论文标题
在莫特金属中截断的质量差异
Truncated mass divergence in a Mott metal
论文作者
论文摘要
在干净,晶体固体中的金属 - 绝缘体转变可以由两种不同的机制驱动。在常规的绝缘子中,当能量隙分离填充和未填充的电子状态时,电荷载体浓度就会消失。相比之下,在已建立的莫特绝缘子的图像中,电子相互作用会导致连贯的电荷载体减速并最终停在电子锁中,而不会严重影响载体浓度本身。到目前为止,该描述通过量子振荡测量结果逃脱了实验验证,该测量直接探测了相干电荷载体的速度分布。通过将该技术扩展到高压,我们能够检查载体浓度和速度在清洁,结晶材料的密切相关的金属状态下的速度的演变,同时将系统调整为莫特绝缘阶段。我们的结果证实,明显的电子减慢确实控制着绝缘状态的方法。但是,临界点本身,即载体速度将达到零并且有效的载体质量差异,这是相位图的绝缘部门隐藏的。在最终的莫特定位视图中,低温莫特临界点的无法访问类似于干净的金属系统中磁性阈值的阈值,在干净的金属系统中,临界点几乎被一阶转变,三个智力行为或新颖的新出现阶段(例如不可行的超导不可传导性)普遍中断。
Metal-insulator transitions in clean, crystalline solids can be driven by two distinct mechanisms. In a conventional insulator, the charge carrier concentration vanishes, when an energy gap separates filled and unfilled electronic states. In the established picture of a Mott insulator, by contrast, electronic interactions cause coherent charge carriers to slow down and eventually stop in electronic grid-lock without materially affecting the carrier concentration itself. This description has so far escaped experimental verification by quantum oscillation measurements, which directly probe the velocity distribution of the coherent charge carriers. By extending this technique to high pressure we were able to examine the evolution of carrier concentration and velocity in the strongly correlated metallic state of the clean, crystalline material NiS$_2$, while tuning the system towards the Mott insulating phase. Our results confirm that pronounced electronic slowing down indeed governs the approach to the insulating state. However, the critical point itself, at which the carrier velocity would reach zero and the effective carrier mass diverge, is concealed by the insulating sector of the phase diagram. In the resulting, more nuanced view of Mott localisation, the inaccessibility of the low temperature Mott critical point resembles that of the threshold of magnetic order in clean metallic systems, where criticality is almost universally interrupted by first order transitions, tricritical behaviour or novel emergent phases such as unconventional superconductivity.