Synthesis and characterization of WO 3 nanostructures preparedby an aged-hydrothermal method R.. The growth direction of the tungsten oxide nanostructures was determined along [010] axis
Trang 1Synthesis and characterization of WO 3 nanostructures prepared
by an aged-hydrothermal method
R Huirache-Acuñaa,b,⁎, F Paraguay-Delgadoc,1, M.A Albiterd, J Lara-Romerod,
aCFATA-UNAM, Boulevard Juriquilla 3001, Juriquilla Querétaro, 76230, Mexico
bUniversidad La Salle Morelia, Av Universidad 500, Mpio Tarímbaro Mich., 58880, Mexico
cCentro de Investigación en Materiales Avanzados, S.C CIMAV, Laboratorio Nacional de Nanotecnología-Chihuahua, Miguel de Cervantes
120, Complejo Industrial Chihuahua, Chih., 31109, Mexico
d
Facultad de Ingeniería Química, Universidad Michoacana de San Nicolás de Hidalgo, Morelia Mich., 58000, Mexico
A R T I C L E D A T A A B S T R A C T
Article history:
Received 7 November 2008
Received in revised form 5 March 2009
Accepted 9 March 2009
Nanostructures of tungsten trioxide (WO3) have been successfully synthesized by using an aged route at low temperature (60 °C) followed by a hydrothermal method at 200 °C for 48 h under well controlled conditions The material was studied by X-ray diffraction (XRD), scanning electron microscopy (SEM) and Energy Dispersive Spectroscopy (EDS), transmission electron microscopy (TEM) and high-resolution transmission electron microscopy (HRTEM), Raman spectroscopy and X-ray photoelectron spectroscopy (XPS) Specific Surface Area (SBET) were measured by using the BET method The lengths of the WO3
nanostructures obtained are between 30 and 200 nm and their diameters are from 20 to
70 nm The growth direction of the tungsten oxide nanostructures was determined along [010] axis with an inter-planar distance of 0.38 nm
© 2009 Elsevier Inc All rights reserved
Keywords:
Nanostructures
Tungsten trioxide (WO3)
Hydrothermal method
1 Introduction
In recent years, studies of transition metal oxides
nanos-tructures have become important due to the different
potential applications, such as nanoelectronics[1], gas sensors
[2,3], optical devices [4], electrochromic windows [5,6], and
catalysts [7,8] Nanostructures of tungsten oxide having
nanometer scale had been formed by using different
condi-tions and preparation methods: electrospinning[9], oxidation
of a substrate under appropriate conditions and the deposition
of tungsten oxide from a tungsten foil heated in the presence
of oxygen [10], by heating a tungsten filament in a partial
oxygen atmosphere[11], by reacting WO(OMe)4under
auto-genic pressure at elevated temperature followed by annealing [12], by hot filament chemical vapor deposition[13], physical vapor deposition process[14]and by ultrasonic spray and laser pyrolysis techniques[15–17] Recently, Therese et al.[18]and
Ha et al.[19]reported the synthesis of WO3nanostructures by following a hydrothermal route They used as raw materials ammonium salts and some additives to control the formation
of nanomaterials In comparison with the methods mentioned before, the hydrothermal route is an economical preparation method of nanostructures since it does not require an expensive experimental setup In this work, we report the synthesis and characterization of WO3 nanostructures pre-pared by following an easy two step aged-hydrothermal
⁎ Corresponding author CFATA-UNAM, Boulevard Juriquilla 3001, Juriquilla Querétaro, 76230, Mexico Tel.: +52 442 238 11 43; fax: +52 442 238 11 65
E-mail address:rafael_huirache@yahoo.it(R Huirache-Acuña)
1Present address: National Institute for Nanotechnology, 11421 Saskatchewan Drive Edmonton (AB) Canada T6G 2M9
1044-5803/$– see front matter © 2009 Elsevier Inc All rights reserved
doi:10.1016/j.matchar.2009.03.006
Trang 2method at low temperature by using ammonium
metatung-state as tungsten source and without the presence of
additives
2 Experimental
2.1 Synthesis of WO3Nanostructures
WO3nanostructures were synthesized by using an
aged-hydrothermal route A saturated aqueous solution of
ammo-nium metatungstate [(NH4)10W12O41xH2O] (0.15 mol of W) was
prepared and acidified with HNO32.2 N (Normal) to produce a
pH around 5 and then kept in a flask hermetically sealed with
stirring by one week at 60 °C Then, 5 ml of the aged solution
was deposited into a Teflon-lined stainless steel autoclave and
heated at 200 °C for 48 h The material obtained was filtered
and washed with deionized water and dried in the presence of
air at room temperature
2.2 Characterization
