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Organic conductor

From Wikipedia, the free encyclopedia

An organic conductor, also known as a molecular conductor, is a material that is primarily composed of organic molecules and exhibits metallic conductivity. Most such materials are based on planar π-conjugated molecular systems and have attracted attention in the study of low-dimensional physics. They are also known for displaying a variety of electronic properties, including superconductivity, charge density waves, spin density waves, Mott insulators, and charge ordering.[1][2][3] This field originated in the early 1950s and has primarily developed through efforts to improve electrical conductivity and develop organic conductors and superconductors.[1][4]

See also

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References

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  1. 1 2 Jérome, Denis; Bourbonnais, Claude (2024). "Quasi one-dimensional organic conductors: from Fröhlich conductivity and Peierls insulating state to magnetically-mediated superconductivity, a retrospective". Comptes Rendus. Physique. 25: 17–178. arXiv:2311.03104. Bibcode:2024CRPhy..25...17J. doi:10.5802/crphys.164.
  2. ↑ Jérome, D (1991). "The Physics of Organic Superconductors". Science. 252 (5012): 1509–1514. Bibcode:1991Sci...252.1509J. doi:10.1126/science.252.5012.1509.
  3. ↑ Seo, H.; Hotta, C.; Fukuyama, H. (2004). "Toward Systematic Understanding of Diversity of Electronic Properties in Low-Dimensional Molecular Solids". Chemical Review. 104 (11): 5005–5036. doi:10.1021/cr030646k. PMID 15535640.
  4. ↑ Naito, Toshio (2021). "Modern History of Organic Conductors: An Overview". Crystals. 11 (7). 838. doi:10.3390/cryst11070838.