The application of ultrasound radiation to the synthesis of nanocrystallinemetal oxide in a non-aqueous solvent Department of Chemistry, Kanbar Laboratory for Nanomaterials, Nanotechnolo
Trang 1The application of ultrasound radiation to the synthesis of nanocrystalline
metal oxide in a non-aqueous solvent
Department of Chemistry, Kanbar Laboratory for Nanomaterials, Nanotechnology Research Center, Institute of Nanotechnology and Advanced Materials, Bar-Ilan University, Ramat-Gan 52900, Israel
a r t i c l e i n f o
Article history:
Received 17 March 2009
Received in revised form 14 May 2009
Accepted 15 May 2009
Available online 22 May 2009
Keywords:
Sonochemistry
Nanoparticles
Non-aqueous solvent
Microwave
a b s t r a c t
Highly crystalline metal oxide nanoparticles of TiO2, WO3, and V2O5were synthesized in just a few min-utes by reacting transition metal chloride with benzyl alcohol using ultrasonic irradiation under argon atmosphere in a non-aqueous solvent The sonochemical process was conducted at a relatively low tem-perature, 363 K A unique crystallization process of these nanoparticles has been observed and character-ized by powder X-ray diffraction (PXRD), high resolution scanning electron microscopy (HRSEM), and BET The particles’ size and shape measured from HRSEM reveal ‘‘quasi” zero-dimensional, spherical TiO2particles in the range of 3–7 nm The V2O5particles have a ‘‘quasi” one-dimensional ellipsoidal mor-phology, with lengths in the range of 150–200 nm and widths varying between 40 and 60 nm The WO3
particles were obtained as ‘‘quasi” two-dimensional platelets with square shapes having facets ranging from 30 to 50 nm The thickness of these platelets was between 2 and 7 nm The mechanism of the reac-tions leading to these three metal oxide nanoparticles in a non-aqueous system is substantiated by Nuclear Magnetic Resonance (NMR), and Electron Spin Resonance (ESR)
Ó 2009 Elsevier B.V All rights reserved
1 Introduction
Among the different synthesis approaches developed during the
last few years, non-aqueous or non-hydrolytic processes were
par-ticularly successful with respect to achieving control of crystallite
size, shape, and hence over dimensionality The synthesis of metal
oxide nanoparticles in an organic solvent without the addition of
water avoided the major problems of aqueous sol–gel methods,
which are based on the hydrolysis of halide precursors, fast
reac-tions, and amorphous products Therefore, non-aqueous solution
routes to create metal oxide are valuable alternatives to the known
aqueous sol–gel process The pioneering work of Niederberger
et al has shown that benzyl alcohol as a solvent enabled the
syn-thesis of a long list of nanosized compounds, especially metal
oxi-des [1–5] Niederberger carried out the reactions under
solvothermal conditions The titanium was heated to 40 °C
be-tween 7 and 14 days For the vanadium and tungsten oxide, the
aging time was 48 h at 100 °C and 120 °C, respectively More
re-cently, he demonstrated that using benzyl alcohol as a solvent
for a solvothermal reaction can be conducted under microwave
radiation, thus saving energy and time[6] In the microwave
reac-tion other metal oxides were prepared, but not titanium, vanadium
or tungsten oxides
The growing number of publications dealing with ultrasonic irradiation gives an idea about the great potential of the method because of its simplicity and efficiency The sonochemical synthesis of metal oxide nanoparticles, as well as many other nanoparticles, has been reported and reviewed It was natural that the non-aqueous process would be extended and performed by using ultrasonic waves The application of sonochemistry allows good yields, high crystallinity of the products, and is more efficient and homogeneous Sonochemistry affords an immense reduction
of the reaction time, from days to minutes
Herein we present a novel, simple sonochemical one-step pro-cess using metal chloride precursors (TiCl4, WCl6, and VOCl3), and obtaining the corresponding nanosized metal oxides (TiO2, WO3, and V2O5) as products In all three reactions, benzyl alcohol
is simultaneously used as a solvent and a ligand, and as mentioned above, the reaction is completed within a few minutes All the spe-cific nanostructured metal oxides have been intensively studied as
a result of their outstanding chemical and physical properties For example, titanium oxides are of interest for applications as gas sen-sors[7–11], catalysts[12], photo catalysts[13–16], and photovol-taic cells[17–22] Vanadium oxides are applied in catalysis[23] and electrochemistry[24], and tungsten oxides have been investi-gated for electrochromic device technology[25]
The synthesis of the metal oxide nanoparticles involved disper-sion of the precursors in benzyl alcohol (Scheme 1), followed by heating them in a sonicator of 60% amplitude, with the collapse
of acoustic the bubble resulting in the shorter reaction time
1350-4177/$ - see front matter Ó 2009 Elsevier B.V All rights reserved.
