Abstract

Non-centrosymmetric superconductors, whose crystal structure is absent of inversion symmetry, have recently received special attentions due to the expectation of unconventional pairings and exotic physics associated with such pairings. The newly discovered superconductors A2Cr3As3 (A = K, Rb), featured by the quasi-one dimensional structure with conducting CrAs chains, belongs to such kind of superconductor. In this study, we are the first to report the finding that superconductivity of A2Cr3As3 (A = K, Rb) has a positive correlation with the extent of non-centrosymmetry. Our in-situ high pressure ac susceptibility and synchrotron x-ray diffraction measurements reveal that the larger bond angle of As-Cr-As (defined as α) in the CrAs chains can be taken as a key factor controlling superconductivity. While the smaller bond angle (defined as β) and the distance between the CrAs chains also affect the superconductivity due to their structural connections with the α angle. We find that the larger value of α-β, which is associated with the extent of the non-centrosymmetry of the lattice structure, is in favor of superconductivity. These results are expected to shed a new light on the underlying mechanism of the superconductivity in these Q1D superconductors and also to provide new perspective in understanding other non-centrosymmetric superconductors.

Highlights

  • In order to clarify the correlation between the superconductivity and characteristic lattice parameters, we performed high pressure investigations on the

  • The first drops displayed at higher temperature are the diamagnetic signals from the Pb, and the second drops at lower temperature are from the sample

  • We find that the lattice parameter a of K2Cr3As3 is compressed by ~5%, while the c is reduced by ~2% at the same pressure of 8.16 GPa

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Summary

Method

The K2Cr3As3 single crystals were prepared by the flux method as described in ref. 4. 4. The Rb2Cr3As3 polycrystalline samples are synthesized by solid reaction method, as described in ref. The sample was loaded into a home-made coil which is immersed into the liquid pressure medium in a Teflon capsule and set in the THPC. For the crystal structure refinements of the high pressure XRD data with the Rietveld method[25], the program RIETAN-FP was employed[26,42,43,44], and the ambient-pressure lattice parameters of the host sample were used as Figure 5. (c) Pressure dependences of difference of electron density distribution (∆EDD =EDDCr1 −EDDCr2) at two sites of Cr ions, and Tc for K2Cr3As3. The electron density distributions (EDD) were determined by maximum entropy method (MEM) based on our XRD data with Dysnomia program[45]. The crystal structures and the EDD were visualized using the software package VEST46

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