first current to said electrode means; a second current source which is switchably connected to supply a second current to said electrode means; and a third current source which is switchably connected to supply a third current to said electrode means; said first and second currents, in combination, generating a net magnetic field which establishes a superconductive state of said element; said first and third currents, in combination, generating a net magnetic field which establishes a magneto-resistive state of said element; said first, second and third currents, in combination, generating a net magnetic field which establishes a magneto-resistive state of said element; said logic device performing IMPLICATION operation. The features of the preamble of claim 1 are known in combination from publication (2) above. According to this first aspect, an IMPLICATION logic device is realised. In a second aspect, the present invention, as defined by claim 2, provides a logic device comprising: a superconducting element having magneto-resistive characteristics, provided on a substrate; electrode means arranged adjacent to said superconducting element; and means for supplying current to said electrode means so as to apply to said element a selected magnetic field to determine the conductive state of the element, characterised in that: said superconducting element comprises ceramic superconductive material; said electrode means is provided on said substrate co-planar with said element; and said means for supplying current comprises: a first current source which supplies a first current to said electrode means; a second current source which is switchably connected to supply a second current to said electrode means; and a third current source which is switchably connected to supply a third current to said electrode means; said first and second currents, in combination, generating a net magnetic field which establishes a superconductive state of said element; said first and third currents, in combination, generating a net magnetic field which establishes a superconductive state of said element; said first, second and third currents, in combination, generating a net magnetic field which establishes a magneto-resistive state of said element; said logic device performing EQUIVALENCE operation. The features of the preamble of claim 2 are known in combination from publication (2) above. According to this second aspect, an EQUIVALENCE logic device is realised. The new phenomenon is explained below. Generally, the ceramic superconducting element shows a superconductive characteristics below a certain temperature, such as 77K, provided that no magnetic field is applied to the ceramic superconducting element. When magnetic field is applied to the ceramic superconducting element, but not greater than a threshold level H0, the ceramic superconducting element continues to show the superconductive characteristics, as shown in Fig. 1. Then, when the magnetic field applied to the superconducting element becomes equal to the threshold level H0, the superconducting element looses its superconductivity and suddenly shows magneto-resistance which increases at a high rate relative to the increase of the magnetic field. Thereafter, when the magnetic field is reduced to the threshold level H0, the magneto-resistance is also reduced to zero, again showing the superconductive characteristics. The same phenomenon is observed when the magnetic field is increased in the opposite polarity, as shown in Fig. 1. Since the resistance of the ceramic superconductive element is obtained by the application of magnetic field, the obtained resistance is referred to as a magneto-resistance, and such a phenomenon observed in the ceramic superconducting element is referred to as a superconducting magneto-resistance system. The superconducting magneto-resistance system can be understood as follows. When the ceramic superconductive element receives a magnetic field greater than the threshold level H0, the superconducting state of the crystal grain boundaries of the ceramic superconductor are destroyed by the applied magnetic field so that the superconductor changes from a superconducting state to an electrical resistance state. More specifically, when the ceramic superconducting element having crystal boundaries formed by the grains of a ceramic material is not receiving any magnetic field, the ceramic element shows no electrical resistance, as shown in Fig. 5. However, when a magnetic field greater than the threshold magnetic field H0 is applied, the ceramic element suddenly exhibits electrical resistance and the electrical resistance increases sharply as the applied magnetic field is increased. Since the rate of the change in resistance ΔR/ΔH at the threshold magnetic field H0 is as great as infinity, the logic device formed by the ceramic superconducting element utilizing superconducting magneto-resistance system