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Unfolding the physics of URu2Si2 through silicon to phosphorus substitution.
Gallagher, A; Chen, K-W; Moir, C M; Cary, S K; Kametani, F; Kikugawa, N; Graf, D; Albrecht-Schmitt, T E; Riggs, S C; Shekhter, A; Baumbach, R E.
Affiliation
  • Gallagher A; National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA.
  • Chen KW; National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA.
  • Moir CM; National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA.
  • Cary SK; Department of Chemistry and Biochemistry, Florida State University, Tallahassee, Florida 32306, USA.
  • Kametani F; Applied Superconductivity Center, Florida State University, Tallahassee, Florida 32310, USA.
  • Kikugawa N; National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA.
  • Graf D; National Institute for Materials Science 3-13 Sakura, Tsukuba 305-0003, Japan.
  • Albrecht-Schmitt TE; National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA.
  • Riggs SC; Department of Chemistry and Biochemistry, Florida State University, Tallahassee, Florida 32306, USA.
  • Shekhter A; National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA.
  • Baumbach RE; National High Magnetic Field Laboratory, Florida State University, Tallahassee, Florida 32310, USA.
Nat Commun ; 7: 10712, 2016 Feb 19.
Article in En | MEDLINE | ID: mdl-26891903
The heavy fermion intermetallic compound URu2Si2 exhibits a hidden-order phase below the temperature of 17.5 K, which supports both anomalous metallic behavior and unconventional superconductivity. While these individual phenomena have been investigated in detail, it remains unclear how they are related to each other and to what extent uranium f-electron valence fluctuations influence each one. Here we use ligand site substituted URu2Si(2-x)P(x) to establish their evolution under electronic tuning. We find that while hidden order is monotonically suppressed and destroyed for x≤0.035, the superconducting strength evolves non-monotonically with a maximum near x≈0.01 and that superconductivity is destroyed near x≈0.028. This behavior reveals that hidden order depends strongly on tuning outside of the U f-electron shells. It also suggests that while hidden order provides an environment for superconductivity and anomalous metallic behavior, it's fluctuations may not be solely responsible for their progression.

Full text: 1 Database: MEDLINE Language: En Journal: Nat Commun Journal subject: BIOLOGIA / CIENCIA Year: 2016 Type: Article Affiliation country: United States

Full text: 1 Database: MEDLINE Language: En Journal: Nat Commun Journal subject: BIOLOGIA / CIENCIA Year: 2016 Type: Article Affiliation country: United States