TY - JOUR
T1 - Magnetic phases in superconducting, polycrystalline bulk FeSe samples
AU - Nouailhetas, Quentin
AU - Koblischka-Veneva, Anjela
AU - Koblischka, Michael R.
AU - Naik, Pavan Kumar S.
AU - Schäfer, Florian
AU - Ogino, H.
AU - Motz, Christian
AU - Berger, Kévin
AU - Douine, Bruno
AU - Slimani, Yassine
AU - Hannachi, Essia
N1 - Funding Information:
This work is part of the SUPERFOAM international project funded by ANR and DFG under the references ANR-17-CE05-0030 and DFG-ANR Ko2323-10, respectively. HO and SPKN gratefully acknowledge the support by JSPS KAKENHI, Grant Number JP16H6439. SPKN also wishes to thank JSPS for the fellowship (Grant No. P19354).
Publisher Copyright:
© 2021 Author(s).
PY - 2021/1/1
Y1 - 2021/1/1
N2 - The FeSe compound is the simplest high-temperature superconductor (HTSc) possible, and relatively cheap, not containing any rare-earth material. Although the transition temperature, Tc, is just below 10 K, the upper critical fields are comparable with other HTSc. Preparing FeSe using solid-state sintering yields samples exhibiting strong ferromagnetic hysteresis loops (MHLs), and the superconducting contribution is only visible after subtracting MHLs from above Tc. Due to the complicated phase diagram, the samples are a mixture of several phases, the superconducting β-FeSe, and the non-superconducting δ-FeSe and γ-FeSe. Furthermore, antiferromagnetic Fe7Se8 and ferromagnetic α-Fe may be contained, depending directly on the Se loss during the sintering process. Here, we show MHLs measured up to ±7 T and determine the magnetic characteristics, together with the amount of superconductivity determined from M(T) measurements. We also performed a thorough analysis of the microstructures in order to establish a relation between microstructure and the resulting sample properties.
AB - The FeSe compound is the simplest high-temperature superconductor (HTSc) possible, and relatively cheap, not containing any rare-earth material. Although the transition temperature, Tc, is just below 10 K, the upper critical fields are comparable with other HTSc. Preparing FeSe using solid-state sintering yields samples exhibiting strong ferromagnetic hysteresis loops (MHLs), and the superconducting contribution is only visible after subtracting MHLs from above Tc. Due to the complicated phase diagram, the samples are a mixture of several phases, the superconducting β-FeSe, and the non-superconducting δ-FeSe and γ-FeSe. Furthermore, antiferromagnetic Fe7Se8 and ferromagnetic α-Fe may be contained, depending directly on the Se loss during the sintering process. Here, we show MHLs measured up to ±7 T and determine the magnetic characteristics, together with the amount of superconductivity determined from M(T) measurements. We also performed a thorough analysis of the microstructures in order to establish a relation between microstructure and the resulting sample properties.
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U2 - 10.1063/9.0000167
DO - 10.1063/9.0000167
M3 - Article
AN - SCOPUS:85099394757
SN - 2158-3226
VL - 11
JO - AIP Advances
JF - AIP Advances
IS - 1
M1 - 015230
ER -