4.8 Article

New magnetic phase diagram of (Sr,Ca)2RuO4

Journal

NATURE MATERIALS
Volume 11, Issue 4, Pages 323-328

Publisher

NATURE PUBLISHING GROUP
DOI: 10.1038/NMAT3236

Keywords

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Funding

  1. US National Science Foundation (NSF) under the Materials World Network (MWN) [DMR-0502706, 0806846]
  2. Partnership for International Research and Education (PIRE) [OISE-0968226]
  3. Canadian Natural Sciences and Engineering Research Council (NSERC) [DMR-1105961]
  4. Canadian Institute for Advanced Research (CIFAR) at McMaster
  5. Japan Society for the Promotion of Science (JSPS) [21684019]
  6. Scientific Research on Priority Areas (SRPA) from the Ministry of Education, Culture, Sports, Science and Technology (MEXT) at Kyoto and Tokyo Universities, [19052003]
  7. MEXT-SRPA at Osaka University [19052006]
  8. Direct For Mathematical & Physical Scien
  9. Division Of Materials Research [0806846, 1105961] Funding Source: National Science Foundation

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High-T-c cuprates, iron pnictides, organic BEDT and TMTSF, alkali-doped C-60, and heavy-fermion systems have superconducting states adjacent to competing states exhibiting static antiferromagnetic or spin density wave order. This feature has promoted pictures for their superconducting pairing mediated by spin fluctuations. Sr2RuO4 is another unconventional superconductor which almost certainly has a p-wave pairing. The absence of known signatures of static magnetism in the Sr-rich side of the (Ca, Sr) substitution space, however, has led to a prevailing view that the superconducting state in Sr2RuO4 emerges from a surrounding Fermi-liquid metallic state. Using muon spin relaxation and magnetic susceptibility measurements, we demonstrate here that (Sr, Ca)(2)RuO4 has a ground state with static magnetic order over nearly the entire range of (Ca, Sr) substitution, with spin-glass behaviour in Sr1:5Ca0:5RuO4 and Ca1.5Sr0.5RuO4. The resulting new magnetic phase diagram establishes the proximity of superconductivity in Sr2RuO4 to competing static magnetic order.

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