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Giant THz photoconductivity and possible non-equilibrium superconductivity in metallic K(3)C(60)

The non-equilibrium control of emergent phenomena in solids is an important research frontier, encompassing effects like the optical enhancement of superconductivity (1) . Recently, nonlinear excitation (2 , 3) of certain phonons in bilayer cuprates was shown to induce superconducting-like optical p...

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Detalles Bibliográficos
Autores principales: Mitrano, M., Cantaluppi, A., Nicoletti, D., Kaiser, S., Perucchi, A., Lupi, S., Di Pietro, P., Pontiroli, D., Riccò, M., Clark, S. R., Jaksch, D., Cavalleri, A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4820655/
https://www.ncbi.nlm.nih.gov/pubmed/26855424
http://dx.doi.org/10.1038/nature16522
Descripción
Sumario:The non-equilibrium control of emergent phenomena in solids is an important research frontier, encompassing effects like the optical enhancement of superconductivity (1) . Recently, nonlinear excitation (2 , 3) of certain phonons in bilayer cuprates was shown to induce superconducting-like optical properties at temperatures far above T(c) (4,5,6). This effect was accompanied by the disruption of competing charge-density-wave correlations(7,8), which explained some but not all of the experimental results. Here, we report a similar phenomenon in a very different compound. By exciting metallic K(3)C(60) with mid-infrared optical pulses, we induce a large increase in carrier mobility, accompanied by the opening of a gap in the optical conductivity. Strikingly, these same signatures are observed at equilibrium when cooling metallic K(3)C(60) below the superconducting transition temperature (T(c) = 20 K). Although optical techniques alone cannot unequivocally identify non-equilibrium high-temperature superconductivity, we propose this scenario as a possible explanation of our results.