ContentslistsavailableatSciVerseScienceDirect
Electrochimica
Acta
j o ur na l h o me p ag e :w w w . e l s e v i e r . c o m / l o c a t e / e l e c t a c t a
Electrochromic
properties
of
nanostructured
tungsten
trioxide
(hydrate)
films
and
their
applications
in
a
complementary
electrochromic
device
Zhihui
Jiao
a,
Jinmin
Wang
a,
Lin
Ke
b,
Xuewei
Liu
c,
Hilmi
Volkan
Demir
a,d,e,
Ming
Fei
Yang
a,
Xiao
Wei
Sun
a,f,∗aSchoolofElectricalandElectronicEngineering,NanyangTechnologicalUniversity,NanyangAvenue,Singapore639798,Singapore
bInstituteofMaterialResearchandEngineering,A*STAR(AgencyforScience,TechnologyandResearch),ResearchLink,Singapore117602,Singapore cSchoolofPhysicalandMathematicalSciences,NanyangTechnologicalUniversity,NanyangAvenue,Singapore637371,Singapore
dDepartmentofElectricalandElectronicsEngineering,DepartmentofPhysics,UNAM–InstituteofMaterialsScienceandNanotechnology,BilkentUniversity,Bilkent,Ankara06800, Turkey
eSchoolofPhysicalandMathematicalSciences,NanyangTechnologicalUniversity,NanyangAvenue,Singapore639798,Singapore
fDepartmentofAppliedPhysics,CollegeofScience,andTianjinKeyLaboratoryofLow-DimensionalFunctionalMaterialPhysicsandFabricationTechnology,TianjinUniversity, Tianjin300072,China
a
r
t
i
c
l
e
i
n
f
o
Articlehistory: Received31August2011 Receivedinrevisedform 16December2011 Accepted18December2011 Available online 26 December 2011 Keywords: Electrochromism Tungstentrioxide Thinfilm Complementarydevice
a
b
s
t
r
a
c
t
Orthorhombichydratedtungstentrioxide(3WO3·H2O)filmsconsistedofnanosticksand
nanoparti-cleswerepreparedonfluorinedopedtinoxide(FTO)-coatedsubstratebyafacileandtemplate-free hydrothermalmethodusingammoniumacetate(CH3COONH4)asthecappingagent.Irregularnanobrick
filmswereobtainedwithoutcappingagent.Duetothehighlyroughsurface,thenanostick/nanoparticle film depicts faster ion intercalation/deintercalation kinetics and a greater coloration efficiency (45.5cm2/C)thanthenanobrickfilm.Acomplementaryelectrochromicdevicebasedonthe
nanos-tick/nanoparticle3WO3·H2OfilmandPrussianblue(PB)wasassembled.Asaresult,thecomplementary
deviceshowsahigheropticalmodulation(54%at754nm),alargercolorationefficiency(151.9cm2/C)
andfasterswitchingresponseswithableachingtimeof5.7sandacoloringtimeof1.3sthanasingle 3WO3·H2Olayerdevice,makingitattractiveforapracticalapplication.
© 2011 Elsevier Ltd. All rights reserved.
1. Introduction
Upon electron-transfer or redox reactions, materials that
undergoreversiblecolorchangeswithvariationsintheiroptical
spectraarecalledelectrochromicmaterials[1–3].Electrochromic
devicescomposedofthesematerials,whichallowforcontrolling
colorcycles,have attractedgreat interestthankstotheir
appli-cations important for smart windows[4–6], displays[7,8] and
antiglare mirrors [9]. The tunable light transmittance resulting
fromthecolorchangeoftheelectrochromicfilmsismuchdesired
insmartwindows,which donotonlyincreasetheaestheticsof
traditional windowsbut also save energy by reducing heating
or cooling loads of the building interiors [10]. Among various
electrochromicmaterials,tungstenoxide(WO3)hasbeen
exten-sivelystudiedbecauseof itshighcolorationefficiencyand high
cyclicstabilitycomparedwithothertransitionmetaloxides[11].
∗ Corresponding author at: School of Electrical and Electronic Engineering, NanyangTechnologicalUniversity,NanyangAvenue,Singapore639798,Singapore. Tel.:+6567905369;fax:+6567933318.
E-mailaddress:exwsun@ntu.edu.sg(X.W.Sun).
Moreover,WO3-basedelectrochromicdevicesexhibitlowpower
consumption,agoodmemoryeffectandahighcontrastratio[12],
offeringthedesiredadvantagesinsmartwindowsanddisplays.Itis
widelyrecognizedthatnanostructuredWO3,incomparisontotheir
compactbulkforms,offerpotentialadvantagesinelectrochromic
applicationduetotheirlargesurfaceareathatcouldbothincrease
thecontactareabetweentheelectrodeandelectrolyteandreduce
thediffusionpathofionsthroughtheporousstructures[13].And
the electrochromic efficiency of WO3 can befurther improved
by doping suitable metal ions with higher electronegativity or
loweroxidizingcapabilitythanWions,suchasMoandTi[14,15].
