On the Thermodynamic Properties of FexSe0.5Te0.5 Superconducting Single Crystals: An Experimental Study
Source abstract
Abstract
The variation of the thermodynamic critical fields (Hc) with temperature has been obtained from the equilibrium magnetization of FexSe0.5Te0.5 superconducting single-crystal with (0.95 ≤ × ≤ 1.1). Based on the BCS theory, we used the Hc values to obtain the variations in the energy gap Δ(T), the cooper pair coupling, the energy gap ratio 2Δ(0)/kBTc, and the specific heat jump {ΔC}BCS/{T}c with varying Fe content. We found that the Cooper pairs coupling strength decreases with increasing Fe content within the range (∼3.1 to 2.6) for 1.0 ≤ × ≤ 1.1, which is consistent with the BCS-weak coupling limit for all samples. Moreover, the value of the energy gap is nearly constant at about 3.5 meV for all samples, while the Hc(0)/Tc ratio reaches a maximum near x ∼ 1.05. The obtained values of the energy gap, the coupling strength, and the specific heat ratio are consistent with recently published results using various experimental techniques.
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Research context
OpenAlex topics: Iron-based superconductors research · Magnetic and transport properties of perovskites and related materials · Rare-earth and actinide compounds
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (42)
Show source-provided references
1. A recent review on iron-based superconductor
2. Superconductivity close to magnetic instability in Fe(Se1−xTex)0.8210.1103/PhysRevB.78.224503 ↗
3. Spontaneous orbital polarization in the nematic phase of FeSe10.1038/s41563-023-01585-2 ↗
4. Pressure effects on FeSe family superconductors10.1016/j.physc.2009.10.098 ↗
5. Superconductivity above 100 K in single-layer FeSe films on doped SrTiO310.1038/nmat4153 ↗
6. Fabrication of binary FeSe superconducting wires by diffusion process10.1063/1.3000616 ↗
7. Enhancement of transition temperature in Fe x Se0.5Te0.5 film via iron vacancies10.1063/1.4886995 ↗
8. Charge-carrier localization induced by excess Fe in the superconductor FeTeSex10.1103/PhysRevB.80.174509 ↗
9. Tunable (δπ, δπ) -type antiferromagnetic order in α-Fe(Te, Se) superconductors10.1103/PhysRevLett.102.247001 ↗
10. Effect of Fe composition on the superconducting properties (Tc, Hc2 and Hirr) of FexSe1/2Te1/2 (x = 0.95, 1.00, 1.05 and 1.10)10.1063/1.3672858 ↗
11. The role of Fe deficiency in FeySe0.5Te0.5 samples prepared by a melting process10.1016/j.physc.2013.05.026 ↗
12. Tuning the superconducting and magnetic properties of FeySe0.25Te0.75 by varying the iron content10.1103/PhysRevB.82.212504 ↗
13. Extreme sensitivity of superconductivity to stoichiometry in Fe1+δSe10.1103/PhysRevB.79.014522 ↗
14. Fe-vacancy order and superconductivity in tetragonal β-Fe1−xSe10.1073/pnas.1321160111 ↗
15. The microstructures and superconducting properties of FeSe0.5Te0.5 bulks with originally milled powders10.1016/j.cryogenics.2013.05.003 ↗
16. Parks · 1969 · 539
17. Superconducting properties of high-purity niobium10.1103/PhysRev.149.231 ↗
18. Strong shift of the irreversibility line in high-Tc superconductors upon vortex shaking with an oscillating magnetic field10.1103/PhysRevB.58.R5940 ↗
19. Scaling of flux pinning with the thermodynamic critical field10.1103/PhysRevB.60.3603 ↗
20. Scaling of the flux pinning in La1.45Nd0.40Sr0.15CuO4 stripe phase superconductor10.1016/S0921-4526(02)01030-X ↗
21. Scaling behavior in aluminum doped MgB2 superconductor10.1007/s10948-012-1879-4 ↗
22. On the thermodynamic critical field in MgB2 superconductor10.1016/j.jallcom.2004.12.050 ↗
23. Salem · 2009
24. Magnetization of hard superconductors10.1103/PhysRevLett.8.250 ↗
25. Reversible magnetization and superconducting-state thermodynamic parameters for underdoped La1.90Sr0.10CuO410.1103/PhysRevB.63.064512 ↗
26. Limitations of the London model for the reversible magnetization of type-II superconductors10.1103/PhysRevLett.67.2371 ↗
27. Comment on ‘Enhanced two-dimensional properties of the four-layered cuprate high-Tc superconductor TlBa2Ca3Cu4Oy’10.1103/PhysRevB.72.176502 ↗
28. The energy gap of the compound FeSe0.5Te0.5 determined by specific heat and point contact spectroscopy10.1016/j.ssc.2015.07.001 ↗
29. Coexistence of weak and strong coupling mechanism, in an iron-based superconductor FeSe0.5Te0.5: possible signature of BCS-BEC crossover10.1007/s10948-017-4103-8 ↗
30. A BCS-like gap in the superconductor SmFeAsO0.85F0.1510.1038/nature07081 ↗
31. Dopant clustering, electronic inhomogeneity, and vortex pinning in iron-based superconductors10.1103/PhysRevB.87.214519 ↗
32. Observation of ordered vortices with Andreev bound states in Ba0.6K0.4Fe2As210.1038/nphys1908 ↗
33. Superconducting energy gap features of FeSe investigated by tunneling spectroscopy on planar junctions10.1007/s10948-015-3364-3 ↗
34. Visible light driven photoluminescence activity of ZnFe2O4 –Ag doped nanomaterials for photostability: green synthesis approach10.1007/s42341-023-00446-8 ↗
35. Investigation of structural, electrical, and magnetic variations of Ni-Zn-Co ferrites by substituting rare Earth Ho3+ for high-frequency applications10.1088/1402-4896/ad3ae0 ↗
36. Local density of states and superconducting gap in the iron chalcogenide superconductor Fe1-δ1+δSe1−x1−xTexx observed by scanning tunneling spectroscopy10.1103/PhysRevB.80.180507 ↗
37. ‘ Electronic correlations and unusual superconducting response in the optical properties of the iron-chalcogenide FeTe0.55Se0.4510.1103/PhysRevB.81.180508 ↗
38. Physical properties of FeSe0.5Te0.5 single crystals grown under different conditions10.1140/epjb/e2010-10473-5 ↗
39. Magnetization of high-field superconductors10.1103/RevModPhys.36.31 ↗
40. Improvement of superconducting properties of FeSe0.5Te0.5 single crystals by Mn substitution10.1088/0953-2048/24/4/045009 ↗
41. Bulk superconductivity at 14 K in single crystals of Fe1+yTexSe1−x10.1103/PhysRevB.79.094521 ↗
42. Meservey · 1969 · 1 · 117