will exhibit stable and high performance when compared with the conventional magneto-resistance elements. The trend in research in ceramic superconducting devices as being advanced by many research organizations today seeks to improve critical temperature (Tc), threshold magnetic field (H0), and threshold current (Jc) characteristics. In the research carried by the present inventors in the ceramic superconducting devices, the above mentioned phenomenon was found in specific types of superconductors (those having a weak coupling state between the grains of the superconducting body). The phenomenon is such that the superconducting state of these weak couplings is destroyed by a weak magnetic field (several gauss) as shown in Fig. 5, and thus exhibit electrical resistance, and that this resistance increases sharply with the increase in the strength of the applied magnetic field. This invention proposes a ceramic superconducting device which operates as a new type of logic circuit device using this phenomenon of a weak critical magnetic field. As shown in Fig. 2, the ceramic superconducting element comprises crystals of many superconducting fine grains in which an extremely thin insulator or resistor is interposed between the grains, but such grain boundaries exhibit zero electrical resistance, in which electrons move freely, due to the tunnel effect under the superconducting state. Or, the grains are contacted by a point. When juxtaposed grain boundaries exhibit a point contact in the so-called weak bond state, the superconductive state is obtained, and when a weak electrical field is applied, the point contacts are destroyed to exhibit ohmic resistance. In other words, a polycrystalline ceramic superconducting body in a weak bond state can equivalently form a bonded body of multiple Josephson bonds 121, as shown in Fig. 2. When a magnetic field is applied to a superconducting device of this type, the effects of the magnetic field break the superconducting state of Josephson bonds 121, specifically, the superconducting weak bond state is broken by the application of a weak magnetic field so that the device exhibits electrical resistance, and the strength of this electrical resistance increases as the strength of the magnetic field is increased. As will be clear from this principle as described above, this property is not dependent upon the direction of the applied magnetic field because the arrangement of the crystal grain boundaries is random, but is determined by the absolute value of the strength of the magnetic field. The present invention utilizes the weak bond existing at the crystal grain boundaries of a ceramic superconducting element. The device according to the present invention includes three conductive strips parallel or perpendicular to the superconducting device to provide different levels of magnetic field to the ceramic superconducting element by the electric current flowing through these conductive strips so as to change the ceramic superconducting element between superconductive and magneto-resistive states. In a preferred embodiment of the present invention, the ceramic superconducting element is made of Y₁Ba₂Cu₃O 7-x , Bi₁Sr₁Ca₁Cu₂O x , or any other ceramic superconducting film, and is formed in an elongated pattern. The electrical current conducting strips are made parallel or perpendicular to the ceramic superconducting film. In alternative embodiments of the aforementioned ceramic superconducting device, the three conductive strips which are provided on a single substrate, may be provided in a layered structure separated by an insulating material, or they may be juxtaposed with a parallel or perpendicular arrangement. Furthermore, in a preferred embodiment according to the present invention, each conductive strip is coupled with an independent current source. BRIEF DESCRIPTION OF THE DRAWINGS The features of the present invention will become apparent from the following description of preferred embodiments thereof with reference to the accompanying drawings, throughout which like parts are designated by like reference numerals, and in which: Fig. 1 is a graph showing the magneto-resistance change relative to the applied magnetic field strength in the ceramic superconducting element; Fig. 2 is a diagrammatic view of electric conductive passages formed in the ceramic superconductive material; Fig. 3 is a diagrammatic view of a logic device employing a ceramic superconducting element according to a preferred embodiment of the present invention; Figs. 4 and 5 are a graph showing condition change of the ceramic superconducting element by the application of magnetic field for performing IMPLICATION logic and EQUIVALENCE logic, respectively; Fig. 6 is a diagrammatic view showing a method for making the ceramic superconductive element on a substrate; Fig. 7 is a graph showing the magneto-resistance change relative to the applied magnetic field strength in the ceramic superconducting element for different electric currents applied to the ceramic superconducting element; Fig. 8 is a view similar to Fig. 3, but showing a modification thereof; Figs. 9a and 9b are views similar to Fig. 3, but showing further modifications thereof. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Structure Referring to Fig. 3, a logic device employing a ceramic superconducting element according to a preferred embodiment of the present invention is shown. In Fig. 3, reference number 2 is a logic device including a ceramic superconducting element 4 deposited on a substrate 3 and having an elongated configuration extending between current electrodes 6a and 6b. Current electrodes 6a and 6b are connected, respectively, with current supply electrodes 8a and 8b extending in opposite directions for supplying an electric current to flow through the ceramic superconducting element 4. Connected intermediately along the ceramic superconducting element 4 are voltage electrodes 10a and 10b for obtaining a voltage drop between the connected points of the ceramic superconducting element 4. Extending closely adjacent and parallel to the ceramic superconducting element 4 are three electrode strips 12, 14 and 16 for providing predetermined different levels of magnetic field in the ceramic superconducting element 4 by the control of electric current flowing through one, two or three of the three electrode strips. IMPLICATION logic In order to perform the IMPLICATION logic by the logic device of Fig. 3, DC current sources 18, 20, 22 and 24 are connected, respectively, to electrodes 8a, 12, 14 and 16. DC current sources 18, 20 and 24 are provided to supply DC current in one direction, e.g., from left to right in Fig. 3, and current source 22 is provided to supply DC current in the opposite direction, e.g., from right to left. A switch 26 is inserted between current source 22 and electrode 14, and a switch 28 is inserted between current source 24 and electrode 16. From current sources 20, 22 and 24, DC currents I1, -I2 and I3 can be supplied to electrodes 12, 14 and 16, respectively, provided that the current flowing from left to right in Fig. 3 is deemed as positive direction. By the currents I1, -I2 and I3, magnetic field having the strengths H1, -H2 and H3 are generated at the ceramic superconducting element 4. Determined by various factors, such as distance between the ceramic superconducting element 4 and electrode 12 and amount of current flowing through electrode 12, the magnetic field strength H1 is selected to satisfy the following inequality: H1>H0 in which H0 is a threshold field strength of the ceramic superconducting element 4. As shown in Fig. 4, if the field strength in the ceramic superconducting element 4 is between -H0 and +H0, the ceramic superconducting element 4 maintains the superconductive state, and if the field strength in the ceramic superconducting element 4 increases greater than +H0 or decreases smaller than -H0, the ceramic superconducting element 4 exhibits magneto-resistive state. Thus, when switches 26 and 28 are turned off to provide only current I1, the ceramic superconducting element 4 receives magnetic field H1, making element 4 in the magneto-resistive state. In a similar manner, the magnetic field strength H2 is selected to satisfy the following inequality: |H1-H2|<H0. Thus, when switch 26 is turned on and switch 28 is turned off to provide current -I2 in addition to current I1, the ceramic superconducting element 4 receives magnetic field H1-H2 which falls, as shown in Fig. 4, between -H0 and +H0, making element 4 in the superconductive state. Furthermore, the magnetic field strength H3 is selected to satisfy the following inequality: H1-H2+H3>H0. Thus, when switches 26 and 28 are both turned on to provide currents -I2 and I3 in addition to current I1, the ceramic superconducting element 4 receives magnetic field H1-H2+H3 which is greater than the threshold field strength H0, as shown in Fig. 4, making element 4 in the magneto-resistive state. Also, when switch 26 is turned off and switch 28 is turned on to provide current I3 in addition to current I1, the ceramic superconductive element 4 receives magnetic field H1+H3 which is greater than H0, as shown in Fig. 4, making element 4 in the magneto-resistive state. If a current is applied to ceramic superconductive element 4 from DC current source 18 a voltage drop will be observed across element 4 between electrodes 10a and 10b when the ceramic superconductive element 4 is in the magneto-resistive state, but no voltage drop will be observed between electrodes 10a and 10b when the ceramic superconductive element 4 is in the superconductive state. Accordingly, if the presence and absence of the current are indicated as "1" and "0", respectively, and the presence and absence of the voltage are also indicated as "1" and "0", respectively, the following Table C