* Corresponding author.
E-mail address: gedanken@mail.biu.ac.il (A Gedanken).
Contents lists available atScienceDirect
Ultrasonics Sonochemistry
j o u r n a l h o m e p a g e : w w w e l s e v i e r c o m / l o c a t e / u l t s o n c h
Trang 22 Experimental section
2.1 Materials
Titanium (IV) chloride (99.9%), Vanadium (V) oxychloride
(99.99%), tungsten (VI) chloride (powder 99.9%) and benzyl alcohol
(99.8%, anhydrous) were obtained from Aldrich These chemicals
were used without further purification
2.2 Synthesis of the metal oxide nanoparticles
In a typical preparation, the transition metal chloride, 0.5 mL of
TiCl4(4.5 mmol), 400 mg of WCl6(1 mmol), and 0.5 mL of VOCl3
(5.3 mmol), was slowly added to 20 mL of benzyl alcohol
(0.193 mol) under vigorous stirring at room temperature All the
materials were introduced into the sonication cell under inert
atmosphere in a glove box The reaction mixture was sonicated
un-der argon–hydrogen atmosphere (60% amplitude) The reaction
time differed depending on the precursor For the vanadium and
the titania, the sonication time was 10 min The tungsten precursor
required between 5 and 7 min to fully react The sonication was
conducted without cooling so that a temperature of 363 K was
reached at the end of the reaction The resulting suspensions were
centrifuged and the precipitate was thoroughly washed three
times with ethanol (1 20 mL) and THF (2 20 mL) The collected
material was left to dry in air and finally ground into a powder
After grinding, the powders were weighed and good yields (85–
95%) were obtained for all three reactions Care should be taken
as the reaction is rather violent
3 Analysis and characterization
The XRD crystallinity and particle size were investigated by
X-ray diffraction (XRD) XRD measurements carried out using a
Mod-el-2028 (Rigaku) diffractometer Transmission electron microscopy
(TEM) samples were prepared by depositing one drop of the
solu-tion on a 400 mesh copper grid coated with carbon and dried
over-night under vacuum The transmission electron micrographs were
obtained with a JEOL JEM-1200EX electron microscope A Scion
Im-age software program was used to measure the mean particle size
of the nanoparticles from the HRSEM High resolution scanning electron microscopy (HR-SEM) micrographs were obtained using
a JEOL-JSM 700F instrument and a LEO Gemini 982 field emission gun SEM (FEG-SEM) The BET surface area measurements were characterized by nitrogen adsorption at 77 K The domestic micro-wave oven (DMO) operates at 2.45 GHz, under argon atmosphere with a power of 900 W output A white product was obtained for the titanium reaction The tungsten product was yellow The color
of the as-prepared vanadium material was black After heating to
450 °C, the color of the powder turned to orange
4 Results and discussion
In contrast to most of the sol–gel processes that lead to amor-phous materials, our synthesized products are highly crystalline Powder X-ray diffraction (PXRD) patterns of the obtained materials are shown inFig 1 The white titania sample consists of a pure ana-tase phase without any indication of other crystalline products (Fig 1a) The broad diffraction peaks obtained for the titania and the WO3indicate clearly the nanosized nature of the as-prepared products The XRD powder patterns of the TiO2, V2O5, and WO3 show diffraction peaks that match well with the PDF tables (01-086-1157), (03-065-013), and (00-041-0905), respectively The pattern of the yellow particles fits the WO3 data (Fig 1b) The XRD diffraction pattern of the as-prepared black vanadium oxide powder can not be assigned to a specific vanadium oxide phase
