Artificial Generation of High Harmonics via Nonrelativistic Thomson Scattering in Metamaterial

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      </button><div class="floats-full-page-caption"><div><b>Geometrical influences on the amplitudes of the transmitted HHG.</b> (a) The gap of the SRR; (b) the distance between two resonators. The amplitudes are normalized to the transmitted second harmonic in<i> y</i> polarization generated by the metamaterial.</div></div><div class="floats-full-page-content"><table class="figure-group"><tr class="fig-image"><td><object data="https://s3-eu-west-1.amazonaws.com/spj-html-parsed-preprod/articles/research/volume-2019/8959285/figures/8959285.fig.006.svgz" name="8959285.fig.006" type="image/svg+xml"></object></td></tr></table></div></div>

Figure 6 | Artificial Generation of High Harmonics via Nonrelativistic Thomson Scattering in Metamaterial

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Figure 6: Artificial Generation of High Harmonics via Nonrelativistic Thomson Scattering in Metamaterial

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