WO1990001461A1

WO1990001461A1 - Superconducting metal oxide compositions and processes for manufacture and use

Info

Publication number: WO1990001461A1
Application number: PCT/US1989/003017
Authority: WO
Inventors: Munirpallam Appadorai Subramanian
Original assignee: EI Du Pont de Nemours and Co
Current assignee: EIDP Inc
Priority date: 1988-08-10
Filing date: 1989-07-17
Publication date: 1990-02-22
Anticipated expiration: 1991-02-10
Also published as: DK15491D0; EP0428630A1; DK15491A; EP0428630B1; AU4349789A; AU632069B2; NO303007B1; DE68909945T2; EP0428630A4; JPH04500062A; NO910514D0; NO910514L; DK175209B1; DE68909945D1; JP2768523B2

Abstract

Compositions having the nominal formula Tle Pba Cab Src Cud Ox wherein a is from about 1/10 to 3/2, b is from about 1 to 4, c is from about 1 to 3, d is from about 1 to 5, e is from about 3/10 to 1, x = (a + b + c + d + e + y) where y is from about 1/2 to 3, are superconducting. Processes for manufacturing such compositions and for using them are disclosed.

Description

SUPERCONDUCTING METAL OXIDE COMPOSITIONS AND PROCESSES FOR MANUFACTURE AND USE

BACKGROUND OF THE INVENTION

Cross Reference to Related Application

This application is a continuation-in- part of U. S. Patent Application Serial No.

07/230,631 . (Docket No. CR-8679) filed

August 10, 1988.

Field of the Invention

This invention relates to novel Tl-Pb-Ca-Sr-Cu-0 compositions which are superconducting.

References

Bednorz and Muller, Z. Phys. B64, 189 (1986), disclose a superconducting phase in the La-Ba-Cu-O system with a superconducting transition temperature of about 35 K. This disclosure was subsequently confirmed by a number of investigators [see, for example, Rao and Ganguly, Current Science, 56, 47 (1987), Chu et al., Science 235, 567 (1987), Chu et al., Phys. Rev. Lett. 58, 405.(1987), Cava et al. , Phys. Rev. Lett. 58, 408 (1987), Bednorz et al., Europhys. Lett. 3, 379 (1987)]. The superconducting phase has been identified as the composition La₁__χ (Ba,Sr,Ca)_χCu0₄__y with the tetragonal K₂NiF₄-type structure and with x typically about 0.15 and y indicating oxygen vacancies. u e a ., ys. ev. e . , (1987), disclose a superconducting phase in the Y-Ba-Cu-0 system with a superconducting transition temperature of about 90 K. Cava et al., Phys. Rev. Lett. 58, 1676 (1987), have identified this superconducting Y-Ba-Cu-0 phase to be orthorhombic, distorted, oxygen-deficient perovskite YBa₂Cu₃0₉__s where δ is about 2.1 and present the powder x-ray diffraction pattern and lattice parameters.

C. Michel et. al., Z. Phys. B - Condensed Matter 68, 421 (1987), disclose a novel family of superconducting oxides in the Bi-Sr-Cu-0 system with composition close to Bi₂Sr₂Cu₂0₇₊₆. A pure phase was isolated for the composition Bi₂Sr₂Cu₂0_7+δ . The X-ray diffraction pattern for this material exhibits some similarity with that of perovskite and the electron diffraction pattern shows the perovskite subcell with the orthorhombic cell parameters of a - 5.32 A (0.532 n ), b •= 26.6 A (2.66 nm) and c - 48.8 A (4.88 nm) . The material made from ultrapure oxides has a superconducting transition with a midpoint of 22 K as determined from resistivity measurements and zero resistance below 14 K. The material made from commercial grade oxides has a superconducting transition with a midpoint of 7 K.

H. Maeda et al., Jpn. J. Appl. Phys. 27, L209 (1988), disclose a superconducting oxide in the Bi-Sr-Ca-Cu-0 system with the composition near BiSrCaCu₂Ox and a superconducting transition temperature of about 105 K.

The commonly assigned application, "Superconducting Metal Oxide Compositions and Process For Making Them", S. N. 153,107, filed 152,186, filed Feb. 4, 1988, disclose superconducting compositions having the nominal formula BiaSr b. CacCu3,0x wherein a is from about 1 to about 3, b is from about 3/8 to about 4, c is from about 3/16 to about 2 and x - (1.5 a + b + c + y) where y is from about 2 to about 5, with the proviso that b + c is from about 3/2 to about 5, said compositions having superconducting transition temperatures of about 70 K or higher. It also discloses the superconducting metal oxide phase having the formula Bi.Sr, .Ca.Cu,0. __ wherein z is from about 0.1 to about 0.9, preferably 0.4 to 0.8 and w is greater than zero but less than about 1.. M. A. Subramanian et al.. Science 239, 1015 (1988) also disclose the Bi.Sr, .Ca Cu,0,_^„ superconductor.