is obtained. As will be understood from Table C, input currents I2 and I3 and output voltage between electrodes 10a and 10b correspond to the IMPLICATION logic. It is to be noted that in order to meet the conditions of inequalities (1a), (1b) and (1c) indicated above, current sources 20, 22 and 24 may produce, for example, 10 mA, 25 mA and 40 mA for currents I1, -I2 and I3, respectively. EQUIVALENCE logic In order to perform the EQUIVALENCE logic, DC current source 24 is replaced by a DC current source 25, shown by a dotted line in Fig. 3, which is provided to supply DC current from right to left when viewed in Fig. 3. Thus, from current sources 20, 22 and 25, DC currents I1, -I2 and -I4 can be supplied to electrodes 12, 14 and 16, respectively, provided that the current flowing from left to right in Fig. 3 is deemed as positive direction. By the currents I1, -I2 and -I4, magnetic field having the strengths H1, -H2 and -H4 are generated at the ceramic superconducting element 4. Similar to the above, the magnetic field strength H1 is selected to satisfy the following inequality: H1>H0 Thus, when switches 26 and 28 are turned off to provide only current I1, the ceramic superconducting element 4 receives magnetic field H1, making element 4 in the magneto-resistive state, as understood from Fig. 5. The magnetic field strength H2 is selected to satisfy the following inequality: |H1-H2|<H0. Thus, when switch 26 is turned on and switch 28 is turned off to provide current -I2 in addition to current I1, the ceramic superconducting element 4 receives magnetic field H1-H2 which falls, as shown in Fig. 5, between -H0 and +H0, making element 4 in the superconductive state. Furthermore, the magnetic field strength H4 is selected to satisfy the following inequality: |H1-H2-H4|>H0. Thus, when switches 26 and 28 are both turned on to provide currents -I2 and -I4 in addition to current I1, the ceramic superconducting element 4 receives magnetic field |H1-H2-H4| which is greater than the threshold field strength H0, as shown in Fig. 5, making element 4 in the magneto-resistive state. Also, when switch 26 is turned off and switch 28 is turned on to provide current -I4 in addition to current I1, the ceramic superconductive element 4 receives magnetic field H1-H4 which falls, as shown in Fig. 5, between -H0 and +H0, making element 4 in the superconductive state. Accordingly, the following Table D is obtained, provided that the presence and absence of the current are indicated as "1" and "0", respectively, and the presence and absence of the voltage are also indicated as "1" and "0", respectively. As will be understood from Table D, input currents I2 and I4 and output voltage between electrodes 10a and 10b correspond to the EQUIVALENCE logic. It is to be noted that in order to meet the conditions of inequalities (2a), (2b) and (2c) indicated above, current sources 20, 22 and 25 may produce, for example, 10 mA, 25 mA and 40 mA for currents I1, -I2 and -I4, respectively. Method for Making the Logic Device In order to manufacture a ceramic superconducting device 2 of the type used in the present invention, a substrate 3 made of stabilized zirconia is heated by a heater Ht provided in a film forming apparatus Fa as shown in Fig. 6 to maintain a substrate temperature of 400°C. The ceramic material is a mixture of Y(NO₃)₃·6H₂O, Ba(NO₃)₂, and Cu(NO₃)₂.3H₂O weighed to form Y₁Ba₂Cu₃O₇-x, mixed in a nitrate solution which is sprayed intermittently by air sprayer Sp onto substrate 3 so as to form a film having a thickness of 5µm. Thus, a spray pyrolysis method may be used. The substrate and film are then baked at 950°C for 60 minutes and thereafter annealed in air for 10 hours at 500°C. Regarding the critical temperature of a ceramic superconducting film thus formed, resistance begins to drop from 100K, and loses all resistance at 83K. Next, in order to process the high temperature ceramic superconducting film to a 50 µm wide, 30 mm long superconducting body 4, the substrate 3 is applied with a photoresist and processed with conventional photolithography processes to form a fine striped shape, thus forming the superconducting element 4 on substrate 3. This ceramic high temperature superconducting element can be easily processed in a phosphoric acid etching agent. Next, in order to manufacture the electrodes 6a, 6b, 8a, 8b, 10a, 10b, 12, 14 and 16, a pattern is formed by Ti deposition film by the photolithographic processes and a lift-off technique, and the ceramic superconducting device as shown in Fig. 3 is prepared. The ceramic superconducting device 2 used in the present invention forms weak couplings due to the point contacts and insulating layer interposed between the grain boundaries, and may be thought of as an aggregation of Josephson junctions. Regarding the relationship between the applied magnetic field and electrical resistance shown in Fig. 7, magneto-resistance suddenly appears