Room-temperature superconductor

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A room-temperature superconductor is a material that is capable of exhibiting superconductivity at operating temperatures above 0 °C (273 K; 32 °F), that is, temperatures that can be reached and easily maintained in an everyday environment. As of 2020 the material with the highest accepted superconducting temperature is an extremely pressurized carbonaceous sulfur hydride with a critical transition temperature of +15°C at 267 GPa.[1]

At atmospheric pressure the temperature record is still held by cuprates, which have demonstrated superconductivity at temperatures as high as 138 K (−135 °C).[2]

Although researchers once doubted whether room-temperature superconductivity was actually achievable,[3][4] superconductivity has repeatedly been discovered at temperatures that were previously unexpected or held to be impossible.

Claims of "near-room temperature" transient effects date from the early 1950s. Finding a room temperature superconductor "would have enormous technological importance and, for example, help to solve the world's energy problems, provide for faster computers, allow for novel memory-storage devices, and enable ultra-sensitive sensors, among many other possibilities."[4][5]

Unsolved problem in physics:

Is it possible to make a material that is a superconductor at room temperature and atmospheric pressure?

Reports[edit]

Since the discovery of high-temperature superconductors, several materials have been reported to be room-temperature superconductors, although most of these reports have not been confirmed.[citation needed]

In 2000, while extracting electrons from diamond during ion implantation work, Johan Prins claimed to have observed a phenomenon that he explained as room-temperature superconductivity within a phase formed on the surface of oxygen-doped type IIa diamonds in a 10−6 mbar vacuum.[6]

In 2003, a group of researchers published results on high-temperature superconductivity in palladium hydride (PdHx: x>1)[7] and an explanation in 2004.[8] In 2007 the same group published results suggesting a superconducting transition temperature of 260 K.[9] The superconducting critical temperature increases as the density of hydrogen inside the palladium lattice increases. This work has not been corroborated by other groups.

In 2012, an Advanced Materials article claimed superconducting behavior of graphite powder after treatment with pure water at temperatures as high as 300 K and above.[10][unreliable source?] So far, the authors have not been able to demonstrate the occurrence of a clear Meissner phase and the vanishing of the material's resistance.

In 2014, an article published in Nature suggested that some materials, notably YBCO (yttrium barium copper oxide), could be made to superconduct at room temperature using infrared laser pulses.[11]

In 2015, an article published in Nature by researchers of the Max Planck Institute suggested that under certain conditions such as extreme pressure H2S transitioned to a superconductive form H3S at 150GPa (around 1.5 million times atmospheric pressure) in a diamond anvil cell. The critical temperature is 203 K (−70 °C) which would be the highest Tc ever recorded and their research suggests that other hydrogen compounds could superconduct at up to 260 K (−13 °C) which would match up with the original research of Ashcroft.[12][13]

In 2018, Dev Kumar Thapa and Anshu Pandey from the Solid State and Structural Chemistry Unit of the Indian Institute of Science in Bangalore claimed the observation of superconductivity at ambient pressure and room temperature in films and pellets of a nanostructured material that is composed of silver particles embedded in a gold matrix.[14] Due to similar noise patterns of supposedly independent plots and the publication's lack of peer review, the results have been called into question.[15] Although the researchers validated their findings in a later paper in 2019,[16] this claim is yet to be verified and confirmed.[citation needed]

Also in 2018, researchers noted a possible superconducting phase at 260 K (−13 °C) in lanthanum decahydride at elevated (200 GPa) pressure.[17]

In 2019 the material with the highest accepted superconducting temperature was highly pressurized lanthanum decahydride (LaH10), whose transition temperature is approximately 250 K (−23 °C).[18][19]

In October 2020, room-temperature superconductivity at 288 K (at 15 °C) was reported in a carbonaceous sulfur hydride at very high pressure (267 GPa) triggered into crystallisation via green laser.[20][21]

In early 2021 an announcement reported room-temperature superconductivity in a layered yttrium-palladium-hydron material at 262 K and a pressure of 187 GPa. Palladium may act as a hydrogen migration catalyst in the material.[22]

Theories[edit]

Theoretical work by British physicist Neil Ashcroft predicted that solid metallic hydrogen at extremely high pressure (~500 GPa) should become superconducting at approximately room-temperature because of its extremely high speed of sound and expected strong coupling between the conduction electrons and the lattice vibrations (phonons).[23] This prediction is yet to be experimentally verified, as the pressure to achieve metallic hydrogen is not known but may be on the order of 500 GPa.

