Kohn–Luttinger superconductivity

Short description: Superconductivity mechanism based on attractive forces generated by screened Coulomb interaction

Not to be confused with Luttinger–Kohn model.

Schematic illustration of mechanism for Kohn-Luttinger superconductivity with p-wave Cooper pair condensation. Over-screening of Coulomb interaction leads to attractive regions at radii on the order of 1/kF where electrons can condense.

Kohn–Luttinger superconductivity is a theoretical mechanism for unconventional superconductivity proposed by Walter Kohn and Joaquin Mazdak Luttinger[1] based on Friedel oscillations. In contrast to BCS theory, in which Cooper pairs are formed due to Bardeen–Pines interaction between electrons and phonons, Kohn–Luttinger mechanism is based on fact that screened Coulomb interaction oscillates as cos⁡(2kFr+ϕ)/r3 and can create Cooper instability for non-zero angular momentum ℓ.

Since Kohn–Luttinger mechanism does not require any additional interactions beyond Coulomb interactions, it can lead to superconductivity in any electronic system. However, the estimated critical temperature, Tc, for Kohn–Luttinger superconductor is exponential in −ℓ4 and thus is extremely small. For example, for metals the critical temperature is given by[1]

kBTcEF=e−(2ℓ)4,

where kB is Boltzmann constant and EF is Fermi energy. For a typical 3D metal with a spherical Fermi surface Kohn and Luttinger estimated that Tc∼10−3K. However, non-spherical Fermi surfaces and variation of parameters may enhance the effect. Indeed, it is proposed that Kohn–Luttinger mechanism is responsible for superconductivity in rhombohedral trilayer graphene,[2][3] which has an annular Fermi surface.

## Further reading

Gor'kov, L. P.; Melik-Barkhudarov, T. K. (November 1961). "Contribution to the theory of superfluidity in an imperfect Fermi gas". Soviet Physics JETP 13 (5): 1018–1022. http://www.jetp.ras.ru/cgi-bin/dn/e_013_05_1018.pdf.

Chubukov, Andrey V. (15 July 1993). "Kohn-Luttinger effect and the instability of a two-dimensional repulsive Fermi liquid at T=0". Physical Review B (American Physical Society) 48 (2): 1097–1104. doi:10.1103/PhysRevB.48.1097. PMID 10007968. Bibcode: 1993PhRvB..48.1097C. https://link.aps.org/doi/10.1103/PhysRevB.48.1097.

Maiti, S.; Chubukov, A. V. (November 2014). "Superconductivity from repulsive interaction". Novel Superfluids: Volume 2. Oxford. pp. 89–158. doi:10.1093/acprof:oso/9780198719267.003.0004. ISBN 978-0-19-871926-7.

## References

1. ↑ 1.0 1.1 Kohn, Walter; Luttinger, Joaquin M. (20 September 1965). "New mechanism for superconductivity". Physical Review Letters (American Physical Society) 15 (12): 524–526. doi:10.1103/PhysRevLett.15.524. Bibcode: 1965PhRvL..15..524K. https://link.aps.org/doi/10.1103/PhysRevLett.15.524.
2. ↑ Ghazaryan, Areg; Holder, Tobias; Serbyn, Maksym; Berg, Erez (9 December 2021). "Unconventional Superconductivity in Systems with Annular Fermi Surfaces: Application to Rhombohedral Trilayer Graphene". Physical Review Letters (American Physical Society) 127 (24). doi:10.1103/PhysRevLett.127.247001. PMID 34951779. Bibcode: 2021PhRvL.127x7001G. https://link.aps.org/doi/10.1103/PhysRevLett.127.247001.
3. ↑ Cea, Tommaso; Pantaleón, Pierre A.; Phong, Võ Tiến; Guinea, Francisco (1 February 2022). "Superconductivity from repulsive interactions in rhombohedral trilayer graphene: A Kohn-Luttinger-like mechanism". Physical Review B (American Physical Society) 105 (7). doi:10.1103/PhysRevB.105.075432. Bibcode: 2022PhRvB.105g5432C. https://link.aps.org/doi/10.1103/PhysRevB.105.075432.

Template:Superconductivity

0.00

(0 votes)

Original source: https://en.wikipedia.org/wiki/Kohn–Luttinger superconductivity. Read more

|

Retrieved from "https://handwiki.org/wiki/index.php?title=Physics:Kohn–Luttinger_superconductivity&oldid=4108654"