TY - JOUR
T1 - Interplay between Magnetism, Superconductivity, and Orbital Order in 5-Pocket Model for Iron-Based Superconductors
T2 - Parquet Renormalization Group Study
AU - Classen, Laura
AU - Xing, Rui Qi
AU - Khodas, Maxim
AU - Chubukov, Andrey V.
N1 - Publisher Copyright:
© 2017 American Physical Society.
PY - 2017/1/20
Y1 - 2017/1/20
N2 - We report the results of the parquet renormalization group (RG) analysis of the phase diagram of the most general 5-pocket model for Fe-based superconductors. We use as an input the orbital structure of excitations near the five pockets made out of dxz, dyz, and dxy orbitals and argue that there are 40 different interactions between low-energy fermions in the orbital basis. All interactions flow under the RG, as one progressively integrates out fermions with higher energies. We find that the low-energy behavior is amazingly simple, despite the large number of interactions. Namely, at low energies the full 5-pocket model effectively reduces either to a 3-pocket model made of one dxy hole pocket and two electron pockets or a 4-pocket model made of two dxz/dyz hole pockets and two electron pockets. The leading instability in the effective 4-pocket model is a spontaneous orbital (nematic) order, followed by s+- superconductivity. In the effective 3-pocket model, orbital fluctuations are weaker, and the system develops either s+- superconductivity or a stripe spin-density wave. In the latter case, nematicity is induced by composite spin fluctuations.
AB - We report the results of the parquet renormalization group (RG) analysis of the phase diagram of the most general 5-pocket model for Fe-based superconductors. We use as an input the orbital structure of excitations near the five pockets made out of dxz, dyz, and dxy orbitals and argue that there are 40 different interactions between low-energy fermions in the orbital basis. All interactions flow under the RG, as one progressively integrates out fermions with higher energies. We find that the low-energy behavior is amazingly simple, despite the large number of interactions. Namely, at low energies the full 5-pocket model effectively reduces either to a 3-pocket model made of one dxy hole pocket and two electron pockets or a 4-pocket model made of two dxz/dyz hole pockets and two electron pockets. The leading instability in the effective 4-pocket model is a spontaneous orbital (nematic) order, followed by s+- superconductivity. In the effective 3-pocket model, orbital fluctuations are weaker, and the system develops either s+- superconductivity or a stripe spin-density wave. In the latter case, nematicity is induced by composite spin fluctuations.
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U2 - 10.1103/PhysRevLett.118.037001
DO - 10.1103/PhysRevLett.118.037001
M3 - Article
C2 - 28157340
AN - SCOPUS:85010931739
SN - 0031-9007
VL - 118
JO - Physical review letters
JF - Physical review letters
IS - 3
M1 - 037001
ER -