scholarly journals Magnetism, superconductivity, and pairing symmetry in iron-based superconductors

2008 ◽  
Vol 78 (13) ◽  
Author(s):  
A. V. Chubukov ◽  
D. V. Efremov ◽  
I. Eremin
2014 ◽  
Vol 10 (11) ◽  
pp. 845-850 ◽  
Author(s):  
Z. P. Yin ◽  
K. Haule ◽  
G. Kotliar

2012 ◽  
Vol 26 (20) ◽  
pp. 1230012 ◽  
Author(s):  
ZHU-AN XU ◽  
GUANGHAN CAO ◽  
YUKE LI

The effect of nonmagnetic Zn impurity on superconductivity in iron-based superconductors is reviewed. Zn impurity can severely suppress the antiferromagnetic (AFM) order of Fe ions in the parent compound LaFeAsO . In the 1111 type F-doped LaFeAs ( O , F ) system, the superconducting transition temperature (Tc) increases in the underdoped regime, remains unchanged in the optimally-doped regime, and is severely suppressed in the overdoped regime in the presence of Zn impurity. The results suggest a switch of the symmetry of the superconducting order parameters from a s-wave to s±- or d-wave states as the charge carrier doping increases in this system. To our surprise, Zn impurity strongly suppresses Tc in the Co -doped LaFeAsO and BaFe 2 As 2 systems despite of the Co doping level. The absence of universal Zn impurity effect implies that the pairing symmetry of the iron-based superconductors may be dependent on the details of the electronic structure.


2015 ◽  
Vol 519 ◽  
pp. 65-70 ◽  
Author(s):  
Xiang-Long Yu ◽  
Da-Yong Liu ◽  
Ya-Min Quan ◽  
Xiao-Jun Zheng ◽  
Liang-Jian Zou

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Tsuyoshi Kawashima ◽  
Shigeki Miyasaka ◽  
Hirokazu Tsuji ◽  
Takahiro Yamamoto ◽  
Masahiro Uekubo ◽  
...  

AbstractThe structural flexibility at three substitution sites in LaFeAsO enabled investigation of the relation between superconductivity and structural parameters over a wide range of crystal compositions. Substitutions of Nd for La, Sb or P for As, and F or H for O were performed. All these substitutions modify the local structural parameters, while the F/H-substitution also changes band filling. It was found that the superconducting transition temperature $$T_{\text{c}}$$ T c is strongly affected by the pnictogen height $$h_{Pn}$$ h Pn from the Fe-plane that controls the electron correlation strength and the size of the $$d_{xy}$$ d xy hole Fermi surface (FS). With increasing $$h_{Pn}$$ h Pn , weak coupling BCS superconductivity switches to the strong coupling non-BCS one where electron correlations and the $$d_{xy}$$ d xy hole FS may be important.


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