TY - JOUR
T1 - Coexistence of magnetism and superconductivity ins(R=Eu and Gd)
AU - Felner, I.
AU - Asaf, U.
AU - Levi, Y.
AU - Millo, O.
PY - 1997
Y1 - 1997
N2 - The superconducting (Formula presented) materials are also magnetically ordered at (Formula presented)≫:(Formula presented) ((Formula presented)∼42, 32 and (Formula presented)∼180, 122 K for R=Gd and Eu, respectively). Magnetic susceptibility and Mössbauer spectroscopy show that superconductivity is confined to the (Formula presented) planes, whereas magnetism is due to the Ru sublattice. Scanning-tunneling-spectroscopy measurements reveal a superconducting gap structure for the whole sample, indicating that the materials are of single phase, which simultaneously manifest both superconductivity and magnetism.
AB - The superconducting (Formula presented) materials are also magnetically ordered at (Formula presented)≫:(Formula presented) ((Formula presented)∼42, 32 and (Formula presented)∼180, 122 K for R=Gd and Eu, respectively). Magnetic susceptibility and Mössbauer spectroscopy show that superconductivity is confined to the (Formula presented) planes, whereas magnetism is due to the Ru sublattice. Scanning-tunneling-spectroscopy measurements reveal a superconducting gap structure for the whole sample, indicating that the materials are of single phase, which simultaneously manifest both superconductivity and magnetism.
UR - http://www.scopus.com/inward/record.url?scp=0642332703&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.55.R3374
DO - 10.1103/PhysRevB.55.R3374
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AN - SCOPUS:0642332703
SN - 1098-0121
VL - 55
SP - R3374-R3377
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 6
ER -