GB2249786A - Superconducting oxide materials - Google Patents

Superconducting oxide materials Download PDF

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Publication number
GB2249786A
GB2249786A GB9122495A GB9122495A GB2249786A GB 2249786 A GB2249786 A GB 2249786A GB 9122495 A GB9122495 A GB 9122495A GB 9122495 A GB9122495 A GB 9122495A GB 2249786 A GB2249786 A GB 2249786A
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ceramic oxide
addition
lithium
oxide material
intercalation
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GB9122495D0 (en
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William James Macklin
Patrick Timothy Moseley
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UK Atomic Energy Authority
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UK Atomic Energy Authority
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Priority claimed from GB909023799A external-priority patent/GB9023799D0/en
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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N60/00Superconducting devices
    • H10N60/80Constructional details
    • H10N60/85Superconducting active materials
    • H10N60/855Ceramic superconductors
    • H10N60/857Ceramic superconductors comprising copper oxide
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N60/00Superconducting devices
    • H10N60/01Manufacture or treatment
    • H10N60/0268Manufacture or treatment of devices comprising copper oxide

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  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Chemical & Material Sciences (AREA)
  • Ceramic Engineering (AREA)
  • Compositions Of Oxide Ceramics (AREA)

Abstract

The superconducting transition temperature (Tc) of a mixed oxide ceramic containing bismuth together with copper and one or more elements of Group 2 of the Periodic Table can be increased by electrochemical intercalation into the ceramic oxide of an alkali metal such as lithium, sodium, potassium, or of a proton (H<+>) or hydronium ion (H3O<+>).

