Thin film Josephson device

Abstract: A thin film device comprising a substrate and an oxide superconductor film formed thereon, wherein said oxide superconductor film comprises atomic monolayers each composed of at least one kind of element of the oxide superconductor, which are deposited substantially in a vertical direction to the substrate so that the pereodicy of the lattice structure of the oxide superconductor is substantially maintained, and at an intermediate portion of the oxide superconductor film, at least a part of the atoms of the oxide superconductor is substituted by other element in the lattice structure of the oxide superconductor to form a non-superconductor interlayer, and the pereodicy of the lattice structure of the oxide superconductor film is substantially maintained across the interface between the oxide superconductor and said non-superconductor interlayer.

Description: The present invention relates to a thin film device and more particularly to a Josephson device wherein an oxide high temperature superconductor is employed. In recent years, research has been actively conducted on an oxide superconductor containing Cu-O layers in the crystal structure, as a superconductor which may be substituted for conventional superconductors of Nb or Al5 type compound (β-W type crystal structure) such as Nb 3 Sn or Nb 3 Ge. As a typical material for such an oxide superconductor, a Y-Ba-Cu-O (YBCO) type (critical temperature Tc > 90K), a Bi-Sr-Ca-Cu type (critical temperature Tc = 80-110K), or a Tℓ-Ba-Ca-Cu-O type (critical temperature Tc = 90-120K) is known. The most important technique in a case where such a material is used as a Josephson device as an electronic device, is formation of a Josephson junction. This Josephson junction is usually formed by a vapor deposition method, a sputter vapor deposition method or laser ablation. However, it is known that in the above mentioned material, the coherence length is very short. It is usually thought that for a good Josephson junction, the size of the disorder at the interface should be less than the coherence length. The surface tends to readily deteriorate. Therefore, when a Josephson junction is formed by laminating thin films of such a material with an interlayer interposed therebetween to form a space, the lattice matching between the superconductor material and the interlayer tends to be poor, and there will be drawbacks such that the properties of the adjacent superconductor layers tend to deteriorate or a leakage current from the interlayer is likely to be observed, whereby it tends to be difficult to obtain a S/N/S (superconductor/normal conductor/superconductor) junction with good reproducibility, or even in the case of a S/I/S (superconductor/insulator/superconductor) junction, a leakage current is likely to result, or a superconducting connection tends to be hardly obtained. To solve such drawbacks, the following methods (a) to (c) have been proposed, for example, in the case of a laminated thin film device. (a) A method wherein an insulating film is formed on an oxide superconductor, and then a conventional type (phonon type) superconductor (such as Nb or a Nb type alloy, or Pb or a Pb compound) is laminated thereon. (b) A method wherein a metal superconductor material having a relatively small amount of oxygen or a material commonly used for a substrate such as MgO, SrTiO 3 or ZrO 2 , is laminated as an interlayer on an oxide superconductor, and a superconductor is laminated thereon. (c) A method wherein on an oxide superconductor, an insulator layer is formed by substituting the rare earth element or alkaline earth metal of such an oxide superconductor by other atoms, and an oxide superconductor is laminated on such an insulator layer. However, in the case of the above method (a), a conventional superconductor is employed, whereby there is a problem that the thin film device can be operated only at a temperature corresponding to the temperature of liquefied helium. The method (b) has a problem that in the case where a metal superconductor material having a relatively small amount of oxygen is used as the interlayer, it is difficult to obtain a sharp interface since the controllability of the diffusion of oxygen during annealing tends to be poor, or in the case where a substrate material like MgO is employed, it tends to be difficult to obtain a film having good properties because of the diffusion of Mg or the like. The method (c) has a problem that-since the bond between the superconducting Cu-O layer and the rare earth element or the like is weak, and the above mentioned substitution is required to be conducted in a large quantity (at least 50%) in order to convert the superconducting properties to the insulating properties. In "Physical Review Letters", Volume 64, Number 7, 12 February 1990, pages 804 to 807, describes a multilayer structure, or a superlattice, wherein several atomic layers of each YBC0 superconductor and PrBC0 are deposited alternately. In the reference, the superlattice is