We interpret the as-prepared product as being composed of a mix-ture of vanadium oxides EDX measurements of the as-prepared product indicate the presence of only vanadium, oxygen, and car-bon Heating the vanadium mixture to 450 °C has led to the forma-tion of a single-phase crystalline V2O5 (Fig 1c) The average crystallite size estimated using the Scherrer equation is about 10–15 nm for the titania The vanadium and tungsten oxide sizes were about 45–64 nm, and 13–20 nm, respectively (Table 1) It is worth noting that in a recent paper by Niederberger et al.[35], the reaction between VOCl3 and benzyl alcohol has led to the formation of VO1.52(OH)0.77 The reaction was conducted under conventional heating for 24 h at 150 °C That means that conven-tional heating produces different product from our V2O5
Representative high resolution scanning electron microscopy (HRSEM) images are presented inFig 2and were used to calculate the size distribution of the products A highly aggregated morphol-ogy is illustrated inFig 2a, which depicts the titania product The aggregate consists of ‘‘quasi” zero-dimensional particles having a diameter ranging from 3 to 7 nm (Fig 2a) After annealing the vanadium, the oxide sample exhibits rather uniform ellipsoidal particle morphology, ‘‘quasi” one-dimensional, with lengths
rang-Scheme 1 General reaction scheme displaying the metal oxide precursors used the
solvent, the experimental condition and the resulting metal oxide nanoparticles.
2θ (degree)
(a)
(b)
(c)
Trang 3ing from 150 to 200 nm and diameters varying between 40 and
60 nm (Fig 2b) The length for the mixed valent vanadium oxide,
the as-prepared material, is between 150 and 250 nm, and the
diameter varies between 30 and 60 nm This means that upon
the annealing process, the product does not undergo any
morpho-logical changes
The tungsten oxide forms nearly square, ‘‘quasi”
two-dimen-sional platelets These nanoparticles have facets ranging from 30
to 50 nm (Fig 2c) Side views of particles that are oriented
verti-cally to the SEM grid reveal that the thickness is between 2 and
7 nm These HRSEM images prove that all the three nanomaterials
have a high crystallinity and their size is in good agreement with
the size calculated from the powder XRD patterns recorded for
the same sample
In our case, the BET surface area of the nanoparticles
synthe-sized by microwaves is higher than that synthesynthe-sized by an
ultra-sonic route, apart from titania The BET surface area of TiO2,
V2O5, and WO3, which were prepared in ultrasonic irradiation,
are 162.6, and 47 m2/g, while that of microwave are 124, 12, and
77 m2/g, respectively
Like the surface area, the particle size also depends on the
reac-tion device/method Although particle-size determinareac-tion by peak
broadening is not a very accurate method, the results coincide well
with HRSEM measurements (Table 1) As expected, the decrease in
particle size is expressed in larger surface areas We have also
syn-thesized the same products in a domestic microwave oven The
precursors and the solvents were identical to those in the
sono-chemistry reaction The microwave and sonochemical results of
the BET surface area and the crystallite size of all the materials,
as obtained from HRSEM and from XRD by the Scherrer equation,
are presented inTable 1
4.1 Reaction mechanisms of metal oxide particles in non-aqueous
synthesis
This section will discuss the organic side of the synthesis of
inorganic nanomaterials performed in non-aqueous, but liquid
reaction media The organic components and the organic reaction
pathways play a fundamental role in the non-aqueous synthesis
of the inorganic products In this process, the formal oxygen that
is required for the fabrication of the metal oxide is not provided
by any added water Therefore, it must stem from the precursor
of the organic media In our case, the benzyl alcohol is used as
the oxygen source It is clear that in our process the organic solvent
