Nonlinear charge oscillation driven by a single-cycle light field in an organic superconductor

Application of an intense light field to solids produces enormous and ultrafast nonlinear phenomena such as high-harmonic generation 1 , 2 and attosecond charge dynamics 3 , 4 . These are distinct from conventional photonics. However, the main targets for investigation have been limited to insulator...

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Published inNature photonics Vol. 12; no. 8; pp. 474 - 478
Main Authors Kawakami, Y., Amano, T., Yoneyama, Y., Akamine, Y., Itoh, H., Kawaguchi, G., Yamamoto, H. M., Kishida, H., Itoh, K., Sasaki, T., Ishihara, S., Tanaka, Y., Yonemitsu, K., Iwai, S.
Format Journal Article
LanguageEnglish
Published London Nature Publishing Group UK 01.08.2018
Nature Publishing Group
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ISSN1749-4885
1749-4893
DOI10.1038/s41566-018-0194-4

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Summary:Application of an intense light field to solids produces enormous and ultrafast nonlinear phenomena such as high-harmonic generation 1 , 2 and attosecond charge dynamics 3 , 4 . These are distinct from conventional photonics. However, the main targets for investigation have been limited to insulators and semiconductors, although theoretical approaches have also been developed for correlated metals and superconductors 5 . Here, in a layered organic superconductor, a nonlinear charge oscillation driven by a nearly single-cycle strong electric field of >10 MV cm −1 is observed as a stimulated emission. The charge oscillation is different from a linear response and ascribed to a polar charge oscillation with a period of ∼6 fs. This nonlinear polar charge oscillation is enhanced by critical fluctuations near a superconducting transition temperature and a critical end-point of first-order Mott transitions. Its observation on an ultrafast timescale of ∼10 fs clarifies that Coulomb repulsion plays an essential role in the superconductivity of organic superconductors. A nonlinear charge oscillation driven by a 6 fs light field of 11 MV cm –1 is observed in a layered organic superconductor. The initial response time of the oscillation on the timescale of 10 fs clarifies that Coulomb repulsion is essential for the superconductivity.
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ISSN:1749-4885
1749-4893
DOI:10.1038/s41566-018-0194-4