and increases rapidly when the strength of the magnetic field applied to the ceramic superconducting element, which has been in the superconductive state, exceeds a threshold level. Such a threshold level varies depending on the current flowing through the ceramic superconducting element. When a 10 mA current is supplied to electrode 12, formed of a Ti film, a magnetic field of 0.4 gauss can be obtained at a distance of 50 µm. Therefore, as apparent from the characteristics of the superconducting material shown in Fig. 7, when a 2 mA constant current is supplied to the superconducting element 4 through terminals 6a and 6b while receiving the 0.4 gauss magnetic field, the superconducting element will show 10 mΩ and thus, a 20 µV (10 mΩ X 2 mA) output can be obtained. According to one preferred embodiment, the ceramic superconducting device 2 shown in Fig. 3 has such a arrangement that the centre to centre distance between electrodes 16 and 14, between electrodes 14 and 12, between electrode 12 and ceramic superconducting element 4 is 50 µm, and the width of each of electrodes 12, 14 and 16 is 30 µm, and the width of ceramic superconducting element 4 is 50 µm. When the ceramic superconducting device 2 of the above described construction is cooled to a temperature lower than 83K, and if no current is supplied to electrodes 12, 14 and 16 to provide no magnetic field at the ceramic superconductive element 4, an output voltage will not appear between electrodes 10a and 10b even when a current is supplied to ceramic superconducting element 4 via electrodes 8a and 8b, because in this case element 4 is maintained in the superconductive state. However, if a 10-mA current I1 is supplied to electrode 12 from current source 20, the magnetic field created by this current destroys the superconductive state of element 4, and produces magneto-resistance. Thus, a 20 µV output is obtained between electrodes 10a and 10b when a constant current 2 mA is supplied through element 4. It is to be noted that, according to the present invention as described above, the values of currents I1, I2, and I3 and the arrangement of electrodes 12, 14, 16 and element 4 are not limited to those described above, but they may take any other amounts and sizes. For example, it is possible that currents I1, I2, and I3 supplied to electrodes 12, 14 and 16 may be made constant and equal to each other, and that electrodes 12, 14 and 16 may be so spaced as to satisfy inequalities (1a), (1b) and (1c) or inequalities (2a), (2b) and (2c). In addition, the method for making electrodes 12, 14 and 16 and superconducting element 4 as described above should not be limited to the process as described above, but other processes, such as sputtering, MOCVD, or electron beam evaporation techniques may be used, as long as the same effects can be obtained. In particular, electrodes 12, 14 and 16 may be formed by a superconducting thin film, and in such a case, they may be formed at the same time as superconducting element 4 is made, thereby simplifying the manufacturing process. Moreover, as apparent to those skilled in the art, while the ceramic high temperature superconducting film used in the present invention is Y₁Ba₂Cu₃O₇-x, the same effect may be obtained by using other high temperature superconductors as long as the grain boundaries form a weak coupling. Furthermore, the relationship of the positions of superconducting element 4 and electrodes 12, 14 and 16 shall not be limited to that described above with respect to the present embodiment. For example, one of the electrodes, such as electrode 12, may be formed on the opposite side of superconducting body 4, as shown in Fig. 8. Moreover, the same effect may be obtained if electrodes 12, 14 and 16 are formed one over the other with an insulation layer of SiO₂ or a polyimide resin inserted therebetween. Also, as shown in Fig. 9a, only one electrode 30 may be provided to receive currents from different current sources 20, 22 and 24. In this case, suitable diodes are provided to prevent currents from flowing back to the current source. Alternatively, as shown in Fig. 9b, one electrode 32 is provided for receiving currents in one direction and another electrode 34 is provided for receiving currents in the other direction. The present invention uses the properties of superconductivity, but does not use Josephson devices which use extremely thin insulation films which are extremely difficult to manufacture by conventional methods. Thus, the ceramic superconductive devices according to the present invention, which uses the weak coupling magneto-resistive effects of a superconducting element formed easily in the grain boundaries of a ceramic superconducting element, can be easily manufactured. Thus, the devices according to the present invention provide good noise resistance with a practical power supply for both input and output, and offer handling which is not difficult.

