Fully gapped superconductivity with no sign change in the prototypical heavy-fermion CeCu 2 Si 2

Author:

Yamashita Takuya1,Takenaka Takaaki2,Tokiwa Yoshifumi1,Wilcox Joseph A.3,Mizukami Yuta2,Terazawa Daiki1,Kasahara Yuichi1,Kittaka Shunichiro4,Sakakibara Toshiro4,Konczykowski Marcin5,Seiro Silvia6,Jeevan Hirale S.6ORCID,Geibel Christoph6,Putzke Carsten3ORCID,Onishi Takafumi1,Ikeda Hiroaki7,Carrington Antony3,Shibauchi Takasada2,Matsuda Yuji1

Affiliation:

1. Department of Physics, Kyoto University, Kyoto 606-8502, Japan.

2. Department of Advanced Materials Science, University of Tokyo, Kashiwa, Chiba 277-8561, Japan.

3. H. H. Wills Physics Laboratory, University of Bristol, Bristol BS8 1TL, UK.

4. Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan.

5. Laboratoire des Solides Irradiés, École Polytechnique, CNRS, Commissariat à l’Energie Atomique et aux Energies Alternatives, Université Paris-Saclay, 91128 Palaiseau Cedex, France.

6. Max Planck Institute for Chemical Physics of Solids, Nöthnitzer Strasse 40, 01187 Dresden, Germany.

7. Department of Physics, Ritsumeikan University, Kusatsu 525-8577, Japan.

Abstract

Heavy electrons with extremely strong Coulomb repulsions can condense into a fully gapped s-wave superconducting state.

Funder

Japan Society for the Promotion of Science

UK Engineering and Physical Sciences Research Council

Publisher

American Association for the Advancement of Science (AAAS)

Subject

Multidisciplinary

Reference54 articles.

1. Superconductivity in the presence of strong Pauli paramagnetism: CeCu 2 Si2;Steglich F.;Phys. Rev. Lett.,1979

2. Superconducting phases of f-electron compounds;Pfleiderer C.;Rev. Mod. Phys.,2009

3. Magnetically mediated superconductivity in heavy fermion compounds;Mathur N. D.;Nature,1998

4. P. Thalmerier G. Zwicknagl Handbook on the Physics and Chemistry of Rare Earths (Elsevier B.V. 2004) vol. 36.

5. The case for dx2−y2 pairing in the cuprate superconductors;Scalapino D. J.;Phys. Rep.,1995

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