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Dispersion of the Third-Order Nonlinear Optical Susceptibility in C60 Calculated with a Tight-Binding Model

1992/05/26 by Kikuo Harigaya, Kikuo Harigaya Kikuo Harigaya, Shuji Abe +1 · 1 citation
Chemistry · Engineering · Materials Science · Physics and Astronomy · #Diamond and Carbon-based Materials Research #Fullerene Chemistry and Applications #Nonlinear Optical Materials Studies #cond-mat

paper · pdf · doi:10.1143/jjap.31.l887

published as Jpn. J. Appl. Phys. 31 (1992) L887-L889 · 7 pages, to be published in Jpn. J. Applied Phys. as a Letter

arxiv created 1992/05/26 · openalex publication_date 1992/07/01 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/07/28

Abstract

The frequency dependence of third harmonic generation (THG) in C 60 is calculated, making use of a tight-binding model for π-electrons. The magnitudes of the THG, about 10 -12 esu, near zero frequency, agree with those in experiments for the low-energy region. We can also explain the order of the magnitude, 10 -11 esu, around the three-photon resonance peak due to the lowest allowed excitation, recently measured by Meth et al . At higher energies, we predict a large enhancement of the THG at 3ω∼6 eV as a result of double resonance enhancement.

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