We calculate RPA-BCS based spin resonance spectra of newly discovered
iron-selenide superconductor using two orbitals tight-binding (TB) model. The
slightly squarish electron pocket Fermi surfaces (FSs) at
(π,0)/(0,π)−momenta produce leading interpocket nesting instability at
incommensurate vector q∼(π,0.5π) in the normal state static
susceptibility, pinning a strong stripe-like spin-density wave (SDW) or
antiferromagnetic (AFM) order at some critical value of U. The same nesting
also induces dx2−y2−pairing. The superconducting (SC) gap is nodeless
and isotropic on the FSs as they are concentric to the four-fold symmetry point
of the d−wave gap maxima, in agreement with various measurements. This
induces an slightly incommensurate spin resonance with `hour-glass'-like
dispersion feature, in close agreement with neutron data of chalcogenides. We
also calculate T pendence of the SC gap solving BCS gap equations and find
that the spin resonance follows the same T evolution of Δ(T) both in
energy and intensity, suggesting that an itinerant weak or intermediate pair
coupling theory is relevant in this system.Comment: 4.5 pages, 4 figures; Submitted (v2): Some types are corrected (v3):
Expanded and published versio