Superconducting wire

An example of a wire (V₃Ga alloy) used in a superconducting magnet.

Superconducting wire is wire made of superconductors. When cooled below its transition temperature, it has zero electrical resistance. Most commonly, conventional superconductors such as niobium-titanium are used,^[1] but high-Tc superconductors such as YBCO are entering the market. Superconducting wire's advantages over copper or aluminum include higher maximum current densities and zero power dissipation. Its disadvantages include the cost of refrigeration of the wires to superconducting temperatures (often requiring cryogens such as liquid helium or liquid nitrogen), the danger of the wire quenching (a sudden loss of superconductivity), the inferior mechanical properties of some superconductors, and the cost of wire materials and construction.^[2] Its main application is in superconducting magnets, which are used in scientific and medical equipment where high magnetic fields are necessary.

Important parameters of SC wires/tapes/conductors

The construction and operating temperature will typically be chosen to maximise:

• critical temperature T_c, below this temperature the wire becomes a superconductor
• critical current density J_c, maximum super-current a superconducting wire can carry per unit cross sectional area (see images below for examples with 20 kA/cm²).

LTS(Low Temperature Superconductor) Wire

LTS wires are made from superconductors with low critical temperature, such as Nb₃Sn(niobium-tin) and NbTi(niobium-titanium). Often the superconductor is in filament form in a copper or aluminium matrix which carries the current should the superconductor quench for any reason. The superconductor filaments can form a third of the total volume of the wire.

Preparation

Wire drawing

The normal wire drawing process can be used for malleable alloys such as niobium-titanium.

Surface diffusion

Vanadium-gallium (V₃) can be prepared by surface diffusion where the high temperature component as a solid is bathed in the other element as liquid or gas.^[3] When all components remain in the solid state during high temperature diffusion this is known as the Bronze Process.^[4]

• 

  Cross sections of various (Nb,Ti)₃Sn composite superconducting cables and wires. (440 to 7,800 Amps in 8 to 19 Tesla fields).

• 

  V₃Ga superconducting tape (10×0.14 mm cross section). A vanadium core is covered with 15 µm V₃Ga layer, then 20 µm bronze (stabilizing layer) and 15 µm insulating layer. Critical current 180 A (19.2 tesla, 4.2 K), critical current density 20 kA/cm²

• 

  Nb/Cu-7.5at%Sn-0.4at%Ti tape (9.5×1.8 mm cross section) originally developed for an 18.1 T magnet. Nb core: 361×348 packs of 5 µm dia. filaments. Critical current 1700 A (16 tesla, 4.2 K), critical current density 20 kA/cm²

HTS(High Temperature Superconductor) Wire

HTS wires are made from superconductors with high critical temperature(high-temperature superconductivity), such as YBCO and BSCCO.

Powder-in-tube

Simplified diagram of the PIT process

The powder-in-tube (PIT, or oxide powder in tube, OPIT) process is often used for making electrical conductors from brittle superconducting materials such as niobium-tin^[5] or magnesium diboride,^[6] and ceramic cuprate superconductors such as BSCCO.^[7][8] It has been used to form wires of the iron pnictides.^[9] (PIT is not used for YBCO (Yttrium barium copper oxide) as it does not have the weak layers required to generate adequate 'texture' (alignment) in the PIT process.)

This process is used because the high-temperature superconductors are too brittle for normal wire forming processes. The tubes are metal, often silver. Often the tubes are heated to react the mix of powders. Once reacted the tubes are sometimes flattened to form a tape-like conductor. The resulting wire is not as flexible as conventional metal wire, but is sufficient for many applications.

