Research into superconductors was likewise one of the most important directions for humanity's future, because superconductors had an enormously broad range of applications for mankind. From the most common superconducting power generation, Controlled Nuclear Fusion, and superconducting power transmission to all kinds of Magnetic Levitation trains, cars, and even magnetic levitation skateboards, as long as they existed, they could be developed.
But all of that depended on one condition: a Room-Temperature Superconductor.
In other words, a superconductor that could achieve a superconducting state at room temperature under natural conditions. Yet no such material currently existed.
A few years earlier, there had been reports that bilayer Graphene, twisted at an angle of 1.1 degrees, had achieved superconductivity and seemed to be a Room-Temperature Superconductor. In truth, it did not qualify, because it had to be produced under conditions of 1.7 K—minus 271.45 degrees Celsius.
Therefore, it could not be considered a Room-Temperature Superconductor in the strict sense. For humanity, preparing materials at 1 K was still extraordinarily difficult. Of course, people had never stopped working toward its discovery, but Graphene itself remained relatively expensive to produce, and its applications were even more difficult. So at present, this material could not truly be called a room-temperature superconductor.
Moreover, a superconductor's three parameters—critical transition temperature, critical magnetic field strength, and critical current density—had to all remain within their critical ranges for superconductivity to hold. In actual use, even the natural temperature fluctuations from summer to winter could cause superconductivity to fail.
Sometimes, a shift of merely one or two degrees Celsius could make superconductivity fail. Yet this metal material could achieve superconductivity at Minus 60 Degrees Celsius. More importantly, all three of its critical parameters were extremely high, especially its superconducting temperature range. That meant partial temperature fluctuations would not interrupt its superconducting