Claims: A logic device comprising: a superconducting element (4) having magneto-resistive characteristics, provided on a substrate (3); electrode means (12,14,16;30;32,34) arranged adjacent to said superconducting element; and means for supplying current (20,22,24) to said electrode means so as to apply to said element a selected magnetic field to determine the conductive state of the element, characterised in that: said superconducting element (4) comprises ceramic superconductive material; said electrode means is provided on said substrate (3) co-planar with said element; and said means for supplying current comprises: a first current source (20) which supplies a first current to said electrode means (12;30;32); a second current source (22) which is switchably connected to supply a second current to said electrode means (14;30;34); and a third current source (24) which is switchably connected to supply a third current to said electrode means (16;30;32); said first and second currents, in combination, generating a net magnetic field which establishes a superconductive state of said element; said first and third currents, in combination, generating a net magnetic field which establishes a magneto-resistive state of said element; said first, second and third currents, in combination, generating a net magnetic field which establishes a magneto-resistive state of said element; said logic device performing IMPLICATION operation. A logic device comprising: a superconducting element (4) having magneto-resistive characteristics, provided on a substrate (3); electrode means (12,14,16;30;32,34) arranged adjacent to said superconducting element; and means for supplying current (20,22,25) to said electrode means so as to apply to said element a selected magnetic field to determine the conductive state of the element, characterised in that: said superconducting element (4) comprises ceramic superconductive material; said electrode means is provided on said substrate (3) co-planar with said element; and said means for supplying current comprises: a first current source (20) which supplies a first current to said electrode means (12;30;32); a second current source (22) which is switchably connected to supply a second current to said electrode means (14;30;34); and a third current source (25) which is switchably connected to supply a third current to said electrode means (16;30;32); said first and second currents, in combination, generating a net magnetic field which establishes a superconductive state of said element; said first and third currents, in combination, generating a net magnetic field which establishes a superconductive state of said element; said first, second and third currents, in combination, generating a net magnetic field which establishes a magneto-resistive state of said element; said logic device performing EQUIVALENCE operation. A logic device according to claim 1 or claim 2, wherein said electrode means comprises: a first electrode (12) connected to said first current source (20); a second electrode (14) switchably connected to said second current source (22); and a third electrode (16) switchably connected to said third current source (24;25); said first, second and third electrodes each being provided on said substrate (3) adjacent to and co-planar with said superconducting element (4).

Inventors: HASHIZUME NOBUO, KATAOKA SHOEI, MORISUE MICHITADA, NOJIMA HIDEO, TSUCHIMOTO SHUHEI, HASHIZUME, NOBUO, KATAOKA, SHOEI, MORISUE, MICHITADA, NOJIMA, HIDEO, TSUCHIMOTO, SHUHEI
Applicants: MORISUE MICHITADA, SHARP KK, MORISUE, MICHITADA, SHARP KABUSHIKI KAISHA
Application year: 1989
Main classification: H01L39
IPC codes: H01L39, G11C11