High-Tc superconducting phases in organic molecular intercalated iron selenides: synthesis and crystal structures

2017 ◽  
Vol 53 (70) ◽  
pp. 9729-9732 ◽  
Author(s):  
Shifeng Jin ◽  
Xiao Fan ◽  
Xiaozhi Wu ◽  
Ruijin Sun ◽  
Hui Wu ◽  
...  

Phase pure hybrid iron-based superconductors with various structural types can be obtained by sonochemical insertion of organic molecules into FeSe-layers.

2015 ◽  
Vol 1 (1) ◽  
Author(s):  
W. Zhou ◽  
Z. X. Shi

AbstractSince the discovery of high temperature superconductivity in iron pnictides in 2008, many iron-based superconductors (IBSs) with various crystal structures have been exploited.Among them, superconductivity with the onset transition temperature T


Crystals ◽  
2021 ◽  
Vol 12 (1) ◽  
pp. 20
Author(s):  
Shiv J. Singh ◽  
Mihai I. Sturza

The discovery of iron-based superconductors (FBS) and their superconducting properties has generated huge research interest and provided a very rich physics high Tc family for fundamental and experimental studies. The 1111 (REFeAsO, RE = Rare earth) and 1144 (AEAFe4As4, AE = Ca, Eu; A = K, Rb) families are the two most important families of FBS, which offer the high Tc of 58 K and 36 K with doping and without doping, respectively. Furthermore, the crystal growth of these families is not an easy process, and a lot of efforts have been reported in this direction. However, the preparation of high-quality and suitable-sized samples is still challenging. In this short review, we will summarize the growth of materials with their superconducting properties, especially polycrystals and single crystals, for the 1111 and 1144 families, and make a short comparison between them to understand the developmental issues.


2019 ◽  
Vol 28 (6) ◽  
pp. 067401
Author(s):  
Rui-Jin Sun ◽  
Shi-Feng Jin ◽  
Jun Deng ◽  
Mu-Nan Hao ◽  
Lin-Lin Zhao ◽  
...  

2014 ◽  
Vol 4 (1) ◽  
Author(s):  
Masanori Sunagawa ◽  
Toshihiko Ishiga ◽  
Koji Tsubota ◽  
Taihei Jabuchi ◽  
Junki Sonoyama ◽  
...  

2010 ◽  
Vol 470 ◽  
pp. S416-S417
Author(s):  
Kazuhiko Kuroki ◽  
Hidetomo Usui ◽  
Seiichiro Onari ◽  
Ryotaro Arita ◽  
Hideo Aoki

Author(s):  
A.Q. He ◽  
G.W. Qiao ◽  
J. Zhu ◽  
H.Q. Ye

Since the first discovery of high Tc Bi-Sr-Ca-Cu-O superconductor by Maeda et al, many EM works have been done on it. The results show that the superconducting phases have a type of ordered layer structures similar to that in Y-Ba-Cu-O system formulated in Bi2Sr2Can−1CunO2n+4 (n=1,2,3) (simply called 22(n-1) phase) with lattice constants of a=0.358, b=0.382nm but the length of c being different according to the different value of n in the formulate. Unlike the twin structure observed in the Y-Ba-Cu-O system, there is an incommensurate modulated structure in the superconducting phases of Bi system superconductors. Modulated wavelengths of both 1.3 and 2.7 nm have been observed in the 2212 phase. This communication mainly presents the intergrowth of these two kinds of one-dimensional modulated structures in 2212 phase.


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