This journal is © The Royal Society of Chemistry and the Centre National de la Recherche Scientifique 2023 New J. Chem.
Cite this: DOI: 10.1039/d2nj05012a
ZnS–RGO nanocomposite structures: synthesis,
characterization and field emission properties
Sanjeewani R. Bansode,* Mahendra A. More and Rishi B. Sharma *
Zinc sulphide–reduced graphene oxide (ZnS–RGO) nanocomposite structures with varying sulphur con-
tent were synthesized by a simple solvothermal process. The various ZnS–RGO nanocomposite struc-
tures were characterized by XRD, SEM, TEM, Raman spectroscopy and field emission (FE) techniques.
The SEM images revealed that the size of the ZnS nanospheres was in the range of B500–2000 nm.
Field emission (FE) measurements on the various ZnS–RGO nanocomposite emitters were carried out in
an ultra-high vacuum (UHV) environment (P o 1 10
8
mbar). The highest current density of
B1490 mA cm
2
was recorded from the nanocomposite at an applied field of 6.40 V mm
1
. The
fluctuations in the field emission current were within 15%. Due to higher current density and lower
fluctuations in the emission current, the ZnS–RGO nanocomposite material could find useful applica-
tions in the development of efficient vacuum nano electronic devices and flat panel displays.
1. Introduction
In recent years, two-dimensional (2D) materials have attracted
the attention of researchers.
1,2
Layered materials like graphene,
its composites, and reduced graphene oxide (RGO) are well
established 2D materials. The atomically sharp edges, rapid
electron transport along the surface, and robust structure of 2D
materials offer unique advantages for the development of
efficient field emission devices. Towards this objective,
researchers have studied the field emission behaviour of single
layer graphene, multilayer graphene, few layer graphene and
reduced graphene oxide.
3–5
The semiconducting ZnS, being a
nontoxic, non-hazardous and eco-friendly material with the
work function of 7 eV, finds several applications in optoelec-
tronics, energy storage, UV and gas sensors, flat panel displays
and field emission devices.
6–9
Synthesis strategies for different
nanostructures of ZnS in the form of nanowire, flower-like
microspheres, hollow ZnS nanospheres and porous ZnO micro-
spheres have been reported in the literature by researchers.
10–13
Field emission studies of ZnS nanobelts, ZnS arrays and
nanotubes, ZnS branched nanotubes and ZnS hexagonal pyr-
amids have been reported in the literature.
14–17
It is well known
that graphene nanostructures tend to re-stack resulting in
reduction of their effective emitting area. This reduction in
the emitting area may cause deterioration in their field emis-
sion behaviour. To prevent the graphene layers from stacking, it
is considered appropriate to prepare suitable nanocomposite
heterostructures for achieving superior field emission proper-
ties. Nanostructured composites of graphene with CdS and ZnS,
and RGO with ZnS have been synthesised by researchers using
different methods for various technological applications.
18–21
Rathi and Kundalwal have employed a novel technique of
ultrasonic dual mixing to prepare a functionalised MWCNT/
epoxy nanocomposite system with enhanced mechanical and
fracture properties.
22
We have recently observed that ZnS nano-
spheres grow on RGO nanosheets.
23
In the present paper, we
report the detailed field emission studies of ZnS–RGO nano-
composite structures synthesized by a simple and cost effective
one-step solvothermal method with different sulphur contents.
2. Experimental
2.1 Synthesis of pristine ZnS nanostructures
Using a solvothermal route, the ZnS nanostructures were
synthesized by using ethanol as a solvent. In a typical solvother-
mal setup, 1.5 g zinc chloride (ZnCl
2
, anhydrous, powder,
Z99.99%, Sigma Aldrich) and 0.75 g thiourea (CH
4
N
2
S, ACS
reagent, Z99.0%, Sigma Aldrich) were dissolved in 40 ml of
ethanol and stirred for 15 min at room temperature. The
prepared solution was transferred into a Teflon-lined stainless-
steel autoclave of 80 ml capacity. Then, the autoclave was placed
in a furnace at 180 1C for 16 h. After completion of the reaction,
the furnace was allowed to cool naturally to room temperature.
The final product was collected from the autoclave and washed
with ethanol and deionised (DI) water. The washed product was
Centre for Advanced Studies in Materials Science and Condensed Matter Physics,
Department of Physics, Savitribai Phule Pune University, Pune-411007,
Maharashtra, India. E-mail: srbansode4@gmail.com, rbs@physics.unipune.ac.in,
rbsharma111@gmail.com
Received 12th October 2022,
Accepted 12th December 2022
DOI: 10.1039/d2nj05012a
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