formed by depositing several atomic layers of each of YBC0 and PrBC0 alternately by single-target dc planar magnetron sputtering, using two targets of YBC0 and PrBC0. The reference describes nothing about the lattice structure across interfaces between the YBC0 and PrBC0 layers or about the control of the interfaces. Further, in "Applied Physics Letters", Volume 55, No. 19, 6 November 1989, pages 2032 to 2034, a Josephson device composed of YBCO and PrBC0 layers is disclosed. However, the reference discloses nothing about interfaces between the YBC0 and PrBC0 layers or about the control of the interfaces. The present inventors have conducted extensive researches with an aim to solve the above problems and have found a method whereby a S/N/S or S/I/S structure can be prepared without substantially changing the structure of the oxide superconductor. Namely, the present invention has been accomplished by paying a particular attention to the specificity of the basic structure of an oxide superconductor containing Cu, particularly to the two dimensional characteristic thereof. The present invention provides a Josephson device comprising a substrate and an oxide superconductor film formed thereon, wherein said oxide superconductor film comprises atomic monolayers each composed of at least one kind of element of the oxide superconductor, which are deposited in a predetermined and periodic order substantially in a vertical direction to the substrate so that the lattice structure of the oxide superconductor is substantially maintained, and at an intermediate portion of the oxide superconductor film, at least a part of the atoms of the oxide superconductor is substituted by other element in the lattice structure of the oxide superconductor to form a non-superconductor interlayer, and the periodicity of the lattice structure of the oxide superconductor film is substantially maintained across the interface between the oxide superconductor and said non-superconductor interlayer. Here non-superconductors are meant to be insulators, semiconductors, compounds which do not undergo super conducting transition, or whose superconducting temperature is below operating temperature. Now, the present invention will be described in detail with reference to the preferred embodiments. Specifically, the above oxide superconductor film is, for example, an oxide superconductor film containing Cu-O layers, which is composed of e.g. LB 2 Cu 3 O 7-δ wherein L is a rare earth element, and B is an alkaline earth metal, TℓBa 2-n Ca n-1+x Cu n O 2n+1 wherein n is 1, 2 or 3, or Bi 2 Sr x Ca y Cu n O 2n+4 wherein n is 1, 2 or 3, and x + y ≃ n + 1. In the present invention, at an intermediate portion of such an oxide superconductor film, a part or whole of such Cu is substituted by other element to form a non-superconductor interlayer. As such a substituting element, an element of Group IIb in the Periodic Table, an element of Group IIIb in the Periodic Table or a transition element other than Cu, may be employed. When the above oxide superconductor is composed of LB 2 Cu 3 O 7-δ wherein L is a rare earth element, and B is an alkaline earth metal, at a non-superconductor interlayer of the oxide superconductor film, a part or whole of such L may be substituted by other rare earth element or alkaline earth metal element. Further, when the above oxide superconductor film is composed of TℓBa 2-n Ca n-1+x Cu n O 2n+1 wherein n is 1, 2 or 3, or Bi 2 Sr x Ca y Cu n O 2n+4 wherein n is 1, 2 or 3, and x + y = n + 1, at an intermediate portion of the oxide superconductor, a part or whole of Ca may be substituted by other alkaline earth metal or a trivalent rare earth element such as Y. For the preparation of such an oxide superconductor film, a method such as molecular beam deposition (MBE), laser ablation or a vapor deposition method by means of electron beams or heating by resistance. Further, as a specific method for depositing the atomic monolayers for the oxide superconductor film substantially in a vertical direction to the substrate so that the periodicity of the lattice structure of the oxide superconductor will be formed as described above, a method similar to the one employed in the conventional art for the preparation of a super-lattice, may be employed. As such a specific method, there may be mentioned a method in which the respective atomic monolayers constituting the oxide superconductor film and non-superconductor interlayer are sequentially deposited one after another, for example, in the case of YBCO, in the order of BaO, CuO 2 , BaO, CuO 2 , Y, CuO 2 , that is to say a layer by layer vapor deposition method. Otherwise, it is, of course, possible to employ a method wherein the respective block layers constituting the oxide superconductor film are sequentially deposited by vapor deposition. In this case, for example, in the case of YBa 2 Cu 3 O 7 , the vapor deposition may be conducted in the order of BaCuO 2 , YCuO 2·5 and BaCuO 2 . Further, in the case of Bi 2 Sr 2 CaCu 2 O 8 , the film can be prepared by