Room-temperature superconductor

Unsolved problem in physics:

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

A room-temperature superconductor is a hypothetical material capable of displaying superconductivity at temperatures above 0 °C (273 K; 32 °F), which are commonly encountered in everyday settings. As of 2023, the material with the highest accepted superconducting temperature was highly pressurized lanthanum decahydride, whose transition temperature is approximately 250 K (−23 °C) at 200 GPa.[1][2]

At standard atmospheric pressure, cuprates currently hold the temperature record, manifesting superconductivity at temperatures as high as 138 K (−135 °C).[3] Over time, researchers have consistently encountered superconductivity at temperatures previously considered unexpected or impossible, challenging the notion that achieving superconductivity at room temperature was infeasible.[4][5] The concept of "near-room temperature" transient effects has been a subject of discussion since the early 1950s.

  1. ^ Cite error: The named reference hemley was invoked but never defined (see the help page).
  2. ^ Cite error: The named reference eremets was invoked but never defined (see the help page).
  3. ^ Dai, Pengcheng; Chakoumakos, Bryan C.; Sun, G.F.; Wong, Kai Wai; Xin, Ying; 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.
  4. ^ Geballe, Theodore Henry (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.
  5. ^ Jones, Barbara A.; Roche, Kevin P. (25 July 2016). "Almaden Institute 2012: Superconductivity 297 K – Synthetic Routes to Room Temperature Superconductivity". researcher.watson.ibm.com. Archived from the original on 12 December 2013. Retrieved 18 September 2018.

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