serves as a solvent as well as a reactant, thus playing a major role
in the formation of the product Generally, two possible organic
mechanisms are suggested for providing the oxygen to enable
the formation of the metal oxide nanostructure The first is the
al-kyl/halide elimination mechanism[26,27] Metal halides are
popu-lar precursors due to their good commercial availability and their
comparatively low cost In alcohol solvents, the alcohol oxygen is
rapidly coordinated to the metal centre, which is followed by an
elimination reaction Basically, two elimination mechanisms can occur: a reaction that directly promotes the formation of the metal oxide by an alkyl halide elimination (Scheme 2, Eq 1), which may
be adequately termed as a hydroxylation process[28] In this case,
a metal-coordinated hydroxyl group is formed that instantly reacts with the precursor to form metal–oxygen–metal groups (Scheme
2, Eq 2) The combination of these two equations leads to the elim-ination of R–X and H–X The other possibility is the elimelim-ination of only hydrogen halide This mechanism constitutes a ligand ex-change reaction[29](Scheme 3, Eq 3)
The second possible mechanism is related to radicals involved
in the reaction as a result of the bubble’s collapse Application of ultrasound to chemical processes involves the use of acoustic cav-itation Acoustic cavitation involves the nucleation, growth, and sudden collapse of the gas of vapor-filled microbubbles formed from acoustical wave-induced compression/rarefaction in a body
of liquid[30] The implosion of the microscopic bubbles in the li-quid generates energy, which induces chemical and mechanical ef-fects It is well known that the sudden collapse leads to localization, a transient high temperature (P5000 K) and pressures (P1000 atm), resulting in an oxidative environment due to the generation of highly reactive species, including hydroxyl radical (
OH)[31,32] This mechanism governs mostly sonochemical reac-tions conducted in aqueous solureac-tions We have examined whether
OH radicals are formed when a bubble collapses in a benzyl alcohol solution The following experimental technique was employed in this probe
ESR: to 20 ml of benzyl alcohol a small amount of a TEMPO trap was added and the sonication took place under identical conditions
to those of the synthesis of the metal oxides It is assumed that if hydroxyl radicals are formed they will be trapped by the TEMPO molecules, and their presence can be detected by electron spin res-onance measurements
Since the possibility of the involvement of hydroxyl radicals is eliminated, we are back to the proposed mechanism of Schemes
2 and 3 To substantiate these mechanisms further experimenta-tion and calculaexperimenta-tion were performed They are outlined below 1
H NMR: the information about the reaction pathway can be found by identifying the organic products, which are present in the final reaction mixture The1H NMR spectra of the pure benzyl alcohol and of the final reaction mixture are presented inFig 3a and b, respectively According toFig 3a of the benzyl alcohol, there are three main peaks The multiplet peaks at 7.25 ppm resulted from the benzene ring proton in the benzyl alcohol structure Addi-tionally, the strong singlet peak at 4.5 ppm refers to the methyl group, whereas the weak singlet peak at 3.3 ppm refers to the
OH group The integration ratios of the benzene ring, the methyl group and the OH peak are 1:0.4:0.2, respectively
The triplet peak at 1.1 ppm and the quartet peak at 3.5 ppm are assigned to the CH3 and CH2 groups of ethanol, respectively According to these benzyl alcohol spectra and the literature values, the1H NMR results show that in a pure TiCl4/benzyl alcohol system,
Table 1
Overview of the surface area and particle sizes calculated from HRSEM and XRD data with a reaction yield.