There are 'in situ' and 'ex situ' variants of the process, as well a 'double core' method that combines both.^[10]

Coated superconductor tape or wire

The coated superconductor tapes are known as second generation superconductor wires. These wires are in a form of a metal tape of about 10 mm width and about 100 micrometer thickness, coated with superconductor materials such as YBCO. Few years after the discovery of the High-temperature superconductivity materials such as the YBCO, it was demonstrated that epitaxial YBCO thin films grown on lattice matched single crystals such as magnesium oxide MgO, Strontium titanate (SrTiO3) and sapphire had high super critical current density of 1-4 MA/cm2.^[11][12] However to produce a long tape, lattice matched flexible material was needed. The YBCO films deposited directly on metal substrate materials exhibit poor superconducting properties. It was demonstrated that a c-axis oriented yttria stabilized zirconia (YSZ) intermediate layer on a metal substrate can yield YBCO films of higher quality which had still one to two orders less critical current density than that produced on the single crystal substrates.^[13][14]

The breakthrough came with the invention of ion beam-assisted deposition(IBAD) technique to produce of bi-axially aligned yttria-stabilized zirconia (YSZ) thin films on metal tapes.^[15] The bi-axial YSZ film acted as a lattice matched buffer layer for the epitaxial growth of the YBCO films on it. These YBCO films achieved critical current density of more than 1 MA/cm2. Other buffer layers such as Cerium oxide CeO2 and Magnesium oxide MgO were produced using the IBAD technique for the superconductor films.^[16][17][18]

Smooth substrates with roughness in the order of 1 nm are essential for the high quality superconductor films. Initially hastelloy substrates were electro polished to create a smoothed surface. Hastelloy is a nickel based alloy capable of withstanding temperatures up to 800C without melting or heavily oxidizing. Currently a coating technique known as “spin on glass” or “ solution deposition planarization” is used to smooth the substrate surface.^[19][20] Currently YBCO coated superconductor tapes capable carrying more than 500 A/cm at 77K and 1000 A/cm at 30K under high magnetic field has been demonstrated.^{[21][22][23][24]}

Chemical vapor deposition

CVD is used for YBCO coated tapes.

Hybrid physical-chemical vapor deposition

HPCVD can be used for thin-film magnesium diboride. (Bulk MgB₂ can be made by PIT or Reactive Mg Liquid Infiltration.)

See also

• Niobium-titanium – easier to handle
• Niobium-tin – difficult to handle
• YBCO
• BSCCO