Y. Yumada et al., Jpn. J. Appl. Phys. 27, L996 (1988), disclose the substitution of Pb for Bi in the series Bi₁__χPb_χSrCaCu₂0 where x - 0, 0.1, 0.3, 0.5, 0.7, 0.9 and 1.0. The T_c increases from 75.5 K for x - 0, no Pb present, to a maximum of 85.5 K for x - 0.5. T C decreases for higher Pb content to 76 K for x «= 0.7. No superconductivity was observed for the samples with x = 0.9 and x * 1.

M. Takano et al., Jpn. J. Appl. Phys. 27, L1041 (1988), disclose that partial substitution of Pb for Bi in the Bi-Sr-Ca-Cu-0 system results in an increase in the volume fraction of the high T_c phase. Coprecipitated oxalates containing the relevant ions in various ratios underwent thermal decomposition below 773 K. The samples in powder form were then heated in air to 1073 K for 12 hours and, after being formed into pellets, at 1118 K for various periods which exten e to more than 240 hours in some cases. A starting composition of Bi:Pb:Sr:Ca:Cu « 0.7:0.3:1:1:1:8 was heated at 1118 K for 244 hours. The high-T_c phase shows an onset of superconductivity at around 115 K. .This phase forms plate-like crystals and analysis of these crystals indicates that^' the cationic ratio is Bi:Pb:Sr:Ca:Cu - 67:5:100:85:180 so that there is considerably less Pb in the high-T_c than in the starting material.

M. Mizuno et al., Jpn. J. Appl. Phys. 27, L1225 (1988), also disclose that the addition of Pb to the Bi-Sr-Ca-Cu-0 system results in an increase in the volume fraction of the high-T_c phase and a lowering of the optimum temperature to obtain this phase to about 855°C.

E. V. Sampathkumaran et al. , J. Phys. F: Met. Phys. 18, L163 (1988) disclose that the partial substitution of K or Pb for Bi in the Bi 4.Ca3, Sr,3Cu4.O4. results in an enhancement of the fraction of the phase superconducting at about 110 K.

Z. Z. Sheng et al., Nature 332, 55 (1988) disclose superconductivity in the Tl-Ba-Cu-0 system in samples which have nominal compositions Tl₂Ba₂Cu₃0_8+χ and TlBaCu₃0_{5 5+χ} . Both samples are reported to have onset temperatures above 90 K and zero resistance at 81 K. The samples were prepared by mixing and grinding appropriate amounts of BaC0₃ and CuO with an agate mortar and pestle. This mixture was heated in air at 925°C for more than 24 hours with several intermediate grindings to obtain a uniform black oxide Ba-Cu oxide powder which was mixed with an appropriate amount of Tl₂0₃, completely ground and pressed into a pellet with - . The pellet was then put into a tube furnace which had been heated to 880-910°C and was heated for 2-5 minutes in flowing oxygen. As soon as it had slightly melted, the sample was taken from the furnace and quenched in air to room temperature. It was noted by visual inspection that Tl₂0₃ had partially volatilized as black smoke, part had become a light yellow liquid, and part had reacted with Ba-Cu oxide forming a black, partially melted, porous material.

Z. Z. Sheng et al.. Nature 332, 138 (1988) disclose superconductivity in the Tl-Ca-Ba-Cu-0 system in samples which have nominal compositions Tl₂Ca₂BaCu₃0_9+χ .

R. M. Hazen et al., Phys. Rev. Lett. 60, 1657 (1988), disclose two superconducting phases in the Tl-Ba-Ca-Cu-0 system, Tl₂Ba₂Ca₂Cu₃0_{: 0} and Tl₂Ba₂CaCu₂0₈.

