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@@ -144,7 +144,7 @@
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optical response has recently emerged as a powerful tool for ultrafast
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all-optical modulation at nanoscale. A strong modulation can be
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achieved via photo-generation of dense electron-hole plasma in the
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- regime of simultaneous excitation of electric and magnetic optical
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+ regime of simultaneous excitation of electric and magnetic Mie
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resonances, resulting in an effective transient reconfiguration of
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nanoparticle scattering properties. However, only homogeneous plasma
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generation was previously considered in the photo-excited
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@@ -208,7 +208,7 @@ All-dielectric nonlinear nanophotonics based on high refractive index
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dielectric materials has become prospective paradigm in modern optics, owing to
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recent advances in harmonics generation~\cite{shcherbakov2014enhanced,
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yang2015nonlinear, makarov2016self, shorokhov2016multifold,
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- makarov2017efficient} and ultrafast all-optical
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+ makarov2017efficient, makarov2017light} and ultrafast all-optical
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modulation~\cite{iyer2015reconfigurable, makarov2015tuning,
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shcherbakov2015ultrafast, yang2015nonlinear, baranov2016nonlinear,
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baranov2016tuning, shcherbakov2017ultrafast}. In fact,
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@@ -224,7 +224,7 @@ to significant changes in optical properties (transmittance or
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reflectance) of all-dielectric nanoantennas~\cite{makarov2015tuning,
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baranov2016nonlinear, baranov2016tuning} and
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metasurfaces~\cite{iyer2015reconfigurable, shcherbakov2015ultrafast,
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- yang2015nonlinear, shcherbakov2017ultrafast, makarov2017light}.
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+ yang2015nonlinear, shcherbakov2017ultrafast}.
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In previous works on all-dielectric nonlinear nanostructures, the
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building blocks (nanoparticles) were considered as objects with
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Sergey Makarov