论文标题
高压结构和磁通型关于II型DIRAC半准候选IR2In8S的研究:减压后超导性的出现
High pressure structural and magneto-transport studies on type-II Dirac semimetal candidate Ir2In8S: Emergence of superconductivity upon decompression
论文作者
论文摘要
在高压下,已经研究了II DIRAC半准候选IR2in8的结构和磁传输特性。发现环境四方结构(p4_2/mnm)稳定至7 GPA,在上面,系统采用正交性PNNM结构,可能会由于四倍螺钉对称性而破坏Dirac锥。在四方结构中,对横向磁电阻的逐渐抑制和高于50k的磁场依赖性的快速变化表明可能依赖于t依赖的费米表面修饰。在高压阶段,金属特性略有增加(从增加的RRR值中可以明显看出),并伴有抑制磁阻塞,而没有超导性的出现,高达20 GPA,且下降至1.4K。最令人惊讶的是,在将压力释放到0.2 GPA时,观察到低于4K的急剧阻力下降,场的变化测量结果证实了这是超导性的开始。在压力释放的四方相中,观察到的载体密度和迁移率的变化表明由不可逆的多面体失真引起的电子结构修饰。减压时残留电阻率和载体密度的同时增加表明,增强的杂质散射在四方IR2IN8S中超导性的出现中起着关键作用,使其成为研究拓扑超导性的理想平台。
The structural and magneto-transport properties of type-II Dirac semimetal candidate Ir2In8S have been investigated under high pressure. The ambient tetragonal structure (P4_2/mnm) is found to be stable up to 7 GPa, above which the system takes an orthorhombic Pnnm structure, possibly destroying the Dirac cones due to the loss of the four-fold screw symmetry. In the tetragonal structure, a gradual suppression of the transverse magneto-resistance and a rapid change in the magnetic field dependence above 50K suggest possible T-dependent Fermi surface modification. In the high pressure phase, the metallic character increases marginally (as evident from the increased RRR value) accompanied with suppressed magneto-resistance, without emergence of superconductivity up to 20 GPa and down to 1.4K. Most surprisingly, upon release of pressure to 0.2 GPa, a sharp resistance drop below 4K is observed, field varying measurements confirm this as the onset of superconductivity. The observed changes of the carrier density and mobility in the pressure-released tetragonal phase indicate electronic structural modification resulting from the irreversible polyhedral distortion. A simultaneous increase in the residual resistivity and carrier density upon decompression indicates that an enhanced impurity scattering play a key role in the emergence of superconductivity in the tetragonal Ir2In8S, making it an ideal platform to study topological superconductivity.