Abstract

Hollow nanostructures have attracted attention because of their unique physiochemical properties and broad potential applications in electronics, optics and photonics. In this study, a facile hydrothermal approach was developed to fabricate hollow ZnO microspheres via self-assembled rod-like nanostructures. The morphology-controlled synthesis was conducted by altering hydrothermal treatment temperature (150, 200 and 250 °C) in solutions containing zinc acetate dihydrate precursor and glycerol as the stabilizing agent. The morphological observations indicated that hydrothermally grown ZnO architectures could be reasonably adjusted by modulating hydrothermal reaction temperature. Possible growth routes are proposed to elucidate the formation process of ZnO microspheres with the rod-like nanostructures. Morphology-dependent absorbance and emission along with red-shifts with improved crystalline qualities were observed with increasing hydrothermal growth temperature. Kerr-type nonlinear optical characteristics examined using single-beam Z-scan technique in the near infrared spectral range under nanosecond Nd-YVO4 laser pulses showed positive values of nonlinear refraction providing an evidence of self-focusing behaviors at the excitation wavelength of 1064 nm in all the samples studied. The highest Kerr-type nonlinear susceptibility was estimated to be 2.31 × 10–6 esu for hollow ZnO microspheres grown at 250 °C, suggesting synergistic effects of surface morphologies on optical nonlinearities.

Highlights

  • Kerr-type nonlinear optics has been an intensive area of research since the observation of birefringence in 1875 by Scottish physicist John Kerr [1]

  • It can be observed that zinc oxide (ZnO) samples prepared at 150 °C show a strong short-wavelength (SW) emission band around * 398 nm (3.11 eV) along with a weaker long-wavelength (LW) band centered at 670 nm (1.85 eV)

  • The extended emission pattern of SW band is from a combination of near band-gap emissions (NBEs) originating from transitions related to band-edge free excitons and those bound to the shallow states

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Summary

Introduction

Kerr-type nonlinear optics (bound-electronic nonlinear refraction) has been an intensive area of research since the observation of birefringence in 1875 by Scottish physicist John Kerr [1]. The improved Kerr nonlinearities along with reduced linear and nonlinear absorption characteristics provide new possibilities to control nonlinear interactions of optical systems for low light powers showing high sensitivities [4,5,6,7,8]. Such notable achievements have been the inspiration for the development of optical materials garnering the advantages of enhanced Kerr nonlinearities. Li et al demonstrated picosecond Z-scan study of bound electronic Kerr effect in LiNbO3 crystal associated with twophoton absorption [13] In another interesting study, Wang and colleagues measured enhanced Kerr nonlinearity via atomic coherence in a three-level atomic system [14]. According to previously published research articles, the optical bi-stability/multi-stability and its plausible applications in all-optical switching nanodevices can be realized through Kerr nonlinearities by changing the optical anisotropy and geometric parameters [15, 16]

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