A scanning electron microscope (JEOL JSM 5800 LV) was used
to perform morphological analysis Several fields were analyzed
at different magnifications in order to get information of the
prevalent features The elemental composition was determined
using energy dispersive spectroscopy (EDS) (Oxford Inca
X-Sight) Specific surface area (SBET) determination was made with
a Quantachrome AUTOSORB-1 model by nitrogen adsorption at
−196 °C using the BET isotherm Samples were degassed under
flowing argon at 200 °C for 2 h before nitrogen adsorption TEM
and HRTEM micrographs were obtained in a Philips TECNAI F20 FEG transmission electron microscope operated at 200 kV X-ray analysis was made with a Philips X Pert MPD diffractometer, equipped with a graphite monochromator, copper Kα radiation with wavelengthλ=1.54056 Å, operated at 43 kV and 30 mA Raman spectroscopy was performed using a Labram system model Dilor micro-Raman equipped with a 20 mW He–Ne laser emitting at 632.8 nm and a holographic notch filter made by Kaiser Optical Systems, Inc (model supertNotch-Plus) with a
256 × 1024-pixel charge-coupled device (CCD) used as the detector; and a computer-controlled XY stage with a spatial resolution of 0.1 µm with two interchangeable gratings (600 and
1800 g mm− 1) and a confocal microscope with 10, 50, and 100× objectives All measurements were collected at room tempera-ture with no special sample preparation Oxidation state and surface composition were analyzed by an X-ray photoelectron spectroscope, Energy Spectrometer EA 11 MCD, using Mg monoenergetic soft X-ray (Kα=1253.6 eV)
3 Results and Discussion
The synthesis method presented in this work for procuring
WO3nanostructures is a modification of the method reported
by Albiter et al for MoO3nanorods[20]and Therese et al for
WO3 nanostructures [18] The main difference between Therese et al method and ours is that we did not use additives
to form the nanostructures On the other hand, nitric acid (HNO3) was not used before the hydrothermal treatment as reported by Albiter et al
To convert W12O41 10− anions to neutral W12O36, excess divalent oxygen anions must be removed Stoichiometrically, five divalent oxygen anions per W12O4110−must be combined with protons from the acidic medium:
W12O 10−
According to reaction (1), high concentrations of both
W12O41 −and H+would shift the reaction to the right ensuring the formation of WO , although many intermediate steps and
Fig 1– XRD pattern for WO3nanostructures Where all
reflections are indexed based on a hexagonal WO3cell
Table 1– Crystallite size (ϕ) determined by Scherer
equation (ϕ=Kλ/βCosθ), where K=0.9, λ=1.54 Å, β is
FWHM in radians andθ is the glancing angle
Fig 2– N2adsorption–desorption isotherm at −196 °C of tungsten oxide nanostructures
Trang 3thus compounds and phases may exist It is thus anticipated
that the formation of WO3should have a strong dependence
on the acid medium Furthermore, the aging time in solution
and the hydrothermal treatment time inside the autoclave
have a strong influence in the formation of nanostructures
Paraguay-Delgado et al.[21], concluded that two conditions
are important for procuring nanostructures, the first being
that for an extended-time-aged solution a short hydrothermal
treatment is required (about 24 h) and the second being that
for a short-time-aged solution (1 week) at least 36 h of
hydrothermal treatment is required
The XRD pattern from WO3nanostructures is reported in
Fig 1where a well crystallized phase was observed The
half-widths reflection indicates the presence of nanoscale
tung-sten oxide which was corroborated measuring the crystallite
size (ϕ) for more intense and representative reflections (100),
(001) and (200) (Table 1) by using the Scherer equation:
The observed peaks could be indexed based in a
hex-agonal cell with inter-planar spacings for tungsten trioxide
(ICSD 32,001, JCPDS 33-1387; a = 7.298 Å, c = 3.899 Å, space group P6/mm)[18,19] It was also observed that there are not other impurity phase peaks
As observed,Fig 2shows the N2adsorption–desorption curve corresponding to a type IV isotherm (IUPAC Classifi-cation) with desorption step characteristic of mesoporous materials above the relative pressure (P/Po) of 0.4 and specific surface area (SBET) values between 34 and 35 m2
(Table 2) The formation of a mesoporous material is due to the water vapor pressure inside the autoclave at 200 °C, at this time the exactly mechanism of formation is not right known[22]
