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arxiv: 1412.2596 · v2 · pith:5U3GCP2Xnew · submitted 2014-12-08 · ❄️ cond-mat.supr-con · cond-mat.mtrl-sci· cond-mat.str-el

Unconventional superconductivity in quasi-one-dimensional Rb₂Cr₃As₃

classification ❄️ cond-mat.supr-con cond-mat.mtrl-scicond-mat.str-el
keywords superconductivitytemperaturequasi-one-dimensionalunconventionalzeroaboveanalogousanother
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Following the discovery of superconductivity in quasi-one-dimensional K$_2$Cr$_3$As$_3$ containing [(Cr$_3$As$_3$)$^{2-}$]$_{\infty}$ chains [J. K. Bao et al., arXiv: 1412.0067 (2014)], we succeeded in synthesizing an analogous compound, Rb$_2$Cr$_3$As$_3$, which also crystallizes in a hexagonal lattice. The replacement of K by Rb results in an expansion of $a$ axis by 3\%, indicating a weaker interchain coupling in Rb$_2$Cr$_3$As$_3$. Bulk superconductivity emerges at 4.8 K, above which the normal-state resistivity shows a linear temperature dependence up to 35 K. The estimated upper critical field at zero temperature exceeds the Pauli paramagnetic limit by a factor of two. Furthermore, the electronic specific-heat coefficient extrapolated to zero temperature in the mixed state increases with $\sqrt{H}$, suggesting existence of nodes in the superconducting energy gap. Hence Rb$_2$Cr$_3$As$_3$ manifests itself as another example of unconventional superconductor in the Cr$_3$As$_3$-chain based system.

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