Flux line lattice state versus magnetism in electron-doped cuprate superconductor Sr_{1-x}La_{x}CuO_{2}
| dc.creator | Satoh, Kohki H. | |
| dc.creator | Takeshita, Soshi | |
| dc.creator | Koda, Akihiro | |
| dc.creator | Kadono, Ryosuke | |
| dc.creator | Ishida, Kenji | |
| dc.creator | Pyon, Sunsen | |
| dc.creator | Sasagawa, Takao | |
| dc.creator | Takagi, Hidenori | |
| dc.date | 2007-10-03 | |
| dc.date | 2008-05-18 | |
| dc.date.accessioned | 2026-07-07T09:39:16Z | |
| dc.date.available | 2026-07-07T09:39:16Z | |
| dc.description | The microscopic details of flux line lattice state studied by muon spin rotation is reported in an electron-doped high-$T_{\rm c}$ cuprate superconductor, Sr$_{1-x}$La$_{x}$CuO$_{2}$ (SLCO, $x=0.10$--0.15). A clear sign of phase separation between magnetic and non-magnetic phases is observed, where the effective magnetic penetration depth [$λ\equivλ(T,H)$] is determined selectively for the latter phase. The extremely small value of $λ(0,0)$ %versus $T_{\rm c}$ and corresponding large superfluid density ($n_s \propto λ^{-2}$) is consistent with presence of a large Fermi surface with carrier density of $1+x$, which suggests the breakdown of the "doped Mott insulator" even at the "optimal doping" in SLCO. Moreover, a relatively weak anisotropy in the superconducting order parameter is suggested by the field dependence of $λ(0,H)$. These observations strongly suggest that the superconductivity in SLCO is of a different class from hole-doped cuprates. | |
| dc.description | 7 pages,6 figures. Added figure and changed content. This manuscript will be published by Physical Review B | |
| dc.identifier | https://arxiv.org/abs/0710.0773 | |
| dc.identifier | http://arxiv.org/abs/0710.0773 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/161107 | |
| dc.subject | Superconductivity | |
| dc.title | Flux line lattice state versus magnetism in electron-doped cuprate superconductor Sr_{1-x}La_{x}CuO_{2} | |
| dc.type | text |