HRSEM particle size (nm) BET surface area (m 2
/g) Reaction yield (%)
Microwave 45–55 b
Microwave 10–15 b
a
The average crystallite size was calculated using the Scherrer equation.
b
These results are assigned to the average size of the thickness.
Trang 4the final reaction solution contained benzyl chloride The results/
spectra of the final reaction solution are presented inFig 3b As
op-posed to benzyl alcohol spectra, in the final reaction the spectra
ex-hibit only two peaks The multiplet peaks at 7.33 ppm resulted from the benzene ring proton in the benzyl chloride structure, and the strong singlet peak at 4.66 ppm refers to the methyl chloride group
Scheme 2.
Scheme 3.
Fig 2 HR-SEM micrographs of: (a) crystalline anatase TiO 2 ; mean particle size is 7 ± 1.0 nm, (b) vanadium mixture after heating (single-phase V 2 O 5 ), mean lengths size is
175 ± 20 nm, and mean diameters is 50 ± 10, (c) WO 3 , mean particle size is 41.2 ± 5.9 nm and mean thickness is 6.3 ± 1.5.
Trang 5This NMR result demonstrates that in this reaction system benzyl
chloride was present as a reaction product
It is well known that sonochemistry is carried out at a much
higher temperature than that of the solution temperature The
endothermic reaction will strongly benefit from this high
temper-ature[33] It was therefore necessary to observe whether the
cur-rent anionic solvothermal reaction is endothermic, and thus
thermodynamic calculations were carried out
DH0
f: the enthalpy of the formation of the synthesis of titanium
oxide from benzyl alcohol and titanium tetra chloride at 298 K was
calculated by using the literature values ofDH0f of the reactants and
the products[34] The enthalpy energy values of TiCl4, benzyl
alco-hol, TiO2, HCl, and benzyl chloride are (804.16), (154.9),
(938.72), (92.3), and (32.6) kJ mol1, respectively
The balanced equation of synthesis titania is the following
reaction:
TiCl4þ 2C6H5CH2—OH ! TiO2þ 2C6H5CH2—Cl þ 2HCl
The calculated value wasDH0f :r= 74 kJ mol1 This value
sur-prised us because it indicates that at 298 K and at 1 atmosphere
of the components, the reaction is exothermic We have also
exam-ined whether the tendency ofDH0f :ris to become more negative or
positive at higher temperatures Our conclusion is (not all the
ther-modynamic values are available) that theDH0
f :rwill become posi-tive at higher temperatures We therefore conclude that the
sonochemistry indeed pushes the reaction towards the products
It is needless to point out that at these high temperatures the
kinetics is indeed much faster Finally, the reaction mechanism of metal oxide particles in non-aqueous systems is proceeding via al-kyl/halide elimination, which is proposed inSchemes 2 and 3, and contains benzyl chloride as a product
5 Conclusion
In summary, transition metal oxide nanoparticles have been successfully prepared using benzyl alcohol–metal chlorides as precursors by a one-step sonochemical method that leads to low-dimensional particle shapes, such as nearly spherical titania nanoparticles, vanadium oxide nanorods, and tungsten oxide nanoplatelets On the one hand, the application of ultrasonic irra-diation offers a fast synthesis route with a low temperature to a variety of metal oxides with high crystallinity, while on the other hand it proposes a non-aqueous, simple method which enables many reaction parameters that are difficult to control in aqueous systems In comparison, in previous reports without ultrasound, the non-aqueous synthesis methods of metal oxide need high tem-peratures or long-time treatments The fact that nanoparticle for-mation is based on the same mechanism in the previous reported and in our report, which done with ultrasound or with the microwave, are strongly supports the proposition that ultra-sound/microwave irradiation has a great potential to control the growth of inorganic nanoparticles through influencing the organic reaction pathway
Scale: 0.4094 ppm/cm, 81.92 Hz/cm
1.2 1.4 1.6 1.8 2.0 2.2 2.4 2.6 2.8 3.0 3.2 3.4
Scale: 0.1514 ppm/cm, 30.29 Hz/cm
a
b
Fig 3 (a) 1
H NMR spectra of pure benzyl alcohol (b) 1
H NMR spectra of the final reaction solution (benzyl chloride).
