Ferromagnetic superconductor

Short description: Superconductors whose ferromagnetism is related to their superconductivity

Ferromagnetic superconductors are materials that display intrinsic coexistence of ferromagnetism and superconductivity. They include UGe2,[1] URhGe,[2] and UCoGe.[3] Evidence of ferromagnetic superconductivity was also reported for ZrZn2 in 2001, but later reports[4] question these findings. These materials exhibit superconductivity in proximity to a magnetic quantum critical point.

The nature of the superconducting state in ferromagnetic superconductors is currently under debate. Early investigations[5] studied the coexistence of conventional s-wave superconductivity with itinerant ferromagnetism. However, the scenario of spin-triplet pairing soon gained the upper hand.[6][7] A mean-field model for coexistence of spin-triplet pairing and ferromagnetism was developed in 2005.[8][9]

These models consider uniform coexistence of ferromagnetism and superconductivity, i.e. the same electrons which are both ferromagnetic and superconducting at the same time. Another scenario where there is an interplay between magnetic and superconducting order in the same material is superconductors with spiral or helical magnetic order. Examples of such include ErRh4B4 and HoMo6S8. In these cases, the superconducting and magnetic order parameters entwine each other in a spatially modulated pattern, which allows for their mutual coexistence, although it is no longer uniform. Even spin-singlet pairing may coexist with ferromagnetism in this manner.

## Contents

* 1 Theory
* 2 See also
* 3 References
* 4 Further reading

## Theory

In conventional superconductors, the electrons constituting the Cooper pair have opposite spin, forming so-called spin-singlet pairs. However, other types of pairings are also permitted by the governing Pauli principle. In the presence of a magnetic field, spins tend to align themselves with the field, which means that a magnetic field is detrimental for the existence of spin-singlet Cooper pairs. A viable mean-field Hamiltonian for modelling itinerant ferromagnetism coexisting with a non-unitary spin-triplet state may after diagonalization be written as[8][9]

H=H0+∑𝐤σE𝐤σγ𝐤σ†γ𝐤σ,
H0=12∑𝐤σ(ξ𝐤σ−E𝐤σ−Δ𝐤σ†b𝐤σ)+INM2/2,
E𝐤σ=ξ𝐤σ2+|Δ𝐤σ|2.

## See also

* Bean's critical state model
* Ferromagnetic superconducting 2D materials
* Reentrant superconductivity

## References

1. ↑ Saxena, S. S.; Agarwal, P; Agarwal, P.; Ahilan, K.; Grosche, F. M.; Haselwimmer, R. K. W.; Steiner, M. J.; Pugh, E. et al. (2000). "Superconductivity on the border of itinerant-electron ferromagnetism in UGe2". Nature 406 (6796): 587–92. doi:10.1038/35020500. PMID 10949292. Bibcode: 2000Natur.406..587S.
2. ↑ Aoki, Dai; Huxley, Andrew; Ressouche, Eric; Braithwaite, Daniel; Flouquet, Jacques; Brison, Jean-Pascal; Lhotel, Elsa; Paulsen, Carley (2001). "Coexistence of superconductivity and ferromagnetism in URhGe". Nature 413 (6856): 613–6. doi:10.1038/35098048. PMID 11595943. Bibcode: 2001Natur.413..613A.
3. ↑ Huy, N.; Gasparini, A.; De Nijs, D.; Huang, Y.; Klaasse, J.; Gortenmulder, T.; De Visser, A.; Hamann, A. et al. (2007). "Superconductivity on the border of weak itinerant ferromagnetism in UCoGe". Physical Review Letters 99 (6). doi:10.1103/PhysRevLett.99.067006. PMID 17930860. Bibcode: 2007PhRvL..99f7006H.
4. ↑ Yelland, E.; Hayden, S.; Yates, S.; Pfleiderer, C.; Uhlarz, M.; Vollmer, R.; Löhneysen, H.; Bernhoeft, N. et al. (2005). "Superconductivity induced by spark erosion in ZrZn2". Physical Review B 72 (21). doi:10.1103/PhysRevB.72.214523. Bibcode: 2005PhRvB..72u4523Y.
5. ↑ Karchev, N. I.; Blagoev, K. B.; Bedell, K. S.; Littlewood, P. B. (1999-11-30). "Coexistence of superconductivity and ferromagnetism in ferromagnetic metals". arXiv:cond-mat/9911489.
6. ↑ MacHida, Kazushige; Ohmi, Tetsuo (2001). "Theory of Ferromagnetic Superconductivity". Physical Review Letters 86 (5): 850–3. doi:10.1103/PhysRevLett.86.850. PMID 11177956. Bibcode: 2001PhRvL..86..850M.
7. ↑ Samokhin, K.; Walker, M. (2002). "Order parameter symmetry in ferromagnetic superconductors". Physical Review B 66 (17). doi:10.1103/PhysRevB.66.174501. Bibcode: 2002PhRvB..66q4501S.
8. ↑ 8.0 8.1 Nevidomskyy, Andriy (2005). "Coexistence of ferromagnetism and superconductivity near quantum phase transition: The Heisenberg- to Ising-type crossover". Physical Review Letters 94 (9). doi:10.1103/PhysRevLett.94.097003. PMID 15783990. Bibcode: 2005PhRvL..94i7003N.
9. ↑ 9.0 9.1 Linder, J.; Sudbø, A. (2007). "Quantum transport in noncentrosymmetric superconductors and thermodynamics of ferromagnetic superconductors". Physical Review B 76 (5). doi:10.1103/PhysRevB.76.054511. Bibcode: 2007PhRvB..76e4511L.

## Further reading

* Soltan Soltan (2005). Interaction of Superconductivity and Ferromagnetism in YBCO-LCMO. Cuvillier Verlag. p. 1. ISBN 3-86537-349-6. https://books.google.com/books?id=RoxyQ8cNdYYC&pg=PA3.
* T Herrmannsdörfer; F Pobell (2003). "The interplay of superconductivity and nuclear magnetism". Recent trends in theory of physical phenomena in high magnetic fields. Springer. p. 18. ISBN 1-4020-1373-6. https://books.google.com/books?id=yNXrbB2UlvoC&pg=PA18.
* T Moriya & K Ueda; Ueda (2003). "Antiferromagnetic spin fluctuation and superconductivity". Rep Prog Phys 66 (8): 1299–1341. doi:10.1088/0034-4885/66/8/202. Bibcode: 2003RPPh...66.1299M.
* Ferromagnetic superconductors – List of Authority Articles on arxiv.org

Template:Superconductivity

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Magnetic states

* diamagnetism
* superdiamagnetism
* paramagnetism
* superparamagnetism
* ferromagnetism
* superferromagnetism
* antiferromagnetism
* ferrimagnetism
* helimagnetism
* metamagnetism
* mictomagnetism
* spin glass
* spin ice
* ferromagnetic superconductor

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