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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...
Autores principales: | , , , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
2016
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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 |
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. |
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