Multigap superconductivity in ThAsFeN investigated using μSR measurements
Devashibhai Adroja, Amitava Bhattacharyya, Pabitra Kumar Biswas, Michael Smidman, Adrian D. Hillier, Huican Mao, Huiqian Luo, Guang-Han Cao, Zhicheng Wang, Cao Wang
DOI 10.1103/PhysRevB.96.144502 · Physical Review B
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
We have investigated the superconducting ground state of the newly discovered superconductor ThFeAsN with a tetragonal layered crystal structure using resistivity, magnetization, heat capacity, and transverse-field muon-spin rotation (TF−μSR) measurements. Our magnetization and heat-capacity measurements reveal an onset of bulk superconductivity with Tc∼30K. A nonlinear magnetic-field dependence of the specific heat coefficient γ(H) has been found in the low-temperature limit, which indicates that there is a nodal energy gap. Our analysis of the TF−μSR results shows that the temperature dependence of the superfluid density is better described by a two-gap model either isotropic s+s wave or s+d wave than a single-gap isotropic s-wave model for the superconducting gap, consistent with other Fe-based superconductors. The combination of γ(H) and TF−μSR results suggest that the (s+d)-wave model is the most consistent candidate for the gap structure of ThFeAsN. The observation of two gaps in ThFeAsN suggests a multiband nature of the superconductivity possibly arising from the d bands of Fe ions. Furthermore, from our TF−μSR study we have estimated the magnetic penetration depth in the polycrystalline sample of λL(0)=375nm, superconducting carrier density ns=4.97×1027m−3, and carrier's effective-mass m*=2.48me. We compare the results of our present paper with those reported for the Fe-pnictide families of superconductors.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| ThFeAsN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 30 | Pressure not reported | onset |
| ThFeAsN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 30 | Pressure not reported | onset |
| ThFeAsN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 30 | Pressure not reported | onset |
| ThFeAsN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 30 | Pressure not reported | onset |
| LaFeAsO1-xFx Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 26 | Pressure not reported | unknown |
Similar papers
Bulk superconductivity at 14 K in single crystals of Fe1+yTexSe1−x
similarity 0.94B. C. Sales et al.
Source status unknown — claims are unverified
Superconductivity at 43 K at ambient pressure in the iron-based layered compound La1−xYxFeAsOy
similarity 0.94Parasharam M. Shirage et al.
Source status unknown — claims are unverified
Exploring multichannel superconductivity in ThFeAsN
similarity 0.94Fabian Schrodi et al.
Source status unknown — claims are unverified
Electronic structure, lattice dynamics, and magnetic properties of ThXAsN (X=Fe,Co,Ni) superconductors: A first-principles study
similarity 0.93Smritijit Sen & Guang-Yu Guo
Source status unknown — claims are unverified
Pressure effects on the electronic properties of the undoped superconductor ThFeAsN
similarity 0.93N. Barbero et al.
Source status unknown — claims are unverified
Multigap superconductivity in ThAsFeN investigated using muSR measurements
similarity 0.93Devashibhai Adroja et al. · 2017 · arXiv:1706.03641
Source status unknown — claims are unverified