SUMMARY OF THE INVENTION

This invention provides novel superconducting compositions having the nominal formula Tl •PbaCa. SrcCuα.Ox wherein a is from about

1/10 to about 3/2, b is from about 1 to about 4, c is from about 1 to about 3, d is from about 1 to about 5, e is from about 3/10 to about 1 and x - (a + b + c + d + e + y) where y is from about 1/2 to about 3. Preferably, the sum of a+e is about 1, b is about 2 , c is about 2 , d is from about 3 to about 4 and y is from about 1/2 to about 2. The onset of superconductivity for these compositions is at least 70 K. This invention includes novel superconducting compositions having the nominal formula TlPbaCa D. SrcCUα.Ox wherein a is from about , o a ou , c is from about 1 to about 3, d is from about 1 to about 5 and x « (a + b + c + d + y) where y is from about 1/2 to about 3. Preferably, a is about 1, b is from about 1 to about 2, c is about 1, d is from about 3 to about 4 and y is from about 1/2 to about 2. The onset of superconductivity for these compositions is at least 70 K.

These superconducting compositions are prepared by heating a mixture of the Tl, Pb, Ca, Sr and Cu oxides, the relative amounts chosen so that the atomic ratio Tl:Pb:Ca:Sr:Cu is e:a:b:c:d, at a temperature of about 850^βC to about 940°C, preferably about 860°C to about 925°C for about -3 to 12 hours in a confined atmosphere, e. g., in a sealed tube made of a non-reacting metal such as gold which prevents any of the reactants including the metals and oxygen from escaping.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a plot of the flux excluded by a composition of this invention as a function of temperature.

DETAILED DESCRIPTION OF THE INVENTION The superconducting compositions of this invention are prepared by the following process. Quantities of the oxide reactants Tl₂0₃, Pb0₂ , Ca0₂ , Sr0₂ and CuO are chosen with the atomic ratio of Tl:Pb:Ca:Sr:Cu of e:a:b:c:d wherein a is from about 1/10 to about 3/2, b is from about 1 to about 4, c is from about 1 to about 3, d is from about 1 to about 5, e is from about 3/10 to about 1, and mixed, for example, by powder may then be heated directly or it can be first formed into a pellet or other shaped object and then heated. The superconducting composition of this invention is produced only when the atmosphere in which the reactants are heated is carefully controlled. One way to accomplish this controlled atmosphere is to place the reactants in a tube made of a non-reacting metal such as gold and then sealing the tube by welding. The sealed tube is then placed in a furnace and heated to about 850°C to about 940^βC for about 3 to 12 hours. The power to the furnace is then turned off and the tube is furnace-cooled to ambient temperature, about 20°C, and then removed from the furnace. The tube is then opened and the black product recovered. The compositions prepared in this manner exhibit the onset of superconductivity above 70 K.

Two superconducting phases have been identified in these superconducting compositions. One phase, the "12 Angstrom phase", has an onset of superconductivity of about 85 K and lattice parameters of a = 0.380 nm and c = 1.21 nm as determined from X-ray powder diffraction results indexed on a tetragonal cell and the other phase, the "15 Angstrom phase", has an onset of superconductivity of about 120 K and lattice parameters of a = 0.380 nm and c - 1.52 nm as determined from X-ray powder diffraction results indexed on a tetragonal cell.

Superconductivity can be confirmed by observing magnetic flux exclusion, i.e., the Meissner effect. This effect can be measured by the method described in an article by E. Polturak an . s er n ys ca ev ew , , 5586(1987).

The superconducting compositions of this invention can be used to conduct current extremely efficiently or to provide a magnetic field for magnetic imaging for medical purposes. Thus, by cooling the composition in the form of a wire or bar to a temperature below the superconducting transition temperature, (T_c ) by exposing the material to liquid nitrogen if T. is above 77K or to liquid, helium if T_c is below 77K in a manner well known to those in this field; and initiating a flow of electrical current, one can obtain such flow without any electrical resistive losses. To provide exceptionally high magnetic fields with minimal power losses, the wire mentioned previously could be wound to form a coil which would be exposed to liquid helium or liquid nitrogen, depending on T_c before inducing any current into the coil. Such fields can be used to levitate objects as large as railroad cars. These superconducting compositions are also useful in Josephson devices such as SQUIDS (superconducting quantum interference devices) and in instruments that are based on the Josephson effect such as high speed sampling circuits and voltage standards.

EXAMPLES OF THE INVENTION EXAMPLE 1 2.2837 g of Tl₂0₃ , 2.3919 g of Pb0₂ , 0.7208 g of Ca0₂ , 1.1962 g of Sr0₂ and 0.7954 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 1:1:1:1:1, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed into a gold tube (3/8" dia and 4" long) and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5°C per minute to 875°C and then held at 875°_C for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to room temperature in the furnace. The tube was then removed from the furnace and cut open. The black product was recovered.

