Electronic and magnetic phase diagram of β-Fe1.01Se with superconductivity at 36.7 K under pressure

S Medvedev, TM McQueen, IA Troyan, T Palasyuk… - Nature materials, 2009 - nature.com
S Medvedev, TM McQueen, IA Troyan, T Palasyuk, MI Eremets, RJ Cava, S Naghavi
Nature materials, 2009nature.com
The discovery of new high-temperature superconductors based on FeAs has led to a new
'gold rush'in high-TC superconductivity. All of the new superconductors share the same
common structural motif of FeAs layers and reach TC values up to 55 K (ref.). Recently,
superconductivity has been reported in FeSe (ref.), which has the same iron pnictide layer
structure, but without separating layers. Here, we report the magnetic and electronic phase
diagram of β-Fe1. 01Se as a function of temperature and pressure. The superconducting …
Abstract
The discovery of new high-temperature superconductors based on FeAs has led to a new ‘gold rush’ in high-TC superconductivity. All of the new superconductors share the same common structural motif of FeAs layers and reach TC values up to 55 K (ref. ). Recently, superconductivity has been reported in FeSe (ref. ), which has the same iron pnictide layer structure, but without separating layers. Here, we report the magnetic and electronic phase diagram of β-Fe1.01Se as a function of temperature and pressure. The superconducting transition temperature increases from 8.5 to 36.7 K under an applied pressure of 8.9 GPa. It then decreases at higher pressures. A marked change in volume is observed at the same time as TC rises, owing to a collapse of the separation between the Fe2Se2 layers. No static magnetic ordering is observed for the whole pT phase diagram. We also report that at higher pressures (starting around 7 GPa and completed at 38 GPa), Fe1.01Se transforms to a hexagonal NiAs-type structure and exhibits non-magnetic behaviour.
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