“…Especially, when the pitch size of the array is close to the specific value d c = λ SP / n (where, λ SP is plasmon resonance wavelength and n is the refractive index of the surroundings), the constructive radiative interactions are induced between neighboring nanostructures, leading to a narrower plasmon resonance band compared to that of the isolated nanostructure. , In contrast to the dark plasmon modes, far-field coupling can be easily induced by fabricating periodic arrays of the metallic nanostructures. To date, some groups have reported that the extinction or scattering spectral features of plasmons can be modified by adjusting the periodicity of the arrays, − suggesting that the plasmon dephasing time can be extended by far-field coupling. − However, in the case of the periodic arrays of nanostructures, their spectral characteristics, such as peak wavelength and bandwidth, are seriously modulated by the diffraction or interference effects arising from their periodic spatial arrangement. Therefore, for the arrayed nanostructures, it is difficult to accurately evaluate their plasmon dephasing time from the conventional extinction or scattering spectral measurements, and the temporal confinement effect of light on the arrayed nanostructures remains ambiguous.…”