TY - JOUR
T1 - Mean-field state population study for iron-based superconductors
AU - Wang, Zhigang
AU - Fu, Zhen Guo
AU - Zheng, Fa Wei
AU - Zhang, Ping
N1 - Publisher Copyright:
© 2017 Elsevier B.V.
PY - 2017/2/26
Y1 - 2017/2/26
N2 - The occupation number distribution in momentum space are theoretically studied within a two-orbital model, which can be unified describing the low-energy physics of the iron pnictides and iron chalcogenides. The mean-field approximation of Hubbard interaction is employed. By tuning the hopping parameters, the difference between the iron pnictides and iron chalcogenides in their occupation number distribution behavior can be clearly observed. The results show that when the pairing interaction tends to zero, the occupation number n(k)≈0 at Γ point for iron chalcogenides while n(k)≈2 at Γ point for iron pnictides. By increasing the strength of the pairing interaction to a large value, the change of n(k) at Γ point for iron chalcogenides (pnictides) is remarkable (unremarkable). In addition, we find that the effect of the nearest-neighbor coupling between the two layers, contained in the S4 model [Hu and Hao, (2012) [33]], is very weak.
AB - The occupation number distribution in momentum space are theoretically studied within a two-orbital model, which can be unified describing the low-energy physics of the iron pnictides and iron chalcogenides. The mean-field approximation of Hubbard interaction is employed. By tuning the hopping parameters, the difference between the iron pnictides and iron chalcogenides in their occupation number distribution behavior can be clearly observed. The results show that when the pairing interaction tends to zero, the occupation number n(k)≈0 at Γ point for iron chalcogenides while n(k)≈2 at Γ point for iron pnictides. By increasing the strength of the pairing interaction to a large value, the change of n(k) at Γ point for iron chalcogenides (pnictides) is remarkable (unremarkable). In addition, we find that the effect of the nearest-neighbor coupling between the two layers, contained in the S4 model [Hu and Hao, (2012) [33]], is very weak.
KW - Hubbard interaction
KW - Iron-based superconductors
KW - Mean-field approximation
UR - http://www.scopus.com/inward/record.url?scp=85009477613&partnerID=8YFLogxK
U2 - 10.1016/j.physleta.2016.12.042
DO - 10.1016/j.physleta.2016.12.042
M3 - Article
AN - SCOPUS:85009477613
SN - 0375-9601
VL - 381
SP - 808
EP - 812
JO - Physics Letters, Section A: General, Atomic and Solid State Physics
JF - Physics Letters, Section A: General, Atomic and Solid State Physics
IS - 8
ER -