Meissner effect measurements showed the onset of superconductivity at about 75 K.

EXAMPLE 2

Two other pellets of the mixed powder of Example 1 were treated as described in Example 1 except that the temperature to which they were heated and held was 925°C.

Meissner effect measurements showed the onset of superconductivity at about 70 K.

EXAMPLE 3 2.2837 g of Tl₂0₃, 2.3919 g of Pb0₂ , 1.1416 g of Ca0₂ , 1.1962 g of Sr0₂ and 2.3862 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 1:1:2:1:3, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed from this mixed powder. Two pellets were loaded into a gold tube (3/8" dia and 4" long) and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5^βC per minute to 875^βC and then held at 875^βC for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to room temperature in the furnace. The tube was then . product was recovered.

Meissner effect measurements showed the onset of superconductivity at about 80 K.

EXAMPLE 4

Two other pellets of the mixed powder of Example 3 were treated as described in Example 3 except that the temperature to which they were heated and held was 925°C.

Meissner effect measurements were carried out and the results are shown in Fig. 1 where the flux exclusion is plotted as a function of temperature. The plot shows the onset of superconductivity at about 110 K.

The X-ray powder diffraction of the product shows that the dominant phase is the 15 Angstrom phase.

EXAMPLE 5

2.2837 g of Tl₂0₃, 2.3919 g of Pb0₂ , 0.7208 g of Ca0₂ , 1.1962 g of Sr0₂ and 2.3862 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 1:1:1:1:3, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed from this mixed powder. Two pellets were loaded into a gold tube (3/8" dia and 4" long) and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5°C per minute to 875°C and then held at 875^βC for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to room temperature in the furnace. The tube was then removed from the furnace and cut open. The black product was recovered.

Meissner effect measurements showed the onset of superconductivity at about 85 K. product shows that the dominant phase is the 12

Angstrom phase.

EXAMPLE 6

Two other pellets of the mixed powder of Example 5 were treated as described in Example 5 except that the temperature to which they were heated and held was 925°C.

Meissner effect measurements showed the onset of superconductivity at about 120 K.

EXAMPLE 7

2.2837 g of Tl₂0₃, 2.3919 g of Pb0₂ , 0.7208 g of Ca0₂ , 1.1962 g of Sr0₂ and 1.5908 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 1:1:1:1:2, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed from this mixed powder. Two pellets were loaded into a gold tube (3/8" dia and 4" long) and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5°C per minute to 875°C and then held at 875^βC for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to room temperature in the furnace. The tube was then removed from the furnace and cut open. The black product was recovered.

Meissner- effect measurements showed the onset of superconductivity at about 80 K.

The X-ray powder diffraction of the product shows that the dominant phase is the 12 Angstrom phase. Two other pellets of the mixed powder of Example 7 were treated as described in Example 7 except that the temperature to which they were heated and held was 925°C.

Meissner effect measurements showed the onset of superconductivity at about 85 K.

The X-ray powder diffraction of the product shows that the dominant phase is the 12 Angstrom phase.

EXAMPLE 9

2.2837 g of l₂0₃ , 2.3919 g of Pb0₂ , 0.7208 g of Ca0₂ , 2.3924 g of Sr0₂ and 2.3862 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 1:1:1:2:3, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed from this mixed powder. Two pellets were loaded into a gold tube (3/8" dia and 4" long) and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5°C per minute to 860°C and then held at 860°C for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to room temperature in the furnace. The tube was then removed from the furnace and cut open. The black product was recovered.

EXAMPLE 10 Two other pellets of the mixed powder of Example 9 were treated as described in Example 9 except that the temperature to which they were heated and held was 890^βC. onset of superconductivity at about 80 K.

EXAMPLES 11

0.6851 g of Tl₂0₃, 1.6743 g of Pb0₂ , 1.4416 g of Ca0₂ , 2.3924 g of Sr0₂ and 2.3862 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 3/10:7/10:2:2:3, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed from this, mixed powder. Two pellets were loaded into a gold tube (3/8" dia and 4" long) and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5^βC per minute to 900^βC and then held at 900^CC for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to room temperature in the furnace. The tube was then removed from the furnace and cut open. The black product was recovered.

Meissner effect measurements showed the onset of superconductivity at about 120 R.

The X-ray powder diffraction of the product is essentially the same as that shown in Example 12.