A team at Harvard University has claimed to make metallic hydrogen and reports a pressure of 495 GPa.[24] Though the exact critical temperature has not yet been determined, weak signs of a possible Meissner effect and changes in magnetic susceptibility at 250K may have appeared in early magnetometer tests on the original now-lost sample and is being analyzed by the French team working with doughnut shapes rather than planar at the diamond culet tips.[25]

In 1964, William A. Little proposed the possibility of high temperature superconductivity in organic polymers.[26] This proposal is based on the exciton-mediated electron pairing, as opposed to phonon-mediated pairing in BCS theory.

In 2016, research suggested a link between the palladium hydride containing small impurities of sulfur nanoparticles as a plausible explanation for the anomalous transient resistance drops seen during some experiments, and hydrogen absorption by cuprates was suggested in light of the 2015 results in H2S as a plausible explanation for transient resistance drops or "USO" noticed in the 1990s by Chu et al. during research after the discovery of YBCO.[citation needed][27] It is also possible that if the bipolaron explanation is correct, a normally semiconducting material can transition under some conditions into a superconductor if a critical level of alternating spin coupling in a single plane within the lattice is exceeded; this may have been documented in very early experiments from 1986. The best analogy here would be anisotropic magnetoresistance, but in this case the outcome is a drop to zero rather than a decrease within a very narrow temperature range for the compounds tested similar to "re-entrant superconductivity".[citation needed]

It was also discovered that many superconductors, including the cuprates and iron pnictides, have two or more competing mechanisms fighting for dominance (Charge density wave)[citation needed] and excitonic states so, as with organic light emitting diodes and other quantum systems, adding the right spin catalyst may by itself increase Tc. A possible candidate would be iridium or gold placed in some of the adjacent molecules or as a thin surface layer so the correct mechanism then propagates throughout the entire lattice similar to a phase transition. As yet, this is speculative; some efforts have been made, notably adding lead to BSCCO, which is well known to help promote high Tc phases by chemistry alone. However, relativistic effects similar to those found in lead-acid batteries might be responsible suggesting that a similar mechanism in mercury- or thallium-based cuprates may be possible using a related metal such as tin.

Any such catalyst would need to be nonreactive chemically but have properties that affect one mechanism but not the others, and also not interfere with subsequent annealing and oxygenation steps nor change the lattice resonances excessively. A possible workaround for the issues discussed would be to use strong electrostatic fields to hold the molecules in place during one of the steps until the lattice is formed.[original research?]

Some research efforts are currently moving towards ternary superhydrides, where it has been predicted that Li2MgH16 would have a Tc of 473 K (200 °C) at 250 GPa[28][29] (much hotter than what is normally considered room temperature).

See also[edit]

  • Persistent current – Perpetual electric current, not requiring an external power source

References[edit]