References

1. "Characteristics of Superconducting Magnets". Superconductivity Basics. American Magnetics Inc. website. 2008. Retrieved 2008-10-11. External link in |publisher= (help)
2. "Superconducting wire breaks record". Physics World. Retrieved 2009-09-03.
3. "Elementary Pinning Force of Grain Boundaries in Supereonducting V3Ga Tapes". Bibcode:1986JaJAP..25L.792M. doi:10.1143/JJAP.25.L792.
4. Dew-Hughes, D. "Solid-state (bronze process) V3Ga from a V-Al alloy core". Bibcode:1978JAP....49..327D. doi:10.1063/1.324390.
5. Lindenhovius, J.L.H.; Hornsveld, E.M.; Den Ouden, A.; Wessel, W.A.J.; Ten Kate, H.H.J. (2000). "Powder-in-tube (PIT) Nb/sub 3/Sn conductors for high-field magnets". IEEE Transactions on Applied Superconductivity 10: 975. doi:10.1109/77.828394.
6. B. A. Glowacki, M. Majoros, M. E. Vickers, B. Zeimetz (2001). "Superconducting properties of the powder-in-tube Cu-Mg-B and Ag-Mg-B wires". arXiv:cond-mat/0109085.
7. Sheathed or Powder-in-Tube Conductors
8. Beales, Timothy P.; Jutson, Jo; Le Lay, Luc; Mölgg, Michelé (1997). "Comparison of the powder-in-tube processing properties of two (Bi2−xPbx)Sr2Ca2Cu 3O10+δpowders" (PDF). Journal of Materials Chemistry 7: 653. doi:10.1039/a606896k.
9. Y. Ma; et al. (2009). "Fabrication and characterization of iron pnictide wires and bulk materials through the powder-in-tube method". Physica C 469: 651–656. arXiv:0906.3114. Bibcode:2009PhyC..469..651M. doi:10.1016/j.physc.2009.03.024.
10. T. Nakane, K. Takahashia, H. Kitaguchia and H. Kumakuraa, T.; Takahashi, K.; Kitaguchi, H.; Kumakura, H. (2009). "Fabrication of Cu-sheathed MgB2 wire with high Jc–B performance using a mixture of in situ and ex situ PIT techniques". Physica C: Superconductivity 469: 1531–1535. Bibcode:2009PhyC..469.1531N. doi:10.1016/j.physc.2009.05.227.
11. Blue, C., & Boolchand, P. (1991). "Insitu preparation of superconducting Y1Ba2Cu3O7− δ thin films by on‐axis rf magnetron sputtering from a stoichiometric target". Applied physics letters 58: 2036. doi:10.1063/1.105005.
12. Savvides, N., & Katsaros, A. (1993). "Insitu growth of epitaxial YBa2Cu3O7 thin films by on‐axis unbalanced direct current magnetron sputtering". Applied physics letters 62: 528. doi:10.1063/1.108901.
13. Russo, R. E., Reade, R. P., McMillan, J. M., & Olsen, B. L. (1990). "Metal buffer layers and Y‐Ba‐Cu‐O thin films on Pt and stainless steel using pulsed laser deposition". Journal of Applied Physics 68: 1354. doi:10.1063/1.346681.
14. Reade, R. P., Berdahl, P., Russo, R. E., & Garrison, S. M. Laser (1992). "deposition of biaxially textured yttria‐stabilized zirconia buffer layers on polycrystalline metallic alloys for high critical current Y‐Ba‐Cu‐O thin films". Applied Physics Letters 61: 2231. doi:10.1063/1.108277.
15. Iijima, Y., Tanabe, N., Kohno, O., & Ikeno, Y. (1992). In‐plane aligned YBa2Cu3O7− x thin films deposited on polycrystalline metallic substrates. Applied Physics Letters, 60(6), 769-771.
16. Gnanarajan, S., Katsaros, A., & Savvides, N. (1997). Biaxially aligned buffer layers of cerium oxide, yttria stabilized zirconia, and their bilayers. Applied physics letters, 70(21), 2816-2818.
17. Wang, C. P., Do, K. B., Beasley, M. R., Geballe, T. H., & Hammond, R. H. (1997). Deposition of in-plane textured MgO on amorphous Si3N4 substrates by ion-beam-assisted deposition and comparisons with ion-beam-assisted deposited yttria-stabilized-zirconia. Applied Physics Letters, 71(20), 2955-2957.
18. Arendt, P. N., Foltyn, S. R., Civale, L., DePaula, R. F., Dowden, P. C., Groves, J. R., ... & Usov, I. (2004). High critical current YBCO coated conductors based on IBAD MgO. Physica C: Superconductivity, 412, 795-800.
19. Gnanarajan, S., & Du, J. (2005). Flexible Y Ba2Cu3O7− δ-coated superconductor tapes on non-metallic substrates with spin-on-glass and IBAD-YSZ buffer layers. Superconductor Science and Technology, 18(4), 381.
20. Sheehan, C., Jung, Y., Holesinger, T., Feldmann, D. M., Edney, C., Ihlefeld, J. F., ... & Matias, V. (2011). Solution deposition planarization of long-length flexible substrates. Applied Physics Letters, 98(7), 071907
21. Foltyn, S. R., Arendt, P. N., Dowden, P. C., DePaula, R. F., Groves, J. R., Coulter, J. Y., ... & Peterson, D. E. (1999). High-T/sub c/coated conductors-performance of meter-long YBCO/IBAD flexible tapes. Applied Superconductivity, IEEE Transactions on, 9(2), 1519-1522.
22. Usoskin, A., & Freyhardt, H. C. (2004). YBCO-coated conductors manufactured by high-rate pulsed laser deposition. Mrs Bulletin, 29(08), 583-589.
23. Pahlke, Patrick, Michael Hering, Max Sieger, Mayraluna Lao, Michael Eisterer, Alexander Usoskin, Jan Stromer, Bernhard Holzapfel, Ludwig Schultz, and Ruben Huhne. "Thick High YBCO Films on ABAD-YSZ Templates." Applied Superconductivity, IEEE Transactions on 25, no. 3 (2015): 1-4.
24. Selvamanickam, V., Gharahcheshmeh, M. H., Xu, A., Zhang, Y., & Galstyan, E. (2015). Critical current density above 15 MA cm− 2 at 30 K, 3 T in 2.2 μm thick heavily-doped (Gd, Y) Ba2Cu3Ox superconductor tapes. Superconductor Science and Technology, 28(7), 072002.