EXAMPLES 12

1.1419 g of Tl₂0₃, 1.1960 g of Pb0₂ , 1.4416 g of Ca0₂ , 2.3924 g of Sr0₂ and 2.3862 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 1/2:1/2:2:2:3, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed from this mixed powder. Two pellets were loaded into a gold tube (3/8" dia and 4" long) and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5°C per minute to 900^βC and then held at 900°C for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to .room temperature in the furnace. The tube was then removed from the furnace and cut open. The black product was recovered.

The d-spacings, the relative intensities and the indices of the observed reflections of the X-ray powder diffraction pattern of the product, which was essentially single phase, is shown in Table I. This is the characteristic pattern of the 15 Angstrom phase.

w - weak m - medium ε - strong

EXAMPLES

1.5986 g of Tl₂0₃ , 0.6696 g of Pb0₂ , 1.4416 g of Ca0₂ , 2.3924 g of Sr0₂ and 2.3862 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 7/10:3/10:2:2:3, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed from this mixed powder. Two pellets were loaded into a gold tube (3/8" dia and 4" long), and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5°C per minute to 900°C and then held at 900°C for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to room temperature in the furnace. The tube was then removed from the furnace and cut open. The black product was recovered.

Meissner effect measurements showed the onset of superconductivity at about 110 K.

EXAMPLES 14

2.0553 g of Tl₂0₃ , 0.22319 g of Pb0₂ , 1.4416 g of Ca0₂ , 2.3924 g of Sr0₂ and 2.3862 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 9/10:1/10:2:2:3, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed from this mixed powder. Two pellets were loaded into a gold tube (3/8" dia and 4" long) and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5°C per minute to 900°C and then held at 900°C for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to room . removed from the furnace and cut open. The black product was recovered.

Meissner effect measurements showed the onset of weak superconductivity at about 85 K.

The X-ray powder diffraction of the product showed the presence of a minor amount of the 12 Angstrom phase.

EXAMPLES 15

2.2838 g of Tl₂0₃ , 1.1960 g of Pb0₂ , 1.1412 g of Ca0₂ , 2.3924 g of Sr0₂ and 2.3862 g of CuO, corresponding to a Tl:Pb:Ca:Sr:Cu atomic ratio of 1:1/2:3/2:2:3, were ground together in an agate mortar for about 30 minutes. Pellets, 10 mm in diameter and about 3 mm thick, were pressed from this mixed powder. Two pellets were loaded into a gold tube (3/8" dia and 4" long) and the tube was sealed by welding both ends. The tube was placed in a furnace and heated at a rate of 5°C per minute to 900^βC and then held at 900^βC for 6 hours. Power to the furnace was then shut off and the tube was allowed to cool to room temperature in the furnace. The tube was then removed from the furnace and cut open. The black product was recovered.

Meissner effect measurements showed two superconductivity transitions, one at about 116 K and one at about 80 K.

The X-ray powder diffraction pattern of the product showed the presence of both the 12 and the 15 Angstrom phases.

Claims

The Invention Being Claimed is:

1. A superconducting composition having the nominal formula

wherein a is from about 1/10 to 3/2, b is from about^* 1 to A , c is from about 1 to 3 d is from about 1 to 5 e is from about 3/10 to 1 x « (a + b + c + d + e + y) where y is from about 1/2 to 3, said composition having a superconducting transition temperature of at least 70 K.

2. A superconducting composition as in Claim 1 wherein "a" is about 1/2, "b" is about 2, "c" is about 2, "d" is from about 3 to 4, "e" is about 1/2 and "y" is from about 1/2 to 2.

3. A superconducting composition as in Claim 1 wherein "a" is about 7/10, "b" and "c" are each equal to 2, "d" is about 3, "e" is about 3/10 and "y" is from about 1/2 to 2.

4. A process for making superconducting compositions consisting essentially of mixing stoichiometric quantities of oxides of Tl, Pb, Ca, Sr and Cu to provide the composition of Claim 1; heating the mixture in a confined atmosphere to a temperature of about 850°C to 940°C and maintaining said temperature for about 3 to 12 hours to form said composition; and cooling said composition.

5. A process as in Claim 4 wherein the stoichiometric quantities of the oxides or oxide precursors are selected to provide the composition of Claim 2. electrical current within a conductor material without electrical resistive losses comprising the steps of: cooling a conductor material composed of a composition of Claim 1 to a temperature below the T_c of said composition; initiating a flow of electrical current within said conductor material while maintaining said material below said temperature.

7. An improved Josephεon-effeet device wherein the superconductive material comprises the composition of Claim 1.