Elsevier

Materials Characterization

Volume 106, August 2015, Pages 185-194
Materials Characterization

Structural- and optical-property characterization of three-dimensional branched ZnO nanospikes

https://doi.org/10.1016/j.matchar.2015.05.031Get rights and content

Highlights

  • Pyrolysis of zinc stearate in synthesizing 3-D ZnO nanospikes

  • ZnO nanospikes possess bundle of nanorods that sprout out from the hexagonal stump

  • Growth mechanism is deduced to elucidate the morphological evolution from nanobullet to nanospike with branching topology

  • PL spectrum indicate that the nanospike exhibit prominent visible-light emission that ranged from green- to red-region

Abstract

Current study reports the synthesis of three-dimensional (3-D) ZnO nanospikes with anomalous optical property, where zinc stearate is adopted as a safe, common and low-cost precursor that undergoes thermal pyrolysis under non-hydrolytic approach. High resolution transmission electron microscope (HRTEM) and scanning electron microscope (SEM) result show that the as-synthesized 3-D ZnO nanospikes are constructed by bundle of nanorods that sprout radially outwards in random orientation. The possible growth mechanism is discussed by referring to the microscopy results. X-ray diffraction (XRD) pattern confirms that the nanospikes are highly crystalline, which existed in hexagonal wurtzite crystal structure. Optical absorption characterization shows that the onset absorption for the nanospikes is slightly red-shifted if compared to commercial ZnO and the corresponding bandgap energy is estimated to be 3.1 eV. The photoluminescene (PL) result of ZnO nanospikes indicate that its optical emission exhibits weak UV emission but very intense visible-light emission that ranged from green- up to red-region. The factors that contributed to the intriguing PL characteristic are discussed. Current finding would offer a versatile synthesis scheme in engineering advanced nanostructures with new design that exhibit congruent optical property.

Introduction

ZnO is an ideal semiconductor material that shows high potential to be used in various optical devices such as LEDs [1], sensors [2], [3], and solar cells [4]. Its wide bandgap (3.36 eV at RT) as well as large exciton binding energy (60 meV) has continued motivate researchers worldwide to unravel its attractive optical characteristic [5] particularly the origin of the visible-light photo-emission (from green up to red region). Various mechanisms have been hypothesized to explain the reasons behind this anomalous optical feature, with particularly on the aspect of defect induced deep level emission. It has been identified that numerous reasons can be accounted for this optical phenomenon, which consisted of geometrical effects [6], crystal imperfection [7], impurities [8], deviation stoichiometry [9] or dopant effects [10]. Therefore, all these possible reasons had been taken into account during the formulation of ZnO as an efficient route in engineering ZnO with sophisticated optical characteristics.

With respect to the aforementioned reasons, geometrical factor (such as size and shape) is one of the crucial factors that can be used in tailoring the physical and chemical properties, which will strictly-govern the optical characteristics. For few decades, researchers have been working actively in fine-tuning the optical characteristic of ZnO nanostructures by exploring various types of efficient synthetic schemes in producing ZnO nanostructures with a controlled size and shape. Among these include physical method synthesis in the controlled growth of advanced nanostructures ranged from 0-D [11], 1-D [12], [13], 2-D [5], [14] and even up to 3-D [15], [16]. In conjunction with this, wet chemistry synthesis through nonhydrolytic colloidal approach also provides a facile yet reproducible route in synthesizing nanostructures that are highly monodispersed in size as well as possesses well-defined shape. This offers a merit for the as-produced nanostructures to be easily dispersed in either organic or aqueous media for variety applications such as organic-based LED applications [17] or biological labelling [18]. Generally, the synthesis via nonhydrolytic colloidal approach is particularly suitable for oxide-based nanomaterial preparation, where it is realized by pyrolysis of molecular precursor (in the form of organometallic compounds) and it offers an effective route for the precisely-controlled nanostructures with advanced nano-architecture. Under finite induction period with sufficient supplying of the heat, the as-obtained nanostructures could own excellent crystallinity and uniformity in terms of both size and shapes. Moreover, both isotropic and anisotropic products can easily be obtained by manipulating the growth parameters such as choice of the molecular precursor and capping ligands, the reaction duration and growth temperature [19].

