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Cuprate superconductor

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Cuprate superconductors are a family of high-temperature superconducting materials made of layers of copper oxides (CuO2) alternating with layers of other metal oxides, which act as charge reservoirs. At ambient pressure, cuprate superconductors are the highest temperature superconductors known. However, the mechanism by which superconductivity occurs is still not understood.

History

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Superconductor timeline. Cuprates are displayed as blue diamonds, magnesium diboride and other BCS superconductors are displayed as green circles, and iron-based superconductors as yellow squares. Cuprates are currently the highest temperature superconductors which are suitable for wires and magnets.

The first cuprate superconductor was found in 1986 in the non-stoichiometric cuprate lanthanum barium copper oxide by IBM researchers Georg Bednorz and Karl Alex Müller. The critical temperature for this material was 35K, well above the previous record of 23 K.[1] The discovery led to a sharp increase in research on the cuprates, resulting in thousands of publications between 1986 and 2001.[2] Bednorz and Müller were awarded the Nobel Prize in Physics in 1987, only a year after their discovery.[3]

From 1986, many cuprate superconductors were identified, and can be put into three groups on a phase diagram critical temperature vs. oxygen hole content and copper hole content:

Structure

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The unit cell of high-temperature cuprate superconductor BSCCO-2212

Cuprates are layered materials, consisting of superconducting planes of copper oxide, separated by layers containing ions such as lanthanum, barium, strontium, which act as a charge reservoir, doping electrons or holes into the copper-oxide planes. Thus the structure is described as a superlattice of superconducting CuO2 layers separated by spacer layers, resulting in a structure often closely related to the perovskite structure. Superconductivity takes place within the copper-oxide (CuO2) sheets, with only weak coupling between adjacent CuO2 planes, making the properties close to that of a two-dimensional material. Electrical currents flow within the CuO2 sheets, resulting in a large anisotropy in normal conducting and superconducting properties, with a much higher conductivity parallel to the CuO2 plane than in the perpendicular direction.

Critical superconducting temperatures depend on the chemical compositions, cations substitutions and oxygen content. Chemical formulae of superconducting materials generally contain fractional numbers to describe the doping required for superconductivity. There are several families of cuprate superconductors which can be categorized by the elements they contain and the number of adjacent copper-oxide layers in each superconducting block. For example, YBCO and BSCCO can alternatively be referred to as Y123 and Bi2201/Bi2212/Bi2223 depending on the number of layers in each superconducting block (n). The superconducting transition temperature has been found to peak at an optimal doping value (p=0.16) and an optimal number of layers in each superconducting block, typically n=3.

The undoped "parent" or "mother" compounds are Mott insulators with long-range antiferromagnetic order at sufficiently low temperatures. Single band models are generally considered to be enough to describe the electronic properties.

Cuprate superconductors usually feature copper oxides in both the oxidation states 3+ and 2+. For example, YBa2Cu3O7 is described as Y3+(Ba2+)2(Cu3+)(Cu2+)2(O2−)7. The copper 2+ and 3+ ions tend to arrange themselves in a checkerboard pattern, a phenomenon known as charge ordering.[8] All superconducting cuprates are layered materials having a complex structure described as a superlattice of superconducting CuO2 layers separated by spacer layers, where the misfit strain between different layers and dopants in the spacers induce a complex heterogeneity that in the superstripes scenario is intrinsic for high-temperature superconductivity.

Superconducting mechanism

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Schematic doping phase diagram of cuprate high-temperature superconductors

Superconductivity in the cuprates is considered unconventional and is not explained by BCS theory. Possible pairing mechanisms for cuprate superconductivity continue to be the subject of considerable debate and further research. Similarities between the low-temperature antiferromagnetic state in undoped materials and the low-temperature superconducting state that emerges upon doping, primarily the dx2−y2 orbital state of the Cu2+ ions, suggest that electron-phonon coupling is less relevant in cuprates. Recent work on the Fermi surface has shown that nesting occurs at four points in the antiferromagnetic Brillouin zone where spin waves exist and that the superconducting energy gap is larger at these points. The weak isotope effects observed for most cuprates contrast with conventional superconductors that are well described by BCS theory.

