TY - JOUR
T1 - Reciprocal-space structure and dispersion of the magnetic resonant mode in the superconducting phase of Rb xFe 2-ySe 2 single crystals
AU - Friemel, G.
AU - Park, J. T.
AU - Maier, T. A.
AU - Tsurkan, V.
AU - Li, Yuan
AU - Deisenhofer, J.
AU - Krug Von Nidda, H. A.
AU - Loidl, A.
AU - Ivanov, A.
AU - Keimer, B.
AU - Inosov, D. S.
PY - 2012/4/20
Y1 - 2012/4/20
N2 - Inelastic neutron scattering is employed to study the reciprocal-space structure and dispersion of magnetic excitations in the normal and superconducting states of single-crystalline Rb 0.8Fe 1.6Se 2. We show that the recently discovered magnetic resonant mode in this compound has a quasi-two-dimensional character, similar to overdoped iron-pnictide superconductors. Moreover, it has a rich in-plane structure that is dominated by four elliptical peaks, symmetrically surrounding the Brillouin zone corner, without √5×√5 reconstruction. We also present evidence for the dispersion of the resonance peak, as its position in momentum space depends on energy. Comparison of our findings with the results of band structure calculations leads to a robust bulk-sensitive estimate of the electron count in the superconducting phase and provides strong support for the itinerant origin of the observed signal. It can be traced back to the nesting of electronlike Fermi pockets in the doped metallic phase of the sample in the absence of iron-vacancy ordering.
AB - Inelastic neutron scattering is employed to study the reciprocal-space structure and dispersion of magnetic excitations in the normal and superconducting states of single-crystalline Rb 0.8Fe 1.6Se 2. We show that the recently discovered magnetic resonant mode in this compound has a quasi-two-dimensional character, similar to overdoped iron-pnictide superconductors. Moreover, it has a rich in-plane structure that is dominated by four elliptical peaks, symmetrically surrounding the Brillouin zone corner, without √5×√5 reconstruction. We also present evidence for the dispersion of the resonance peak, as its position in momentum space depends on energy. Comparison of our findings with the results of band structure calculations leads to a robust bulk-sensitive estimate of the electron count in the superconducting phase and provides strong support for the itinerant origin of the observed signal. It can be traced back to the nesting of electronlike Fermi pockets in the doped metallic phase of the sample in the absence of iron-vacancy ordering.
UR - https://www.scopus.com/pages/publications/84860299649
U2 - 10.1103/PhysRevB.85.140511
DO - 10.1103/PhysRevB.85.140511
M3 - Article
AN - SCOPUS:84860299649
SN - 1098-0121
VL - 85
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 14
M1 - 140511
ER -