Hereby, for the first time, we successfully use zinc-stearate (Zn(C18H35O2)2), an environmentally benign metal-soap precursor for the controlled-synthesis of 3-D ZnO nanospikes. Current study demonstrates a single step nonhydrolytic reaction instead of multiple step synthesis in the producing of truly 3-D ZnO nanostructures as compared to earlier reports [20], [21]. Systematic characterization on the as-synthesized ZnO nanospikes has been carried out to probe its structural- and optical-property. The nanospikes exhibit branched topology with good crystallinity, in which bundle of nanorods that sprout radially outwards in three-dimensional space to form spiky nanostructure. The possible growth mechanism is deduced based on the microscopy results. Moreover, the optical measurement indicates the absorption onset of nanospikes is red shifted; while its PL spectra reveal a weak UV-light emission but strong visible-light emission (ranged from green up to red region). The possible reasons accounted for these emissions are also discussed.

Section snippets

Experimental details

All chemicals were used as received without further purification. The reaction was performed in an inert atmosphere under continuous flow of argon (Ar) gas. In a typical synthesis, 3.3 mmol of zinc stearate (Zn(C18H35O2)2, Meryer Chemicals), 1.5 mmol of oleylamine (C18H37N, Sigma-Aldrich, technical grade 70%) and 50 mL of n-octadecene (C18H36, Sigma-Aldrich, technical grade 90%) were loaded into a 250 mL four neck flask equipped with an Allihn condenser. The mixture was heated to 180 °C for 1 h by

Result and discussion

Fig. 1(a) shows the low-magnification TEM micrograph for the as-synthesized ZnO nanospikes with average dimension of 200 nm. It is perceived that the nanospikes are constructed by bundle of nanorods which are bound together at a neck that located at one end of the rectangular basement (or the so-called stump afterwards). Occasionally, it is observed that some of the nanospikes appear to have smaller dimension due to incomplete grow, where the densities of the nanorods are found to be lower as

Conclusion

In summary, 3-D ZnO nanospikes have been successfully synthesized by pyrolysis of zinc stearate through organometallic approach for the first time. The as-synthesized ZnO nanospikes are constructed by the bundle of nanorods that are stacked randomly in three-dimensional space and exhibit good crystallinity. The X-ray diffraction and Raman spectra confirm the formation of ZnO with hexagonal wurtzite phase. The optical bandgap energy of the as-synthesized nanospikes is calculated to be 3.1 eV and

Acknowledgements

The financial support by Chancellory of University Malaya under High Impact Research Grant (HIR-UM) (J-21002-73810) and HIR-MOHE (UM.C/625/1/HIR/MOHE/SC/06) are acknowledged. W. S. Chiu is also grateful for the research grants that funded by the Ministry of Science, Technology and Innovation (MOSTI) (ScienceFund: 03-01-03-SF0658), Ministry of Higher Education (MOHE) (FRGS: FP-038-2014B; ERGS: ER002-2013A) and University Malaya Research Grant (UMRG: RP007B-13AFR). S. N. H. Daud would like to

References (67)

  • N. Soltani et al.

    Photocatalytic degradation of methylene blue under visible light using PVP-capped ZnS and CdS nanoparticles

    Sol. Energy

    (2013)
  • V. Khranovskyy et al.

    Comparative PL study of individual ZnO nanorods, grown by APMOCVD and CBD techniques

    Phys. B Condens. Matter

    (2012)
  • A. Singh et al.

    Synthesis, effect of capping agents, structural, optical and photoluminescence properties of ZnO nanoparticles

    J. Lumin.

    (2009)
  • Y. Wang et al.

    Catalytic growth of semiconducting zinc oxide nanowires and their photoluminescence properties

    J. Cryst. Growth

    (2002)
  • A. Ghosh et al.

    Effect of annealing on structural and optical properties of zinc oxide thin film deposited by successive ionic layer adsorption and reaction technique

    J. Alloys Compd.

    (2009)
  • J.H. Lim et al.

    UV electroluminescence emission from ZnO light‐emitting diodes grown by high‐temperature radiofrequency sputtering

    Adv. Mater.

    (2006)
  • N. Kumar et al.

    Ultrasensitive DNA sequence detection using nanoscale ZnO sensor arrays

    Nanotechnology

    (2006)
  • M. Law et al.

    Nanowire dye-sensitized solar cells

    Nat. Mater.

    (2005)
  • M. Ghosh et al.

    Shape transition in ZnO nanostructures and its effect on blue–green photoluminescence

    Nanotechnology

    (2008)
  • T. Voss et al.

    Influence of exciton–phonon coupling on the energy position of the near-band-edge photoluminescence of ZnO nanowires

    Appl. Phys. Lett.

    (2006)
  • V.A. Fonoberov et al.

    Photoluminescence investigation of the carrier recombination processes in ZnO quantum dots and nanocrystals

    Phys. Rev. B

    (2006)
  • S. Mahamuni et al.

