Multigap nodeless superconductivity in the Dirac intermetallic alloy V2Ga5 with one-dimensional vanadium chains
C. Q. Xu, C. C. Zhao, Y. Shen, D. Ratkovski, X. Ma, W. Zhou, Xunqing Yin, B. Li, A. F. Bangura, Chao Cao, Baomin Wang, Ziming Zhu, X. Ke, Dong Qian, Shiyan Li, Xiaofeng Xu
DOI 10.1103/PhysRevB.109.L100506 · Physical Review B
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Abstract
Superconductors possessing diverse symmetry-enforced topological states have been a subject of intense interest as they are arguably one of the most feasible candidates to realize so-called topological superconductivity, a source of Majorana fermions that hold great promise for topological quantum computing. Here we study the low-lying quasiparticle excitations in the superconducting intermetallic alloy V2Ga5 by low-temperature heat capacity and ultra-low-temperature thermal conductivity measurements. It is found that its electronic specific heat can be fitted by either a d-wave gap or two s-wave gaps. However, the low-T thermal conductivity clearly points to the multiple nodeless energy gaps in its low-lying excitation spectrum. On the other hand, first-principles calculations reveal a multitude of topological fermions near the Fermi level, involving discrete Dirac nodes as well as Dirac nodal lines. These topological carriers, when condensed into Cooper pairs, provide a natural platform for achieving topologically nontrivial phases and possible Majorana fermions.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| V2Ga5 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.6 | Pressure not reported | midpoint |
| V2Ga5 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.6 | Pressure not reported | onset |
| V2Ga5 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | 3.6 | Pressure not reported | unknown |
| V3Ga Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Nb3Sn Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| Tl2Ba2CuO6+δ Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
| NbSe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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