Trang 6[1] M Niederberger, M.H Bartl, G.D Stucky, Benzyl alcohol and transition metal
chlorides as a versatile reaction system for the nonaqueous and
low-temperature synthesis of crystalline nano-objects with controlled
dimensionality, J Am Chem Soc 124 (2002) 13642–13643.
[2] M Niederberger, M.H Bartl, G.D Stucky, Benzyl alcohol and titanium
tetrachloride – a versatile reaction system for the non-aqueous and
low-temperature preparation of crystalline and luminescent titania nanoparticles,
J Chem Mater 14 (2002) 4364–4370.
[3] N Pinna, S Grancharov, P Beato, P Bonville, M Antonietti, M Niederberger,
Magnetite nanocrystals: nonaqueous synthesis, characterization, and
solubility, J Chem Mater 17 (2005) 3044–3049.
[4] M Niederberger, G Garnweitner, N Pinna, M Antonietti, Nonaqueous and
halide-free route to crystalline BaTiO 3 , SrTiO 3 , and (Ba, Sr)TiO 3 nanoparticles
via a mechanism involving C–C bond formation, J Am Chem Soc 126 (2004)
9120–9126.
[5] M Niederberger, N Pinna, J Polleux, M Antonietti, A general soft-chemistry
route to perovskites and related materials: synthesis of BaTiO 3 , BaZrO 3 , and
LiNbO 3 nanoparticles, Chem Commun 43 (2004) 2270–2273.
[6] I Bilecka, I Djerdj, M Niederberger, One-minute synthesis of crystalline
binary and ternary metal oxide nanoparticles, Chem Commun (2008) 886–
888.
[7] M Ferroni, M.C Carotta, V Guidi, G Martinelli, F Ronconi, M Sacerdoti, E.
Traversa, Preparation and characterization of nanosized titania sensing film,
Sens Actuators B: Chem 77 (2001) 163–166.
[8] N Kumazawa, M.R Islam, M Takeuchi, Photoresponse of a titanium dioxide
chemical sensor, J Electroanal Chem 472 (1999) 137–141.
[9] C Garzella, E Comini, E Tempesti, C Frigeri, G Sberveglieri, TiO 2 thin films by
a novel sol–gel processing for gas sensor applications, Sens Actuators B: Chem.
68 (2000) 189–196.
[10] H.M Lin, C.H Keng, C.Y Tung, Gas-sensing properties of nanocrystalline TiO 2 ,
Nanostruct Mater 9 (1997) 747–750.
[11] D Morris, R.G Egdell, Application of V-doped TiO 2 as a sensor for detection of
SO 2 , J Mater Chem 11 (2001) 3207–3210.
[12] W.J Stark, K Wegner, S.E Pratsinis, A Baiker, Flame aerosol synthesis of
vanadia–titania nanoparticles: structural and catalytic properties in the
selective catalytic reduction of NO by NH 3 , J Catal 197 (2001) 182–191.
[13] J.C Yu, J Yu, W Ho, L Zhang, Preparation of highly photocatalytic active
nano-sized TiO 2 particles via ultrasonic irradiation, Chem Commun (2001)
1942–1943.
[14] Z.B Zhang, C.C Wang, R Zakaria, J.Y Ying, Role of particle size in
nanocrystalline TiO 2 -based photocatalysts, J Phys Chem B 102 (1998)
10871–10878.
[15] W Choi, A Termin, M.R Hoffmann, The role of metal ion dopants in
quantum-sized TiO 2 : correlation between photoreactivity and charge carrier
recombination dynamics, J Phys Chem 98 (1994) 13669–13679.
