Superconductivity triggered or enhanced by light exposure in atomic or quantum systems.Light-induced superconductivity is a phenomenon where exposing certain materials to intense, brief pulses of light can temporarily make them superconduct — conduct electricity with zero resistance — at temperatures far above their normal transition point. This is not the same as conventional superconductivity, which requires cooling materials to extremely low temperatures; here, light energy briefly reorganizes the material's electrons into a paired state that flows without loss. The effect is particularly striking in materials like fullerenes (carbon spheres) and cuprates, where light can trigger superconductivity at or near room temperature, albeit only for picoseconds.
The concept gained prominence in the 2010s, with experiments by Andrea Cavalleri's group at the Max Planck Institute for the Structure and Dynamics of Matter demonstrating light-induced superconductivity in cuprates and fullerenes. The specific mechanism for fullerenes was proposed and tested around 2023–2024.
In a superconductor, electrons form Cooper pairs that move coherently without scattering. Normally, this pairing is mediated by lattice vibrations (phonons) and only occurs at low temperatures. Light pulses can transiently excite the material's lattice or electronic structure, creating a new configuration where pairing is much stronger. For example, in fullerenes, mid-infrared light pulses can distort the molecular lattice, enhancing the coupling between electrons and phonons enough to allow pairing at higher temperatures. The effect is fleeting — the superconducting state decays within a few picoseconds — but it reveals pathways to room-temperature superconductivity that are inaccessible through static conditions.
While the effect is too short-lived for direct technological use, it informs the search for materials that could sustain superconductivity at room temperature, potentially revolutionizing power transmission and magnetic levitation.
In some experiments, light pulses have induced superconductivity in fullerenes at temperatures as high as 100 K, which is about 40 K above their normal superconducting transition temperature.
| β_app | variable | apparent transverse speed in units of c — apparent speed |
| β | variable | actual speed in units of c — vitesse |
| θ | variable | angle between velocity and line of sight — angle radian |
| \sigma | variable | electrical conductivity — electrical conductivity siemens per metre |
| \sigma_0 | variable | pre-exponential factor (conductivity at infinite temperature) — electrical conductivity siemens per metre |
| E_a | variable | activation energy for conduction — énergie joule |
| T | variable | absolute temperature — température kelvin |
| k_B | constante | Relates temperature to energy in statistical mechanics. — constante de Boltzmann = 1.380649e-23 joule per kelvin |
