Superconductivity in Multi-orbital t-J1-J2 Model and its Implications for Iron Pnictides

preprint2010arXivOpen access

Abstract

Motivated by the bad metal behavior of the iron pnictides, we study a multi-orbital t−J1−J2\mathrm{t-J_1-J_2} model and investigate possible singlet superconducting pairings. Magnetic frustration by itself leads to a large degeneracy in the pairing states. The kinetic energy breaks this into a quasi-degeneracy among a reduced set of pairing states. For small electron and hole Fermi pockets, an A1gA_{1g} state dominates over the phase diagram but a B1gB_{1g} state has close-by energy. In addition to the nodeless A1gA_{1g} sx2y2s_{x^2y^2} channel, the nodal A1gA_{1g} sx2+y2s_{x^2+y^2} and B1gB_{1g} dx2−y2d_{x^2-y^2} channels are also competitive in the magnetically frustrated J1∼J2J_1 \sim J_2 parameter regime. An A1g+iB1gA_{1g}+i B_{1g} state, which breaks time-reversal symmetry, occurs at low temperatures in part of the phase diagram. Implications for the experiments in the iron pnictides are discussed.

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