Fig 3a–c shows SEM micrographs at different magnifica-tions from separable WO3nanostructures with different size protruding out The oxide nanostructures had smooth sur-faces and a not well-defined rectangular cross section These particles were about 0.1 to 3 µm long, and 50–200 nm wide as determined from SEM images As illustrated inFig 3a–c this method led to the formation of nanostructures in a wide range
of thicknesses, most of which had shown an irregular shape The oxygen (O) and tungsten (W) atomic contents were determined by Energy Dispersive Spectroscopy (EDS) analysis (1% error) and the results are reported in Table 2 The EDS spectrum presented in Fig 3d reveals a 3:1 atomic ratio for oxygen and tungsten elements, which solely constitute the composition of WO3
Transmission electron microscopy (TEM) micrographs of
WO3nanostructures are reported (Fig 4a–b) A representative TEM image of the tungsten oxide nanostructures is given in
Table 2– Elemental analysis determined by EDS (% atomic)
and specific surface area (SBET)
Sample % at O % at W SBET(m2/g)
Fig 3– Scanning electron microscopy images of WO3nanostructures at different magnifications: (a) 5000×, b) 14,000× and c) 15,000× (d) EDS spectrum
Trang 4Fig 4a This sample consists of very well separated particles
with irregular shape and lengths between 30 and 200 nm and
wide from 20 to 70 nm, aggregated together due to the high
surface energy owing to their nanosize.Fig 4b shows a TEM
micrograph at a higher magnification By using HRTEM we
observed that the growth direction of the tungsten oxide
nanostructures is along [010] axis with an inter-planar
distance of 0.38 nm (Fig 4b) It seems that the WO3growth
proceeds layer by layer increasing the thickness and the width
of the nanostructures
Raman spectroscopy was used to characterize this
material since this technique is suitable to obtain details
of the WO3chemical structure (Fig 5) Three broad bands
were clearly detected: high in the 900–1000 cm− 1 region,
medium in the 600–800 cm− 1region and low in the 200–
400 cm− 1 region The most intense peak is centered at
780 cm− 1with a shoulder at 730 cm− 1and they are attributed
to the symmetric and asymmetric vibrations of W6+–O
bonds (O–W–O stretching modes) Two peaks centered at
320 and 270 cm− 1can be found in the 200–400 range and correspond to W–O–W bending modes of the bridging oxygen [23–25] A peak at 910 cm− 1 with a shoulder positioned at 960 cm− 1 in the 900–1000 cm− 1 can be observed These peaks correspond to the WfO stretching mode of terminal oxygen atoms that are present on the surface of the cluster (dangling bonds) or at the boundaries
of nanometre grains[15,26] The small feature observed at
435 cm− 1is attributed to the characteristic band of crystal-line WO3[27] Note that these results confirm the formation
of hexagonal WO3since the main features corresponding to monoclinic WO3typically reported at 807 and 715 cm− 1are absent in the Raman spectrum[28–30]
The XPS collected spectra of the material for the peaks O1 s
and W4fare shown inFig 6a and b respectively Peaks position for O1 sis 530.3 eV and binding energy peak located at 35.4 and 40.6 eV is attributed to W4 f According to the literature[31]it is
WO3, this means that the surface of the material contains W6+
and not other oxidation state for this metal was detected This was also verified by calculating the O/W ratio using their relative peak areas (I) and atomic sensitivity factors (S), which
is shown below (Eq (3)):
Atomic Ratio O
W =
I 0
S 0
I W
S W
=
47483:97 0:66 63692:91 2:75
4 Conclusions
WO3nanostructures with hexagonal phase and mesopor-osity were obtained by using a two step aged-hydrothermal method By using HRTEM we observed that the growth direction of the tungsten oxide nanostructures is along [010]
Fig 4– Transmission electron microscopy (TEM) micrographs
of WO nanostructures
Fig 5– Typical Raman spectrum of hexagonal WO3
nanostructures obtained by the aged-hydrothermal method
Trang 5axis with an inter-planar distance of 0.38 nm Raman, EDS and
XPS analysis confirmed that the chemical structure and
oxidation states belong to tungsten oxide (WO3)
Acknowledgements
The authors appreciate the valuable technical assistance
of M.C W Antúnez, M.I.Q Alicia del Real, M.C E Torres, Ing
C Ornelas, Dr A Medina, Dr Ismeli Alfonso and M.C F
Rodríguez Melgarejo This work was financially supported by
CIMAV, S.C., Universidad La Salle Morelia and Postdoctoral
fellowship-UNAM
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