Novel BiS2-based layered superconductor Bi4O4S3

TL;DR

This paper reports the discovery of superconductivity in a new layered bismuth-oxysulfide compound Bi4O4S3, highlighting its unique structure and electronic properties, and suggesting a new class of layered superconductors.

Contribution

The study introduces a novel BiS2-based layered superconductor, expanding the family of layered superconductors and providing insights into its structure and electronic characteristics.

Findings

Bi4O4S3 exhibits superconductivity with a transition temperature (Tc) of approximately 4.5 K.

The compound has a layered structure with Bi4O4(SO4)1-x and Bi2S4 layers, with the parent compound being an insulator.

Band calculations indicate the Fermi level is on a peak of the Bi 6p orbital density of states within the BiS2 layer.

Abstract

Exotic superconductivity has often been discovered in materials with a layered (two-dimensional) crystal structure. The low dimensionality can affect the electronic structure and can realize high transition temperatures (Tc) and/or unconventional superconductivity mechanisms. As standard examples, we now have two types of high-Tc superconductors. The first group is the Cu-oxide superconductors whose crystal structure is basically composed of a stacking of spacer (blocking) layers and superconducting CuO2 layers.1-4 The second group is the Fe-based superconductors which also possess a stacking structure of spacer layers and superconducting Fe2An2 (An = P, As, Se, Te) layers.5-13 In both systems, dramatic enhancements of Tc are achieved by optimizing the spacer layer structure, for instance, a variety of composing elements, spacer thickness, and carrier doping levels with respect to the superconducting layers. In this respect, to realize higher-Tc superconductivity, other than Cu-oxide and Fe-based superconductors, the discovery of a new prototype of layered superconductors needs to be achieved. Here we show superconductivity in a new bismuth-oxysulfide layered compound Bi4O4S3. Crystal structure analysis indicates that this superconductor has a layered structure composed of stacking of Bi4O4(SO4)1-x and Bi2S4 layers; the parent compound (x = 0) is Bi6O8S5. Band calculation suggests that Bi4O4S3 (x = 0.5) is metallic while Bi6O8S5 (x = 0) is a band insulator with Bi3+. Furthermore, the Fermi level for Bi4O4S3 is just on the peak position of the partial density of states of the Bi 6p orbital within the BiS2 layer. The BiS2 layer is a basic structure which provides another universality class for layered superconducting family, and this opens up a new field in the physics and chemistry of low-dimensional superconductors.