INSTITUTE OF PHYSICS PUBLISHING SEMICONDUCTOR SCIENCE AND TECHNOLOGY
Semicond. Sci. Technol. 19 (2004) 1057–1060 PII: S0268-1242(04)77399-X
Synthesis and characterization of tin
oxide microfibres electrospun from a
simple precursor solution
Yu Wang
1,3
, Milca Aponte
1
, Neliza Leon
1
, Idalia Ramos
1
,
Rogerio Furlan
1
, Stephane Evoy
2
and Jorge J Santiago-Avil´ es
2
1
Department of Physics & Electronics, University of Puerto Rico at Humacao,
CUH Station, Humacao 00791, Puerto Rico
2
Department of Electrical & Systems Engineering, University of Pennsylvania,
200 South 33rd Street, Philadelphia, PA 19104, USA
Received 8 March 2004, in final form 13 May 2004
Published 7 July 2004
Online at stacks.iop.org/SST/19/1057
doi:10.1088/0268-1242/19/8/017
Abstract
Tin oxide (SnO
2
) microfibres in the rutile structure were synthesized using
electrospinning and metallorganic decomposition techniques. Fibres were
electrospun from a precursor solution containing 20 mg poly(ethylene
oxide) (molecular weight 900 000), 2 ml chloroform and 1 ml
dimethyldineodecanoate tin, and sintered in the air for 2 h at 400, 600 and
800
◦
C, respectively. Scanning electron microscopy, x-ray diffraction and
Raman microspectrometry were used to characterize the sintered fibres. The
results showed that the synthesized fibres are composed of SnO
2
.
(Some figures in this article are in colour only in the electronic version)
1. Introduction
Tin oxide, SnO
2
, is a functional material with multiple
interesting properties and important applications. As a
semiconductor with a large bandgap (E
g
= 3.6 eV), it is
transparent in the visible region of the spectrum, and has been
used as conductive electrodes and anti-reflective coatings in
solar cells and light emitting diodes (LEDs) [1–3]. Usually
SnO
2
can be doped only as n-type. Cukrov et al [4] recently
reported a weak p-type response in 5 mol%Fe
2
O
3
-doped
SnO
2
. This promises a p-type SnO
2
semiconductor and
wider applications such as the blue LED. More interestingly,
the conductivity of SnO
2
semiconductor is modulated by
the physisorbed oxygen molecules on its surface. The
absorbed oxygen, receiving electrons from the conduction
band, produces an electron depletion layer under the absorbing
surface, and a potential barrier between particles, and thus
decreases the conductivity of the SnO
2
[4–6]. This makes
SnO
2
a good candidate for a gas sensor, whose conductivity
will increase sharply when exposed to a reducing gas [4, 5].
3
Present address: Department of Electrical and Computer Engineering,
University of California, Davis, CA 95616, USA.
Due to its high surface-to-volume ratio, SnO
2
film based gas
sensors have been used widely to detect trace amount of gases
such as carbon monoxide and ethanol. With a higher surface-
to-volume ratio than thin films, fibres are expected to be more
sensitive in these applications. This can be instrumental in the
miniaturization of devices. In fact, one dimensional (1D)
or quasi-1D structures have the lowest dimensionality for
effective electron transport and photon excitations, and can
be used as basic building blocks in the bottom-up assembly in
diverse applications in electronics and photonics.
However, while SnO
2
films have been synthesized using
various methods, such as evaporation [7], reactive sputtering
[8], spray pyrolysis [9], chemical vapour deposition (CVD)
[1, 10] and sol-gel process [5, 11], only a few ways have been
found to synthesize SnO
2
fibres. Liu et al [2] synthesized SnO
2
nanowires using laser ablation. Xu et al [6] prepared SnO
2
nanorods by thermal decomposition of SnC
2
O
4
precursor.
Kolmakov et al [12] obtained SnO
2
nanowires by oxidizing
electrodeposited metallic tin nanowires using a self-organized,
highly ordered porous anodic alumina (PAO) template. Li et al
[3] prepared Sb-doped SnO
2
nanofibres by electrospinning a
solution containing poly(vinyl pyrrolidone) (binder), tin and
antimony (III) alkoxides, acetic acid and organic solvents.
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