Abstract
We report the discovery of superconductivity with Tc = 5.5 K in Nb2PdxSe5, in which one-dimensional (1D) Nb–Se chains existing along the b-direction hybridize each other to form the conducting b–c* plane. The magnetic susceptibility and specific heat data in both single crystal and polycrystal show evidence of bulk superconductivity. The resistivity, Hall coefficient and magneto-resistance data all indicate the presence of an energy scale T* = ∼ 50 K, which becomes systematically lowered under hydrostatic pressure and competes with the stabilization of superconductivity. Combined with the band calculation results showing the Fermi surfaces with 1D character, we postulate that the energy scale T* is related to the formation of a density wave or a stabilization of low-dimensional electronic structure. The zero-temperature upper critical field, Hc2(0), of the single crystal is found to be 10.5, 35 and 22 T in the a′, b and c* directions, respectively. While the linearly increasing Hc2(T) for H//c* indicates the multi-band effect, Hc2(0) for H//b and c* are found to be much bigger than the Bardeen–Cooper–Schrieffer (BCS) Pauli limiting field, 1.84 Tc ∼ 9 T. The suppressed Pauli paramagnetic effect points to the possibility of enhanced spin–orbit scattering related to the low-dimensional electronic structure or the presence of heavy elements such as Pd.
Highlights
The quasi one-dimensional (q1D) electronic structure is a fertile playground to search for novel states in strongly correlated materials
Interesting phenomena can be observed in the q1D materials upon applying a magnetic field, whose energy scale is comparable to their inter-chain interaction
We found a perfect Meissner shielding in the magnetic susceptibility and confirmed bulk superconductivity at Tc = 5.5 K by the specific heat measurements
Summary
The quasi one-dimensional (q1D) electronic structure is a fertile playground to search for novel states in strongly correlated materials. 3.4 Transport properties under hydrostatic pressure Resistivity measurements under hydrostatic pressure were performed on another piece of a single crystal showing an even steeper resistivity increase at low temperatures below ~ 50 K. the resistivity upturn was gradually suppressed upon increasing pressure to induce the metallic ground state down to Tc. In each pressure, T* was determined by an intersection temperature of the two linearly extrapolated lines in the ρ(T) curve below and above the transition and Tc was determined at which 50 % of the normal state resistivity is realized.
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