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Scientists Discover Quantum Phase Transition in Pressurized Cuprate Superconductors

Feb 21, 2022

The discovery of cuprate high-temperature superconductors in 1986 impacted science and technology considerably and continues to fascinate the communities of condensed matter physics and material sciences because they host the highest ambient-pressure superconducting transition temperature and unconventional electronic behavior. However, the underlying mechanism of the superconductivity is yet an unsolved mystery. Searching for the universal links between the superconducting state and its neighboring quantum states is considered an effective approach to elucidate the high temperature superconducting mechanism.

Recently, Prof. SUN Liling's team from the Institute of Physics (IOP) of the Chinese Academy of Sciences, in collaboration with Profs. XIANG Tao, ZHOU Xingjiang and HU Jiangping Hu from IOP, Prof. GU Genda from the Brookhaven National Laboratory and Prof. LIN Chengtian from the Max Planck Institute, has discovered the pressure-induced quantum transition from superconducting state to insulating-like state in bismuth-based cuprate superconductors, through their state-of-the-art in-situ high-pressure measurements.

These experimental results reveal that the observed quantum phase transition is universal in the bismuth-bearing cuprate superconductors, regardless of the doping level and the number of copper oxide (CuO2) planes in a unit cell.

It is a grand surprise for them that the system enters into an insulating-like state after the superconductivity is fully suppressed, because it is well known that the ground state of the over-hole-doped non-superconducting cuprate is a metallic state, and naively one expects that by applying pressure the bandwidth should be increased.

As a result, the system should become more metallic, instead of insulating-like. This discovery of the universal quantum transition provides a fresh challenge and a new opportunity for better understanding the mechanism of superconductivity in these materials.

This study entitled "Quantum phase transition from superconducting to insulating-like states in a pressurized cuprate superconductor" has been published on Nature Physics.

The study was supported by the National Science Foundation of China, the Ministry of Science and Technology of China, and the Chinese Academy of Sciences.

 

Temperature dependence of in-plane resistance for Bi2Sr2CaCu2O8+δ at different pressures. (a) and (d) are the plots of temperature versus resistance with linear and log scales for the under-doped superconductor; (b) and (e) for the optimally-doped sample, the two-step superconducting transition demonstrates a crossover from two-dimensional to three-dimensional superconducting phases in the pressure range of 4.9- 23.1 GPa, in good agreements with our previous studies; (c) and (f) for the over-doped (OD) sample. (Image by IOP)

 

In-plane resistance (R) and ac susceptibility (Δχ') as a function of temperature (T) for the Bi2Sr2CaCu2O8+δ superconductors at different pressures: (a)-(d) for the under-doped superconductor; (e)-(h) for the optimally-doped superconductor; (i)-(l) for the over-doped superconductor. The blue lines in the figures are the data of Δχ'(T), while the red lines are the data of R(T). The red and blue arrows indicate the temperatures of the onset superconducting transition detected by resistance and ac susceptibility measurements, respectively. (Image by IOP)

 

Pressure-Tc phase diagrams for Bi2Sr2CaCu2O8+δ superconductors. The Right panels are the phase diagrams established by the experimental results from the under-doped (UD), optimally-doped and over-doped samples, together with the mapping information of temperature and pressure dependent R (shown in color scale). The left panel is a normalized phase diagram that is built on the basis of the experimental phase diagrams (the right panels). (Image by IOP)

Contact

SUN Liling

Institute of Physics

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Quantum phase transition from superconducting to insulating-like state in a pressurized cuprate superconductor

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