Description

Oxide Materials This invention relates to ceramic oxide materials having a superconducting transition temperature above 10 K.
Since early 1986, certain families of ceramic oxide materials have been found to be superconductive at temperatures above the highest superconducting transition temperatures (Tc) known for metal alloys. One such family comprises material formulations based on ABxCuyOz and derivatives, where A is a metal in the oxidation state Ill and B is a metal in the oxidation state II. In an example of a member of such a family, A is bismuth and B is one or more elements of Group 2 of the Periodic Table such as strontium and calcium. Examples of such materials are given in International Patent Publication No. W089/07087.
It is also known that such materials may be doped with lead and further doping with small amounts of antimony can enhance the superconducting properties.
Our patent specification No. 2 232 664 describes the use of additions of one or more of indium, gallium and possibly arsenic in place of all or part of the lead or antimony or both in such materials.
Recent published reports have indicated that electrochemical intercalation of silver into the superconductor Bi2Sr2CaCu2O8+x enhanced Tc by about 15 K (G.A.
Scholz and F.W. Boswell, Solid State Communications, 74,959(1990)). A recent report has also referred to lithium doping by a high temperature reaction treatment of flexible whiskers of a superconducting oxide of bismuth, strontium, calcium and copper. This doping treatment was reported to be effective in raising Tc in both Bi2Sr2CaCu2O8+x and Bi2Sr2Ca2Cu3Ol0.
We have now found that Tc for superconducting oxide phases of bismuth, strontium, calcium and copper, including such phases with indium doping or lead doping, can be increased by the electrochemical intercalation of lithium or sodium into the materials. On theoretical grounds, it is anticipated that a similar result may be achieved by electrochemical intercalation of potassium, or protons (H+) or hydronium ions (H30+), but this has not yet been established by experiment.
In view of the similarity to these bismuth based materials in the structure of the thallium-based superconducting materials, such as, for example Tl2Ba2CaCu2Oy, it is to be expected that Tc of such thallium-based superconducting materials can also be increased by electrochemical intercalation of lithium.
However, no such effect has been positively demonstrated by experiments so far carried out.
The invention provides, in one of its aspects, a ceramic oxide material having a superconducting transition temperature above 10 K comprising a mixed oxide of bismuth, together with copper and one or more elements of Group 2 of the Periodic Table, and having an intercalation addition which has been electrochemically introduced into the ceramic oxide, and which addition comprises at least one of the alkali metals lithium, sodium, potassium, or protons (H+) or hydronium ions (H30+). Preferably, the one or more elements of Group 2 are strontium and calcium.
Preferably the bismuth based ceramic oxide contains an addition of an oxide or oxides of one or more of indium, gallium, arsenic, scandium, lead and antimony.
The invention provides, in another of its aspects, a method of manufacturing a ceramic oxide material having a superconducting transition temperature above 10 K which method comprises forming a homogeneous mixture by mixing together powders of oxides, or precursors of oxides, of bismuth, copper and one or more elements of Group 2 of the Periodic Table in relative proportions appropriate for those desired in the product mixed oxide phase, firing the mixture to form the said product, and electrochemically introducing into the said product an addition comprising at least one of the alkali metals lithium, sodium, potassium, or protons (H+) or hydronium ions (H30+).
Preferably the intercalation addition comprises lithium or sodium, and of these, lithium is the more preferable.
The electrochemical intercalation is conveniently carried out by galvanostatic discharge of an electrochemical cell having the said product as working electrode, a counter-electrode of the addition material and an electrolyte capable of conducting lithium ions.
Specific examples of materials and methods for their manufacture embodying the invention will now be described with reference to the drawings filed herewith in which: Figure 1 is a diagrammatic illustration of an electro-chemical cell, Figure 2 is a graph illustrating discharge curves for electrochemical cells as shown in Fig. 1 and containing respectively three superconducting ceramic oxide material samples.
Figures 3 - 5 are graphs showing the inductance against temperature for these three superconducting ceramic oxide material samples, and Figure 6 is a graph showing inductance against temperature for a further example of superconducting ceramic oxide material sample.
The three examples of superconducting ceramic oxide material identified in Figures 2 to 5 will first be described. In each case the homogeneous mixture was prepared from stoichiometric quantities of powdered Bi203, CuO, SrCO3 and CaCO3. For the second example including indium doping, powdered In203 was incorporated in the mix. Similarly for the third example incorporating lead, powdered PbO was incorporated in the mix. The mixture was then pressed into pellets for each example and sintered at 8600C for seventy hours. The sintering was carried out in air for the undoped example and for that containing indium, but was carried out in an atmosphere of argon and oxygen for the material doped with lead.
At this stage, measurements were made on the product materials and these are discussed more fully below.
Intercalation of lithium into the superconducting ceramic oxide materials prepared as described above was carried out by galvanostatic discharge of electrochemical cells containing the superconductor material as working electrode 11, a lithium counter electrode 12 and a lithium ion conducting electrolyte. These components are shown in Fig. 1 which is a teflon cell 13 having two terminals 14, 15 configuration in which the working electrode 11 and counter electrode 12 are separated by pads 16 of Whatman filter paper soaked in electrolyte. The electrolyte comprised a 1M LiC104 solution in propylene carbonate.
