Muon spin rotation in GdSr2Cu2RuO8: Implications
- Dale R. Harshmand, f, g, h(Author),
- John D. Dowd(Author),
- W. J. Kosslerg(Author),
- D. R. Noakesc(Author),
- C. E. Stronachc(Author),
- ,
- bUniversity of British Columbia,
- cVirginia State University,
- dArizona State University,
- eBoston College,
- fUniversity of Notre Dame
Abstract
Muon spin rotation measurements are reported for GdSr2Cu 2RuO8, a material with an onset temperature for superconductivity of about 45 K (which is virtually the same for its superconducting sister compounds Sr2YRu1-uCu uO6 and Gd2-zCezSr 2Cu2RuO10). The data indicate two magnetic ordering transitions, at about 15 K and about 130 K, in addition to the Gd ordering transition known to occur at about 2.6 K. We tentatively attribute the 130 K transition to Ru and the 15 K transition to Cu ordering, effectively ruling out any superconducting mechanism based on fluctuating magnetic moments, which are frozen below about 15 K. If there is only one mechanism of high-temperature superconductivity, then the three facts that (i) all three sister compounds have essentially the same onset Tc for superconductivity and (ii) all three of these compounds contain SrO layers but (iii) only two of the three compounds, GdSr2Cu2RuO 8 and Gd2-zCezSr2Cu 2RuO10 (and not Sr2YRu1-uCu uO6) contain cuprate planes imply that the superconducting layers of all three compounds must be the common SrO layers, and not the cuprate planes (which do not occur in Cu-doped Sr 2YRuO6). Otherwise the coincidence of onset temperatures must be an accident, and there must be at least two mechanisms of high-T c superconductivity: one for doped Sr2YRuO6 and another for cuprate-plane superconductivity.