[16] M Anpo, T Shima, S Kodama, Y Kubokawa, Photocatalytic hydrogenation of propyne with water on small-particle titania: size quantization effects and reaction intermediates, J Phys Chem 91 (1987) 4305–4310.
[17] B O’Regan, M Gratzel, A low-cost, high-efficiency solar cell based on dye-sensitized colloidal TiO 2 films, Nature 353 (1991) 737–740.
[18] M Gratzel, Sol–gel processed TiO 2 films for photovoltaic applications, J Sol– Gel Sci Technol 22 (2001) 7–13.
[19] U Bach, D Lupo, P Comte, J.E Moser, F Weissortel, J Salbeck, H Spreitzer, M Gratzel, Solid-state dye-sensitized mesoporous TiO 2 solar cells with high photon-to-electron conversion efficiencies, Nature 395 (1998) 583–585 [20] A Hagfeldt, M Gratzel, Molecular photovoltaics, Acc Chem Res 33 (2000) 269–277.
[21] N.G Park, J van de Lagemaat, A.J Frank, Comparison of dye-sensitized rutile-and anatase-based TiO 2 solar cells, J Phys Chem B 104 (2000) 8989–8994 [22] M Thelakkat, C Schmitz, H.W Schmidt, Fully vapor-deposited thin-layer titanium dioxide solar cells, Adv Mater 14 (2002) 577–581.
[23] D Gasser, A Baiker, Methanol oxidation on vanadium oxide catalyst prepared
by in situ activation of amorphous vanadium pentoxide precursor, J Catal 113 (1988) 325–333.
[24] J.X Dai, S.F.Y Li, Z.Q Gao, K.S Siow, Novel method for synthesis ofc-lithium vanadium oxide as cathode materials in lithium ion batteries, Chem Mater 11 (1999) 3086–3090.
[25] C.G Granqvist, Electrochromic tungsten oxide films: review of progress 1993–
1998, Sol Energy Mater Sol Cells 60 (2000) 201–262.
[26] G Garnweitner, M Niederberger, Organic chemistry in inorganic nanomaterials synthesis, J Mater Chem 18 (2008) 1171–1182.
[27] G Garnweitner, M Niederberger, Organic reaction pathways in the nonaqueous synthesis of metal oxide nanoparticles, Chem Eur J 12 (2006) 7282–7302 [28] R.J.P Corriu, D Leclercq, P Lefevre, P.H Mutin, A Vioux, Preparation of monolithic gels from silicon halides by a non-hydrolytic sol–gel process, J Non-Cryst Solids 146 (1992) 301–303.
[29] A Vioux, Nonhydrolytic sol–gel routes to oxides, Chem Mater 9 (1997) 2292– 2299.
[30] Y.G Adewuyi, Sonochemistry: environmental science and engineering applications, Ind Eng Chem Res 40 (2001) 4681–4715.
[31] K.S Suslick, Sonochemistry, Science 247 (1990) 1439–1445.
[32] E.B Flint, K.S Suslick, The temperature of cavitation, Science 253 (1991) 1397– 1399.
[33] S Avivi, Y Mastai, G Hodes, A Gedanken, Sonochemical hydrolysis of Ga 3+ ions: synthesis of scroll-like cylindrical nanoparticles of gallium oxide hydroxide, J Am Chem Soc 121 (1999) 4196–4199.
[34] S.P Verevkin, E.L Krasnykhz, J.S Wright, Thermodynamic properties of benzyl halides: enthalpies of formation, strain enthalpies, and carbon–halogen bond dissociation enthalpies, Phys Chem Chem Phys 5 (2003) 2605–2611 [35] I Djerdj, D Sheptyakov, F Gozzo, D Arcon, R Nesper, M Niederberger, Oxygen self-doping in hollandite-type vanadium oxyhydroxide nanorods, J Am Chem Soc 130 (2008) 11364–11375.