Pressure Dependence of Superconducting Properties, Pinning Mechanism, and Crystal Structure of the Fe 0.99 Mn 0.01 Se 0.5 Te 0.5 Superconductor
We have investigated the pressure ( ) effect on structural (up to 10 GPa), transport [ ( ): up to 10 GPa], and magnetic [( ( ): up to 1 GPa)] properties and analyzed the flux pinning mechanism of the Fe Mn Se Te superconductor. The maximum superconducting transition temperature ( ) of 22 K with the...
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Veröffentlicht in: | ACS omega 2021-11, Vol.6 (45), p.30419-30431 |
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Hauptverfasser: | , , , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | We have investigated the pressure (
) effect on structural (up to 10 GPa), transport [
(
): up to 10 GPa], and magnetic [(
(
): up to 1 GPa)] properties and analyzed the flux pinning mechanism of the Fe
Mn
Se
Te
superconductor. The maximum superconducting transition temperature (
) of 22 K with the
coefficient of
d
/d
= +2.6 K/GPa up to 3 GPa (d
/d
= -3.6 K/GPa, 3 ≤
≥ 9 GPa) was evidenced from
(
) measurements. The high-pressure diffraction and density functional theory (DFT) calculations reveal structural phase transformation from tetragonal to hexagonal at 5.9 GPa, and a remarkable change in the unit cell volume is observed at ∼3 GPa where the
starts to decrease, which may be due to the reduction of charge carriers, as evidenced by a reduction in the density of states (DOS) close to the Fermi level. At higher pressures of 7.7 GPa ≤
≥ 10.2 GPa, a mixed phase (tetragonal + hexagonal phase) is observed, and the
completely vanishes at 9 GPa. A significant enhancement in the critical current density (
) is observed due to the increase of pinning centers induced by external pressure. The field dependence of the critical current density under pressure shows a crossover from the δ
pinning mechanism (at 0 GPa) to the δ
pinning mechanism (at 1.2 GPa). The field dependence of the pinning force at ambient condition and under pressure reveals the dense point pinning mechanism of Fe
Mn
Se
Te
. Moreover, both upper critical field (
) and
are enhanced significantly by the application of an external
and change over to a high
phase (hexagonal ∼5.9 GPa) faster than a Fe
Ni
Se
Te
(7.7 GPa) superconductor. |
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ISSN: | 2470-1343 2470-1343 |
DOI: | 10.1021/acsomega.1c03721 |