In 1987, Philip Anderson proposed that superexchange could act as a high-temperature superconductor pairing mechanism. In 2016, Chinese physicists found a correlation between a cuprate's critical temperature and the size of the charge transfer gap in that cuprate, providing support for the superexchange hypothesis. A 2022 study found that the varying density of actual Cooper pairs in a bismuth strontium calcium copper oxide superconductor matched with numerical predictions based on superexchange.[9] But so far there is no consensus on the mechanism, and the search for an explanation continues.

Applications

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BSCCO superconductors already have large-scale applications. For example, tens of kilometers of BSCCO-2223 at 77 K superconducting wires are being used in the current leads of the Large Hadron Collider at CERN[10] (but the main field coils are using metallic lower temperature superconductors, mainly based on niobium–tin).

See also

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Bibliography

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  • Rybicki et al, Perspective on the phase diagram of cuprate high-temperature superconductors, University of Leipzig, 2015 doi:10.1038/ncomms11413

References

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  1. ^ J. G. Bednorz; K. A. Mueller (1986). "Possible high TC superconductivity in the Ba–La–Cu–O system". Z. Phys. B. 64 (2): 189–193. Bibcode:1986ZPhyB..64..189B. doi:10.1007/BF01303701. S2CID 118314311.
  2. ^ Mark Buchanan (2001). "Mind the pseudogap". Nature. 409 (6816): 8–11. doi:10.1038/35051238. PMID 11343081. S2CID 5471795.
  3. ^ Nobel prize autobiography.
  4. ^ Wu, M. K.; Ashburn, J. R.; Torng, C. J.; Hor, P. H.; Meng, R. L.; Gao, L.; Huang, Z. J.; Wang, Y. Q.; Chu, C. W. (1993), "Superconductivity at 93 K in a New Mixed-Phase Y-Ba-Cu-O Compound System at Ambient Pressure", Ten Years of Superconductivity: 1980–1990, Perspectives in Condensed Matter Physics, vol. 7, Dordrecht: Springer Netherlands, pp. 281–283, doi:10.1007/978-94-011-1622-0_36, ISBN 978-94-010-4707-4, retrieved October 14, 2021
  5. ^ Sheng, Z. Z.; Hermann A. M. (1988). "Bulk superconductivity at 120 K in the Tl–Ca/Ba–Cu–O system". Nature. 332 (6160): 138–139. Bibcode:1988Natur.332..138S. doi:10.1038/332138a0. S2CID 30690410.
  6. ^ Schilling, A.; Cantoni, M.; Guo, J. D.; Ott, H. R. (1993). "Superconductivity above 130 K in the Hg–Ba–Ca–Cu–O system". Nature. 363 (6424): 56–58. Bibcode:1993Natur.363...56S. doi:10.1038/363056a0. S2CID 4328716.
  7. ^ Lee, Patrick A. (2008). "From high temperature superconductivity to quantum spin liquid: progress in strong correlation physics". Reports on Progress in Physics. 71 (1): 012501. arXiv:0708.2115. Bibcode:2008RPPh...71a2501L. doi:10.1088/0034-4885/71/1/012501. S2CID 119315840.
  8. ^ Li, Xintong; Zou, Changwei; Ding, Ying; Yan, Hongtao; Ye, Shusen; Li, Haiwei; Hao, Zhenqi; Zhao, Lin; Zhou, Xingjiang; Wang, Yayu (January 12, 2021). "Evolution of Charge and Pair Density Modulations in Overdoped ". Physical Review X. 11 (1): 011007. arXiv:2101.06598. doi:10.1103/PhysRevX.11.011007.
  9. ^ Wood, Charlie (September 21, 2022). "High-Temperature Superconductivity Understood at Last". Quanta Magazine. Retrieved September 22, 2022.
  10. ^ Amalia Ballarino (November 23, 2005). "HTS materials for LHC current leads". CERN.
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