  1. ^ Snider, Elliot; Dasenbrock-Gammon, Nathan; McBride, Raymond; Debessai, Mathew; Vindana, Hiranya; Vencatasamy, Kevin; Lawler, Keith V.; Salamat, Ashkan; Dias, Ranga P. (15 October 2020). "Room-temperature superconductivity in a carbonaceous sulfur hydride". Nature. 586 (7829): 373–377. doi:10.1038/s41586-020-2801-z. PMID 33057222.
  2. ^ Dai, P.; Chakoumakos, B.C.; Sun, G.F.; Wong, K.W.; Xin, Y.; Lu, D.F. (1995). "Synthesis and neutron powder diffraction study of the superconductor HgBa2Ca2Cu3O8+δ by Tl substitution". Physica C. 243 (3–4): 201–206. Bibcode:1995PhyC..243..201D. doi:10.1016/0921-4534(94)02461-8.
  3. ^ Geballe, T. H. (12 March 1993). "Paths to Higher Temperature Superconductors". Science. 259 (5101): 1550–1551. Bibcode:1993Sci...259.1550G. doi:10.1126/science.259.5101.1550. PMID 17733017.
  4. ^ a b "Almaden Institute 2012: Superconductivity 297 K – Synthetic Routes to Room Temperature Superconductivity". researcher.watson.ibm.com. 25 July 2016.
  5. ^ NOVA. Race for the Superconductor. Public TV station WGBH Boston. Approximately 1987.
  6. ^ Prins, Johan F (1 March 2003). "The diamond vacuum interface: II. Electron extraction from n-type diamond: evidence for superconduction at room temperature". Semiconductor Science and Technology. 18 (3): S131–S140. Bibcode:2003SeScT..18S.131P. doi:10.1088/0268-1242/18/3/319.
  7. ^ Tripodi, P.; Di Gioacchino, D.; Borelli, R.; Vinko, J. D. (May 2003). "Possibility of high temperature superconducting phases in PdH". Physica C: Superconductivity. 388–389: 571–572. Bibcode:2003PhyC..388..571T. doi:10.1016/S0921-4534(02)02745-4.
  8. ^ Tripodi, P.; Di Gioacchino, D.; Vinko, J. D. (August 2004). "Superconductivity in PdH: Phenomenological explanation". Physica C: Superconductivity. 408–410: 350–352. Bibcode:2004PhyC..408..350T. doi:10.1016/j.physc.2004.02.099.
  9. ^ Tripodi, P.; Di Gioacchino, D.; Vinko, J. D. (2007). "A review of high temperature superconducting property of PdH system". International Journal of Modern Physics B. 21 (18&19): 3343–3347. Bibcode:2007IJMPB..21.3343T. doi:10.1142/S0217979207044524.
  10. ^ Scheike, T.; Böhlmann, W.; Esquinazi, P.; Barzola-Quiquia, J.; Ballestar, A.; Setzer, A. (2012). "Can Doping Graphite Trigger Room Temperature Superconductivity? Evidence for Granular High-Temperature Superconductivity in Water-Treated Graphite Powder". Advanced Materials. 24 (43): 5826–31. arXiv:1209.1938. Bibcode:2012arXiv1209.1938S. doi:10.1002/adma.201202219. PMID 22949348. S2CID 205246535.
  11. ^ Mankowsky, R.; Subedi, A.; Först, M.; Mariager, S. O.; Chollet, M.; Lemke, H. T.; Robinson, J. S.; Glownia, J. M.; Minitti, M. P.; Frano, A.; Fechner, M.; Spaldin, N. A.; Loew, T.; Keimer, B.; Georges, A.; Cavalleri, A. (2014). "Nonlinear lattice dynamics as a basis for enhanced superconductivity in YBa2Cu3O6.5". Nature. 516 (7529): 71–73. arXiv:1405.2266. Bibcode:2014Natur.516...71M. doi:10.1038/nature13875. PMID 25471882. S2CID 3127527.
  12. ^ Cartlidge, Edwin (18 August 2015). "Superconductivity record sparks wave of follow-up physics". Nature. 524 (7565): 277. Bibcode:2015Natur.524..277C. doi:10.1038/nature.2015.18191. PMID 26289188.
  13. ^ Ge, Y. F.; Zhang, F.; Yao, Y. G. (2016). "First-principles demonstration of superconductivity at 280 K (7 °C) in hydrogen sulfide with low phosphorus substitution". Phys. Rev. B. 93 (22): 224513. arXiv:1507.08525. Bibcode:2016PhRvB..93v4513G. doi:10.1103/PhysRevB.93.224513. S2CID 118730557.
  14. ^ Thapa, Dev Kumar; Pandey, Anshu (2018). "Evidence for Superconductivity at Ambient Temperature and Pressure in Nanostructures". arXiv:1807.08572. Bibcode:2018arXiv180708572T. Cite journal requires |journal= (help)
  15. ^ Desikan, Shubashree (18 August 2018). "IISc duo's claim of ambient superconductivity may have support in theory". The Hindu. Retrieved 4 October 2018.
