APS March Meeting 2013
Volume 58, Number 1
Monday–Friday, March 18–22, 2013;
Baltimore, Maryland
Session A2: Invited Session: Novel Superconductivity in FE Selenide Superconductors
8:00 AM–11:00 AM,
Monday, March 18, 2013
Room: Ballroom II
Sponsoring
Unit:
DCMP
Chair: Douglas Scalapino, University of California at Santa Barbara
Abstract ID: BAPS.2013.MAR.A2.5
Abstract: A2.00005 : S$_{4}$ Symmetric Microscopic Model for Iron Based Superconductors
10:24 AM–11:00 AM
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Abstract
Author:
Jiangping Hu
(Institute of Physics, CAS, China and Department of Physics, Purdue University)
How are cuprates and iron-based high temperature superconductors correlated? What is the common mechanism behind two different families of iron-based superconductors, iron-pnicitides and iron-chalcogenides? These two questions
are two major challenges in the today's field of high temperature superconductors.
In this talk, we will show when the lattice symmetry, the \textbf{S}$_{\mathbf{4}}$ symmetry, of the building block, the
tri-layer structure of FeAs or FeSe, is properly considered, the low energy physics of iron-based superconductors is governed by a two-orbital Hamiltonian near half filling that can be divided two weakly coupled one-orbital model. We will discuss the microscopic origin and some unique properties of the model, including magnetism and pairing symmetry. The model
provides a unified understanding of iron pnictides and iron chalcogenides, and suggests that cuprates and iron-based superconductors share an identical high-T$_{c}$~superconducting mechanism.
The model leads to a natural classification of pairing symmetry according to \textbf{S}$_{\mathbf{4}}$ symmetry. When the pairing is driven by antiferromagnetic exchange couplings, there are two different s-wave states. One s-wave is the well-studied s$\pm$ pairing which is in the A phase of \textbf{S}$_{\mathbf{4}}$ symmetry ( even under \textbf{S}$_{\mathbf{4}}$ symmetry operation), and the other is a new type of extended s-wave pairing which is in the B phase of \textbf{S}$_{\mathbf{4}}$ symmetry ( odd under\textbf{S}$_{\mathbf{4}}$ symmetry operation). The superconductivity order in the B phase are characterized by opposite signs between up and bottom As(Se) layers in the trilayer Fe-As(Se) structure. The 122 Iron-chalcogenides and the single layer FeSe are most likely in the B-phase.
We believe that the model establishes a new foundation for exploring novel properties of iron based superconductors.
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References: J.P. Hu and Ningning Hao, Phys. Rev. X, 021009 (2012); T. X. Ma, H.Q. Lin and J.P. Hu, Arxiv:1206.6277 (2012); N.N. Hao, Y.P. Wang and J.P. Hu, Arxiv: 1207.6798 (2012); J.P. Hu, and NingNing Hao, unpublished; J.P. Hu, Arxiv: 1208.6201 (2012)
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2013.MAR.A2.5