A phase of matter in certain superconductors above their critical temperature where resistance grows linearly with temperature and conventional metal theory breaks down.Strange metals are a phase of matter observed in certain high-temperature superconductors and other strongly correlated electron systems. Unlike conventional metals, where electrical resistance decreases with temperature and eventually becomes constant, strange metals exhibit a linear increase in resistance with temperature over a wide range. This behavior defies the standard Fermi liquid theory, which successfully describes ordinary metals. Strange metals are also characterized by a universal scattering rate that is proportional to temperature, hinting at a deep, yet not fully understood, quantum mechanical principle.
The term 'strange metal' was coined in the 1990s to describe the anomalous properties of copper-oxide high-temperature superconductors above their critical temperature. The concept has since been extended to other materials, including heavy-fermion compounds and certain organic conductors.
In ordinary metals, electrons behave as weakly interacting quasiparticles that scatter off impurities and lattice vibrations, leading to a resistance that scales with temperature squared at low temperatures. In strange metals, this quasiparticle picture breaks down: electrons appear to lose their individual identity, and the scattering rate becomes set by temperature alone. This suggests that the electrons are strongly entangled and that quantum fluctuations play a central role, possibly related to a quantum critical point—a phase transition at absolute zero where competing orders fluctuate violently.
Understanding strange metals is crucial for developing room-temperature superconductors, which would revolutionize power transmission, magnetic levitation, and medical imaging. They also serve as a testing ground for new theoretical frameworks beyond Fermi liquid theory.
In strange metals, the electrical resistance increases exactly linearly with temperature, even down to a few kelvin—a behavior that has no analogue in any known conventional metal.