    Spectroscopic and structural characterization of electrochemically grown ZNO quantum dots

    J. Appl. Phys.

    (1998)
  • M. Yin et al.

    Zinc oxide quantum rods

    J. Am. Chem. Soc.

    (2004)
  • X. Wang et al.

    Low-temperature growth and properties of ZnO nanowires

    Appl. Phys. Lett.

    (2004)
  • M. Fu et al.

    ZnO nanosheet with ordered pore periodicity via colloidal crystal template assisted electrochemical deposition

    Adv. Mater.

    (2006)
  • Q. Xie et al.

    Synthesis of ZnO three-dimensional architectures and their optical properties

    Solid State Commun.

    (2005)
  • S. Cho et al.

    Exposed crystal face controlled synthesis of 3D ZnO superstructures

    Langmuir

    (2010)
  • V. Wood et al.

    Air-stable operation of transparent, colloidal quantum dot based LEDs with a unipolar device architecture

    Nano Lett.

    (2009)
  • M. Bruchez et al.

    Semiconductor nanocrystals as fluorescent biological labels

    Science

    (1998)
  • M. Casavola et al.

    Topologically controlled growth of magnetic-metal-functionalized semiconductor oxide nanorods

    Nano Lett.

    (2007)
  • K. Sun et al.

    3D branched nanowire heterojunction photoelectrodes for high-efficiency solar water splitting and H 2 generation

    Nanoscale

    (2012)
  • H. Zhang et al.

    Self-assembly fabrication of 3D flower-like ZNO hierarchical nanostructures and their gas sensing properties

    CrystEngComm

    (2012)
  • P.X. Gao et al.

    Metal/semiconductor core/shell nanodisks and nanotubes

    Adv. Funct. Mater.

    (2006)
  • Cited by (15)

    • Defects and dopant alliance towards bound magnetic polarons formation and mixed magnetic characteristics in Fe doped ZnO nanoparticles

      2020, Journal of Industrial and Engineering Chemistry
      Citation Excerpt :

      Saikia et al. have observed such emissions to be fixed at 390 nm for ZnO NPs despite having different morphologies [44]. The violet emission peak located around 422–424 nm may originate due to several reasons such as Zni occupying grain boundaries [45], electrons confined to Zni recombination with the holes of the VB [46], movement of CB electrons to recombine with Oi defect (lying 0.4 eV above the VB) [47] and VZn related defects [48]. In this study, this peak is significantly close to that (∼425 nm) observed by Kumar et al. who assigned it to be caused by the recombination processes between the VB and Zni defects [49].

    • ZnO branched p-Cu<inf>x</inf>O @n-ZnO heterojunction nanowires for improving acetone gas sensing performance

      2020, Sensors and Actuators, B: Chemical
      Citation Excerpt :

      However, comparing to core-shell nanomaterial heterostructures, the branched core-shell nanomaterials are more promising for improving the gas detection ability due to the enhanced surface area and the improved gas absorption capacity [24]. It is known that the different characteristics including the shape and size of the stem and branches have the great influence on the chemical and physical properties of nanostructures which will eventually affect the gas sensing performance [25]. Based on the stem-branch heterostructure, the main factors affecting the gas sensing properties include the surface depletion area on the stem and branched NWs, and the additional potential barrier between the heterojunction interfaces [26].

    • Phase segregation induced third order nonlinear saturable absorption behavior in Erbium doped ZnO nanoparticles synthesized by facile hydrothermal method

      2020, Physica E: Low-Dimensional Systems and Nanostructures
      Citation Excerpt :

      Several reasons are accounted for this peak. For instance, A. Spaodoni et al. [35]report this peak as the result of electron recombination from shallow donor level of zinc interstitials to the valence band. In another report [36], the same peak is attributed to the electron recombination from the level of ionized oxygen vacancy to the valence band.

    • Promotional effects of ZnO-branching and Au-functionalization on the surface of SnO<inf>2</inf> nanowires for NO<inf>2</inf> sensing

      2019, Journal of Alloys and Compounds
      Citation Excerpt :

      In particular, for sensing applications, heterojunction b-NWs have large surface areas that can offer plenty of sites for adsorption of target gasses [9]. Also, the size and shape of sensing materials are crucial factors that can be used to tune their chemical and physical properties, which ultimately govern the sensing properties [10]. Accordingly, heterojunction b-NWs with nano-scale dimensions, special geometries, and a large number of hetero- and homojunctions are promising for sensing applications, where the response to a particular gas can be greatly improved by increasing the amount of chemiresistive junctions [11,12].

    View all citing articles on Scopus
    View full text