APS March Meeting 2011
Volume 56, Number 1
Monday–Friday, March 21–25, 2011;
Dallas, Texas
Session A26: Focus Session: Iron Based Superconductors -- Theory
8:00 AM–11:00 AM,
Monday, March 21, 2011
Room: D162/164
Sponsoring
Units:
DMP DCOMP
Chair: Qimiao Si, Rice University
Abstract ID: BAPS.2011.MAR.A26.4
Abstract: A26.00004 : Computational studies of models for the magnetism and superconductivity in iron pnictides
8:36 AM–9:12 AM
Preview Abstract
Abstract
Author:
Adriana Moreo
(University of Tennessee and Oak Ridge National Lab)
The properties of multiorbital electronic model Hamiltonians for
the pnictides are explored using a variety of many-body
techniques. Via mean-field approximations, a regime where the
undoped system develops $(\pi,0)$ magnetic order
while remaining metallic is found at intermediate values of the
Hubbard repulsion $U$. Comparison of our results against ARPES
and neutron scattering data allows us to determine a range of
realistic values for the parameters in the models [1]. The
orbital spectral weight redistribution that occurs near the Fermi
surface in the $(\pi,0)$ magnetic state without long-range
orbital order is also discussed [2]. The two-orbital
``$t$-$U$-$J$'' Hubbard model at intermediate $U$,
with magnetic order and pairing tendencies enhanced by the
addition of Heisenberg terms that arise from the strong coupling
expansion, is studied via exact diagonalization. At intermediate
couplings and considering two extra electrons added to the
undoped system, an $A_{1g}$ bound state is
found compatible with the ``extended s$\pm$'' pairing discussed
in the RPA approximation. Bound states with $B_{2g}$ symmetry,
involving intra- and inter-band components, are also stable
in portions of the phase diagram, while states with $B_{1g}$
symmetry are close in energy, suggesting that small changes in
parameters may render any of the three channels stable [3].
Finally, using the real-space Hartree-Fock approximation on
finite clusters the presence of charge stripes at intermediate $U$ is
also observed for electron-doped systems. The patterns
of charge, spin, and orbital order, as well as the influence of
quenched disorder will be discussed [4].\\[4pt]
[1] Q. Luo {\it et al.}, Phys. Rev. B {\bf 82}, 104508(2010). See
also R. Yu {\it et al.}, Phys. Rev. B {\bf 79}, 104510 (2009).\\[0pt]
[2] M. Daghofer {\it et al.}, Phys. Rev. B {\bf 81}, 180514(R)
(2010).\\[0pt]
[3] A. Nicholson {\it et al.}, preprint. See also M. Daghofer
{\it et al.}, Phys. Rev. Lett. {\bf 101}, 237004 (2008), and A.
Moreo {\it et al.}, Phys. Rev. B {\bf 79}, 134502 (2009).\\[0pt]
[4] Q. Luo {\it et al.}, preprint.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2011.MAR.A26.4