  16. ^ Prasad, R.; Desikan, Shubashree (25 May 2019). "Finally, IISc team confirms breakthrough in superconductivity at room temperature". The Hindu – via www.thehindu.com.
  17. ^ Grant, Andrew (23 August 2018). "Pressurized superconductors approach room-temperature realm". Physics Today. doi:10.1063/PT.6.1.20180823b.
  18. ^ Somayazulu, M.; Ahart, M.; Mishra, A.K.; Geballe, Z.M.; Baldini, M.; Meng, Y.; Struzhkin, V.V.; Hemley, R.J. (2019). "Evidence for Superconductivity above 260K in Lanthanum Superhydride at Megabar Pressures". Phys. Rev. Lett. 122 (2): 027001. arXiv:1808.07695. Bibcode:2019PhRvL.122b7001S. doi:10.1103/PhysRevLett.122.027001. PMID 30720326. S2CID 53622077.
  19. ^ Drozdov, A. P.; Kong, P. P.; Minkov, V. S.; Besedin, S. P.; Kuzovnikov, M. A.; Mozaffari, S.; Balicas, L.; Balakirev, F. F.; Graf, D. E.; Prakapenka, V. B.; Greenberg, E.; Knyazev, D. A.; Tkacz, M.; Eremets, M. I. (2019). "Superconductivity at 250 K in lanthanum hydride under high pressures". Nature. 569 (7757): 528–531. arXiv:1812.01561. Bibcode:2019Natur.569..528D. doi:10.1038/s41586-019-1201-8. PMID 31118520. S2CID 119231000.
  20. ^ Kenneth Chang (14 October 2020). "Finally, the First Room-Temperature Superconductor". The New York Times.
  21. ^ Snider, Elliot; Dasenbrock-Gammon, Nathan; McBride, Raymond; Debessai, Mathew; Vindana, Hiranya; Vencatasamy, Kevin; Lawler, Keith V.; Salamat, Ashkan; Dias, Ranga P. (October 2020). "Room-temperature superconductivity in a carbonaceous sulfur hydride". Nature. 586 (7829): 373–377. doi:10.1038/s41586-020-2801-z. PMID 33057222.
  22. ^ https://phys.org/news/2021-03-material-superconductive-room-temperature-pressure.html
  23. ^ Ashcroft, N. W. (1968). "Metallic Hydrogen: A High-Temperature Superconductor?". Physical Review Letters. 21 (26): 1748–1749. Bibcode:1968PhRvL..21.1748A. doi:10.1103/PhysRevLett.21.1748.
  24. ^ Ian Johnston (26 January 2017). "Hydrogen turned into metal in stunning act of alchemy that could revolutionise technology and spaceflight". The Independent.
  25. ^ Loubeyre, Paul; Occelli, Florent; Dumas, Paul (2019). "Observation of a first order phase transition to metal hydrogen near 425 GPa". arXiv:1906.05634. Bibcode:2019arXiv190605634L. Cite journal requires |journal= (help)
  26. ^ Little, W. A. (1964). "Possibility of Synthesizing an Organic Superconductor". Physical Review. 134 (6A): A1416–A1424. Bibcode:1964PhRv..134.1416L. doi:10.1103/PhysRev.134.A1416.
  27. ^ Transient High-Temperature Superconductivity in Palladium Hydride. Griffith University (Griffith thesis). Griffith University. 2016.
  28. ^ Sun, Ying; Lv, Jian; Xie, Yu; Liu, Hanyu; Ma, Yanming (26 August 2019). "Route to a Superconducting Phase above Room Temperature in Electron-Doped Hydride Compounds under High Pressure". Physical Review Letters. 123 (9): 097001. Bibcode:2019PhRvL.123i7001S. doi:10.1103/PhysRevLett.123.097001. PMID 31524448. The recent theory-orientated discovery of record high-temperature superconductivity (Tc∼250 K) in sodalitelike clathrate LaH10 is an important advance toward room-temperature superconductors. Here, we identify an alternative clathrate structure in ternary Li2MgH16 with a remarkably high estimated Tc of ∼473 K at 250 GPa, which may allow us to obtain room-temperature or even higher-temperature superconductivity.
  29. ^ Extance, Andy (1 November 2019). "The race is on to make the first room temperature superconductor". www.chemistryworld.com. Royal Society of Chemistry. Retrieved 30 December 2019. In August, Ma and colleagues published a study that showed the promise of ternary superhydrides. They predicted that Li2MgH16 would have a Tc of 473 °K at 250 GPa, far in excess of room temperature.