conducting the deposition in the order of Bi 2 O 2 -SrCuO 2 -CaCuO 2 -SrCuO 2 (-Cu), as described in the article by Kawai, Adachi, et al in JJAP 27 (1988) 21883. In the accompanying drawings: Figure 1(A) is a view illustrating the basic structure of an oxide superconductor of YBCO type having a c-axis orientation. Figures 1(B) to (D) are views likewise illustrating the structures of the present invention. Figure 2(A) is a view illustrating the basic structure of an oxide superconductor of YBCO type having an a-axis orientation. Figures 2(B) and (C) are views likewise illustrating the structures of the present invention. Figure 3(A) is a view illustrating the basic structure of Bi 2 Sr 2 CaCu 2 O 2n+4+δ . Figure 3(B) is a view illustrating the same structure in which Cu is substituted by CuM. Figure 3(C) is a view likewise illustrating a case wherein Ca is substituted by CaY. Figure 4 is a view illustrating an embodiment of the laminated structure of a thin film device of the present invention. Figure 5 is a view illustrating a conventional hetero epitaxial growth in an oxide superconductor of YBCO type. In an actual thin film device, current contacts are provided independently at the upper and lower portions of the modulated portion where at least a part of atoms is substituted at an intermediate portion (interlayer) of the oxide superconductor film. Therefore, after the preparation of the above mentioned oxide superconductor layer, etching treatment is conducted to expose the lower superconductor portion S 1 as shown in Figure 4, or after preparation of the lower superconductor portion S 1 or, in some cases, after preparation of a modulated portion D, masking is conducted to expose a part of the lower superconductor portion S 1 and to have the rest covered by the modulated portion D and the upper superconductor portion S 2 . In the present invention, the laminated structure may, for example, be of a type S/I/S/I/S or S/N/S/I/S, and other known structure may be deposited on or under the thin film device. For example, in the research article by Mr. Kawai in ISTEC Journal 2 (3) 1989, p. 19, preparation of a super lattice structure by laser ablation is explained. However, the purpose of this research is to study the dimensional nature of a superconductor or to prepare a super lattice structure, and it is different in the structure from the preparation of the above mentioned hetero interface according to the present invention. Namely, in the present invention, such a technique for the preparation of a super lattice is utilized, but the present invention is based on the recognition that the substituted portion (interlayer) where a rare earth element or Cu in a YBCO type oxide superconductor, or an alkaline earth metal or Cu in a Bi type oxide superconductor, is substituted by other element, is present in the crystal structure with the original crystal structure maintained in a stabilized state, and on the knowledge that this substituted portion (interlayer) exhibits an insulating property or a normal conductivity property required for a Josephson junction. Heretofore, a S/I/S structure such as YBa 2 CuO 7 /(YPr)Ba 2 Cu 3 O 7 /YBa 2 Cu 3 O 7 has been studied. However, such a study is based on a conventional hetero deposited film and is not directed to the one formed by locally modulating the original composition of the YBCO type oxide superconductor film. Namely, a conventional crystal structure such as YBa 2 Cu 3 O 7 or Bi 2 Sr 2 CaCu 2 O 8-δ is stable within a wide temperature range from a very low temperature (4K) to a high temperature (∼600°C). However, a conventional hetero structure has been prepared by destroying such a stable structure across the interface between the oxide superconductor and said non-superconductor interlayer, and with such a conventional structure, control of the interface between layers of different types can not satisfactorily be conducted, and it has been difficult to prepare a thin film device having a thermodynamically stable structure and interface without disorder. Whereas, according to the present invention, the electrical properties substantially the same as the above mentioned conventional hetero structure can be obtained while maintaining the original stable crystal structure substantially completely, and the composition of the modulated portion employed can be present in the form of a stable film since the crystal structure of the modulated portion is thermodynamically stable like the oxide conductor as the basic composition. Therefore, according to the present invention, it is possible to obtain a thin film device which is free from the above mentioned conventional problems and which has a high operational temperature and excellent properties. Now, the present invention will be described in further detail with reference to Examples. However, it should be understood that the present invention is by no means restricted to such specific Examples. The feature of the present invention resides solely in the layer structure, and the following