In each case, the cell was assembled in a dry room held at a temperature of 20 C, the dew point temperature being -30 C.
In each example, the cell was discharged at room temperature to a voltage of 1.OV, using a microprocessor controlled multi-channel galvanostat. The current densities were typically of the order of 0.1 mA cm~2. The mole fraction of the intercalated lithium in the superconducting phase was calculated from the capacity obtained on the discharge together with the weight of the pellet. After discharge, each cell was dismantled and the electrolyte removed from the pellet surface.
The respective electrochemical cell discharge curves for each of the sample pellets of superconducting ceramic oxide are shown in Fig. 2. The code is as follows: 2212 for Bi2Sr2CaCu2O8+x In-2212 for Bi1 .91n0 .1Sr2CaCu2O8+x Pb-2223 for Bi1#84Pb0#34Sr2Ca2Cu3O10 Although the open circuit voltages on assembly of the electrochemical cells were in the region 3.43V to 3.53V there is no significant capacity at these high voltages and the discharge voltage rapidly falls below 2V in each case. The discharge curves for the indium and lead doped samples decrease monotonously with lithium insertion, this being indicative of a single phase reaction. The discharge curve for the Bi2Sr2CaCu2O8+x material has a short step at about 1.4 volts that may be associated with a two- phase region in the intercalation process. The final compositions based on the quantity of charge passed were as follows: Li0 .l6Bi2Sr2CaCu2O8+x Lio . 23bit 91n0 lSr2Cacu2og+x Lio . 19Bi1 . 84PbO . 34Sr2Ca2Cu30l0 The lattice parameters for the tetragonal host oxide materials and the corresponding lithiated phases were derived from X-ray diffraction patterns using a Siemens D500 diffractometer and the results are given as follows in Table 1:: TABLE 1 Bi2Sr2CaCuO8+x a=3.824(2), c=30.724(25) Li0.16Bi2Sr2CaCu2O8+x a=3.835(11), c=30.911(94) Bi1,9In0.1Sr2CaCu208+x a=5.439(5),c=30.818(43) Li0.23Bil.9In0.1Sr2CaCU-2 s+x a=5.453(12) , c=30.867(97) Bi1.84Pb0.34Sr2Ca2Cu3O10 a=5.437(8), c=37.292(85) Li0.19Bi1.84PS0.34Sr2Ca2Cu3010 a=5.439(13), c=37.373(134) In each case it can be seen that the introduction of lithium results in an expansion in the c lattice parameter.
However, lithiation results in line broadening in the X-ray diffraction pattern that makes the determination of accurate lattice parameters difficult. This is reflected in the greater standard deviations (indicated in parenthesis) for the lithiated phases. The standard deviations are largest in the lithiated super-conducting ceramic oxide phases that contain the additional dopant ion (indium or lead). This type of anisotropic lattice expansion on intercalation is a feature of. layered materials, and is consistent with the lithium ions occupying the space between the segregated copper-oxygen layers in the perovskite structure.
Inductance measurements were made on the sample pellets by measuring the self-inductance of a transversely wound coil adjacent to the sample, using a Hewlett Packard 4274A LCR meter. The sample probe was lowered down the temperature gradient set up above the surface of liquid helium. The temperature gradient was approximately 10K per mm depending on the level of liquid in the dewar. For these routine measurements, the magnetic flux density produced by the coil was less than 10-4 Tesla.
The results of these measurements of inductance against temperature are shown in Figs. 3, 4, 5. The measurements were made on each sample both before (curves (a)) and after (curves (b)) lithiation. The respective curves are readily distinguishable in that the curves (a) for the material before lithiation exhibit a sharp downturn in inductance at the critical temperature whereas the curves (b) for the lithiated material show a more gradual decrease in inductance with decreasing temperature.The data shown in the figures relates to the materials in each case before and after lithiation as follows: Fig. 3 - Bi2Sr2CaCu2O8+x Fig. 4 - Bi1.9In0.1Sr2CaCu2OB+x Fig. 5 - Bil#84Pb0#34Sr2Ca2Cu3010 It will be noted that in Fig. 4 the intercalation of lithium has resulted in a significant increase of about 150K in the temperature at which onset of superconductivity is evident. It was noted that in all the samples there appeared to be a decrease in the volume of the superconducting phase as a result of intercalating lithium.
This may be because the method used to introduce lithium into the starting material was not producing a homogeneous modification. For example it is possible that grain surfaces might accept more lithium than the bulk material.
In a modification of the method above described, a lithium polymer solid electrolyte based on a modified polyethylene oxide electrolyte was used in the electrochemical cell. The sample before lithiation had the composition: Bi1,7In0.3Sr2CaCu208+, A lower level of lithiation (about 4%) was achieved, yielding: Li0 .O4Bil .71n0 .3Sr2CaCu208+x The increase in Tc was about 5 K, and with a much smaller reduction in the superconducting volume, as is apparent from Figure 6.
In an example for the electrochemical intercalation of sodium, instead of lithium, into a bismuth based superconducting ceramic material, the apparatus and procedures were as described with reference to Figure 1, except that the electrolyte comprised a 1 molar solution of NaC104 in propylene carbonate, and the counter-electrode was sodium metal. After passage of 5 mole % of sodium into the superconducting ceramic material, the Tc had increased from 100 K to 105 K.
For intercalation of hydrogen into such superconducting ceramic oxide starting material, it is envisaged that the electrochemical cell would comprise the ceramic oxide as working electrode, a hydrogen or hydride counter electrode 12 and a proton conducting electrolyte such as 1M HC104 solution in propylene carbonate.
The invention is not restricted to the details of the foregoing examples. For instance the selected alkali metal need not necessarily be introduced electrochemically on its own into the ceramic oxide, but may be introduced in combination with one or more other alkali metals.

Claims (9)

Claims
1. A ceramic oxide material having a superconducting transition temperature above 10 K comprising a mixed oxide of bismuth, together with copper and one or more elements of Group 2 of the Periodic Table, and having an intercalation addition which has been electrochemically introduced into the ceramic oxide, and which addition comprises at least one of the alkali metals lithium, sodium potassium, or protons (H+) or hydronium ions (H30+).
2. A ceramic oxide material as claimed in Claim 1, wherein the said one or more elements of Group 2 are strontium and calcium.
3. A ceramic oxide material as claimed in Claim 1 or Claim 2, containing an addition of an oxide or oxides of one or more of indium, gallium, arsenic, scandium, lead and antimony.
4. A ceramic oxide material as claimed in any of Claims 1 to 3, wherein the addition comprises lithium and/or sodium.
5. A ceramic oxide material as claimed in any of Claims. l to 3, wherein the intercalation addition comprises lithium.
6. A method of manufacturing a ceramic oxide material having a superconducting transition temperature above 10 K which method comprises forming a homogeneous mixture by mixing together powders of oxides, or precursors of oxides, of bismuth, copper and one or more elements of Group 2 of the Periodic Table in relative proportions appropriate for those desired in the product mixed oxide phase, firing the mixture to form the said product, and electrochemically introducing into the said product an addition comprising at least one of the alkali metals lithium, sodium, potassium, or protons (H+) or hydronium ions (H30+).
7. A method as claimed in Claim 4, wherein the electrochemical intercalation is conveniently carried out by galvanostatic discharge of an electrochemical cell having the said product as working electrode, a counter-electrode of the addition material and an electrolyte capable of conducting ions of the addition material.
8. A ceramic oxide substantially as herein described in any one of the examples.
9. A method of manufacturing a ceramic oxide material as herein described in any one of the examples and with reference to Figure 1 of the drawings filed herewith.
GB9122495A 1990-11-01 1991-10-23 Superconducting oxide materials Withdrawn GB2249786A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1994020991A1 (en) * 1993-03-08 1994-09-15 International Business Machines Corporation Method and apparatus for doping a solid material

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2232664A (en) * 1989-06-17 1990-12-19 Atomic Energy Authority Uk Oxide materials

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2232664A (en) * 1989-06-17 1990-12-19 Atomic Energy Authority Uk Oxide materials

Non-Patent Citations (5)

* Cited by examiner, † Cited by third party
Title
J.Electrochem.Soc.Vol.136,No.8,August 1989,pages 2300-2305 *
Physica C Vol.172, No.3-4,15 Dec.1990, pages 193-8 *
Physica C Vol.173, No.3-4,1 Feb.1991, pages 220-6 *
Physica C Vol.180, No.5-6,15 Sept.1991, pages 387-93 *
Solid State Communications,Vol.74,No.9,June 1990, pages 959-60 *

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1994020991A1 (en) * 1993-03-08 1994-09-15 International Business Machines Corporation Method and apparatus for doping a solid material

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