description will be directed solely to the layer structure. Figure 1(A) illustrates the basic structure of a YBCO type oxide superconductor film having a c-axis orientation, in which a basic cycle of BaO-CuO-BaO-CuO-Y-CuO is repeated. However, due to formation of defects, a part of this basic cycle may locally break. Shown in Figure 1(B) is an Example of the present invention relating to the above film having a c-axis orientation, which has such a structure that at an intermediate portion of the structure of Figure 1(A), Cu-O layers (Cu-O in the CuO plane in the Figure) are substituted by CuMO, so that a modulated portion is formed between two layers of CuMO as illustrated. This modulated portion is introduced so that the above basic cycle is maintained. Here, M may be an element of Group IIb in the Periodic Table such as Zn, an element of Group IIIb in the Periodic Table such as Al or Ga, or a transition element other than Cu, such as Cr, Fe, Co, Ni, Zr or Pt, and it is preferably an element having an ion radius which does not substantially differ from Cu. The length of the above modulated portion is usually required to be longer than the superconductor coherence length and not very much (e.g. ten times) longer than the coherence length. An oxide having a critical temperature Tc of at least the liquefied nitrogen temperature (77K) has an anisotropy, but typically, the coherence length is about 1nm (10Å) or less. Therefore, the length of the modulated portion is preferably within a range of from the minimum basic structural unit (c-axis length) to ten times the c-axis length, i.e. from 1 to 10 nm (10 to 100Å) for S/I/S structure. The superconductor layers above and below the modulated portion may usually be from 5 to 100 nm (50 to 1,000Å). Figure 1(C) illustrates another Example of the modulation of a film having a c-axis orientation. In this Example, not a CuO plane, but a CuO chain is substituted by CuMO. Figure 1(D) illustrates an Example wherein Y is substituted by YL where L is a rare earth element other than Y having a different valence, such as Ce 4+ or Pr 4+ . This substitution may be conducted by an alkaline earth metal such as Ca 2+ . Figure 2(A) illustrates the basic structure of a YBCO type oxide superconductor film having an a-orientation, wherein a basic cycle of YBaO-CuO is repeated. In a thin film device of the present invention, modulation is conducted so that this basic cycle is maintained. Namely, Figures 2(B) and (C) illustrate Examples of the present invention relating to this film having an a-axis orientation. The Example of Figure 2(B) has a structure wherein at an intermediate portion, CuO layers are substituted by CuMo, and a modulated portion is formed between two layers of CuMo. Figure 2(C) illustrates an Example wherein Y in Y-BaO layers is substituted by YL where L is a rare earth element other than Y. Figure 3(A) illustrates the basic structure of a Bi 2 Sr 2 CaCu 2 O 2n+4-δ film having a c-axis orientation, wherein a basic cycle of BiO-SrO-CuO-CaO-CuO-SrO-BiO is repeated. And, a thin film device of the present invention shown in Figure 3(B) has a structure in which a part of Cu is substituted by CuM, and a modulated portion is formed between two layers of CuMO (=Cu 1-x M y -O). In the Example shown in Figure 3(C), a part of Ca is substituted by Y, and a modulated portion is formed between two layers of CaY-O. In a case of an oxide superconductor of Tℓ-Ba-Ca-Cu-O type, the structure may be the same as that of Figures 3(A) to (C) where Bi is changed to Tℓ, and Sr is changed to Ba. Two or more of the above-described various manners for the substitution of elements, may be combined as the case requires. For example, in a case of an oxide superconductor film of YBCO type, the manners for substitution as illustrated in Figure 1(B) and Figure 1(C) may be combined simultaneously. Figure 5 illustrates an Example of a conventional hetero epitaxial growth in a thin film device composed of an oxide superconductor film of YBCO type. In the Figure, a hetero interface is formed between two BaO layers. Thus destroying the periodicity of structure of the oxide super conductor. EXAMPLE 1 An oxide superconductor film of YBCO type was formed by vapor deposition using electron beam and resistance heating source, on a SrTiO 3 (001) substrate in an atmosphere of an oxygen partial pressure of 3,99 x 10 -2 Pa (3 x 10 -4 torr), as follows. Namely, control of the thickness of each layer was conducted by adjusting the applied power and time while detecting the layer thickness by a crystal oscillation type layer thickness monitor. Firstly, a BaO layer was vapor-deposited on the substrate by opening and closing the shutter, then one layer of Cu was vapor-deposited thereon, and vapor deposition of BaO, Cu, Y 2 O 3 , Cu and BaO atomic monolayers was further conducted sequentially in this order. This vapor deposition was repeated 30 times to form a YBa 2 Cu 3 O x film. The substrate temperature was 700°C, and the vapor deposition rate of each layer was 1 nm/min (10Å/min). Thereafter, the film device was maintained under an oxygen partial pressure of 133.3 hPa (100 torr) for 5 hours, and then cooled to room temperature at a rate of 50°C/min. The obtained film showed zero resistance at 87K, and from the X-ray diffraction, it was found to be a film having an excellent c-axis orientation. Then, in the same manner as described above, a YBa 2 Cu 3 o x film composed of 30 lattices was prepared, and then using Co 0.5 Cu 0.5 instead of Cu, layer-forming by similar vapor deposition was repeated for five cycles to obtain a YBa(Cu 0.5 Co 0.5 ) 3 O x film. Then, using BaO, Y 2 O 3 and Cu again, vapor deposition for 20 lattices was repeated to obtain a YBa 2 Cu 3 O x film. This film was maintained under an oxygen partial pressure of 133.3 hPa (100 torr) for 5 hours in the same manner as described above, and then cooled to room temperature at a rate of 50°C/min. The resistance in the film surface of the film thus obtained was measured, whereby it was found that zero resistance was obtained at 87K. Further, from the X-ray diffraction, an excellent c-axis orientation was also confirmed. Thus, it is evident that Co did not diffuse into the superconducting portions at both sides and a thin film device having excellent properties was obtained. EXAMPLE 2 Under the same manner and the same conditions as in Example 1, YBa 2 CuO 7 , (Pr 0.5 Y 0.5 )Ba 2 CuO 7 obtained by changing Y in YBa 2 CuO 7 to (Pr 0.5 Y 0.5 ), and YBa 2 CuO 7 , were sequentially layer by layer deposited on a SrTiO 3 (001) substrate surface to obtain a thin film device of the present invention. This film was maintained under an oxygen partial pressure of 133.3 hPa (100 torr) for 5 hours in the same manner as in Example 1, and then cooled to room temperature at a rate of 50°C/min. The resistance in the film surface of the film thus obtained was measured, and the X-ray diffraction was analyzed, whereby it was found to be a thin film device having excellent properties like in Example 1. As described in the foregoing, according to the present invention, a thin film device having a high operational temperature and excellent properties can be prepared without any problems of the above mentioned conventional techniques.

Claims: A Josephson device comprising a substrate and an oxide superconductor film formed thereon, wherein said oxide superconductor film comprises atomic monolayers each composed of at least one kind of element of the oxide superconductor, which are deposited in a predetermined and periodic order substantially in a direction perpendicular to the substrate so that the lattice structure of the oxide superconductor is substantially maintained, and at an intermediate portion of the oxide superconductor film, at least a part of the atoms of the oxide superconductor is substituted by other element in the lattice structure of the oxide superconductor to form a non-superconductor interlayer, and the periodicity of the lattice structure of the oxide superconductor film is substantially maintained across the interface between the oxide superconductor and said non-superconductor interlayer. The device according to Claim 1, wherein said atomic monolayers are sequentially formed by vapor deposition. The device according to Claim 1, wherein the oxide superconductor film is an oxide superconductor film containing Cu-O. The device according to Claim 3, wherein the oxide superconductor film containing Cu-O is composed of LB 2 Cu 3 O 7-δ wherein L is a rare earth element, and B is an alkaline earth metal, TℓBa 2-n Ca n-1+x Cu n O 2n+1 wherein n is 1, 2 or 3, or Bi 2 Sr x Ca y Cu n O 2n+4 wherein n is 1, 2 or 3, and x + y ≃ n + 1. The device according to Claim 1, wherein a part or whole of Cu element in said non-superconductor interlayer is substituted by other element. The device according to Claim 5, wherein said other element is an element of Group IIb in the Periodic Table, an element of Group IIIb in the Periodic Table or a transition element other than Cu. The device according to Claim 1, wherein the oxide superconductor film is composed of LB 2 Cu 3 O 7-δ wherein L is a rare earth element, and B is an alkaline earth metal, and at said non-superconductor interlayer of the oxide superconductor film, a part or whole of L is substituted by other rare earth element or alkaline earth metal. The device according to Claim 1, wherein the oxide superconductor film is composed of TℓBa 2-n Ca n-1+x Cu n O 2n+1 wherein n is 1, 2 or 3, or Bi 2 Sr x Ca y Cu n O 2n+4 wherein n is 1, 2 or 3, and x + y ≃ n + 1, and at said non-superconductor interlayer of the oxide superconductor film, a part or whole of Ca is substituted by other alkaline earth metal or a trivalent rare earth metal. The device according to Claim 1, which is a Josephson device designed to conduct an electric current in the thickness direction of the superconductor film.

Inventors: WATANABE YUKIO, WATANABE, YUKIO
Applicants: MITSUBISHI CHEM CORP, MITSUBISHI CHEMICAL CORPORATION
Application year: 1991
Main classification: H01L39
IPC codes: H01L39