Recently, one-dimensional(1D) WO3 nanostructureswithlarge
surfaceareas,includingnanowires[16,17],nanorods[18,19]and
nanobelts[20],havebeeninvestigated.Forelectrochromic
appli-cations,WO3nanostructuresneedtobeassembledasathinfilm
onconductivesubstratesandthemicrostructuresofthefilm
con-cerning the electrochromic performance largely dependon the
filmassemblingtechniquesandprocessingconditions.Suchthin
filmsofWO3 havebeengrownbyvacuumdeposition[21],
elec-trodeposition[22],sol–gel[23]andhydrothermalmethod[24,25].
Hydrothermal approach is one ofthe mostpromising methods
for fabricatingWO3 film becauseof itsmerits oflow cost, low
0013-4686/$–seefrontmatter © 2011 Elsevier Ltd. All rights reserved. doi:10.1016/j.electacta.2011.12.069
154 Z.Jiaoetal./ElectrochimicaActa63 (2012) 153–160
reactiontemperature,flexiblesubstrateselectionandeasy
scaling-upfor production.Moreover,the microstructuresof WO3 films
grown by hydrothermal approach can be precisely tailored by
varyingtheprecursorconcentration,temperature,duration, and
adoptingvarioussurfactantsandcappingagents.
Todate,anumberofhydrothermalmethodshavebeen
devel-opedforpreparing 1DWO3 nanostructures,includingnanorods
[19]andnanoribbons[26] byaddingdifferentinorganicsaltsas
cappingagents.However,previousreportsofdirectlygrownWO3
thinfilmsonsubstrateusingatemplate-freehydrothermalprocess
andtheircorrespondingelectrochromiccharacteristicshavebeen
quitelimited.Forexample,Tu’sgroupreportsahydrothermally
grownWO3nanowirearraysfilmrecently[27].Ahighcoloration
efficiencyof102.8cm2/Candfastswitchingresponseof4.2sfor
col-orationand7.6sforbleachingisachievedforthisfilm.Ourgroup
hasalsofabricatednanobrickWO3 filmontransparent
conduc-tivesubstrateusingacrystal-seed-assistedhydrothermalmethod
previously[24].Thefilmshowsagoodcyclicstabilityand
com-parablecolorationefficiency(38.2cm2/C).Althoughconsiderable
achievementshavebeenmade,theelectrochromicpropertiesof
hydrothermallygrownnanostructuredWO3 filmscanbefurther
improvedbyincreasingtheirsurfacearea.Moreover,thecapping
agenteffectsonthemorphologyofthehydrothermallygrownWO3
filmsandtheirresultantelectrochromiccharacteristicshavenot
beentotallyunderstoodyet.
Comparedwithasinglelayerelectrochromicdevice,itiswell
knownthatacomplementarydevicecontainingtwoproper
elec-trochromiclayerscouldfurtherimprovetheperformance,suchas
theopticalmodulation, cyclicstability andcoloration efficiency
[28,29]. Prussian blue (PB, iron (III) [hexacyanoferrate (II)]), a
coordination-compoundedtransitionmetal hexacyanometallate,
isasuitablecomplementaryelectrochromicmaterialtoWO3due
toitsoutstandingelectrochromicperformanceandproper
oper-ationalvoltage range. Although complementary electrochromic
deviceswithimprovedpropertiesbasedonelectrodepositedWO3
andPBfilmshavebeenreported[30],tothebestofour
knowl-edge,littleworkhasbeendoneonapplyingthehydrothermally
grownnanostructuredhydratedtungstenoxidefilmsinsuchkind
ofdevices.
In this work, we make an attempt to grow nanostructured
WO3filmsdirectlyonFTO-coatedglassbyahydrothermalmethod
usingammoniumacetate(CH3COONH4)asthecappingagent.The
cappingeffectsofCH3COONH4onthestructure,morphologyand
electrochromicpropertyoftheresultingnanostructuredhydrated
tungstenoxidefilmsareinvestigated.Moreover,acomplementary
electrochromicdevicecombiningthehydratedtungstenoxidefilm
withPBfilmisfabricatedand,asaresult,increasedoptical
modu-lationandcolorationefficiencyisdemonstrated.
2. Experimental
2.1. Preparationofcrystalseedlayers,precursorand
hydrothermaltreatment
Thedetailedproceduresforpreparingcrystalseedlayerscan
befoundelsewhere[24].Inatypicalexperimentforpreparingthe
precursor,Na2WO4·2H2O(0.0655g)wasdissolvedinto20mLof
de-ionizedwaterandthen4mLofHClwasaddedintothe
solu-tionuntilnomoreprecipitatewasformed.Theabovesuspension
waskeptin ice bathforabout10min,thenthetop liquidpart
wasremovedandde-ionizedwaterwasaddedtoobtaina20mL
suspension.SubsequentlyH2O2(0.2g)wasaddedintotheabove
suspensionunderintenselystirringandheating.Thewhite
precip-itatewasdissolvedandatransparentsolutionwasobtained.After
stirringfor5min,CH3COONH4(0.1g)wasaddedasthecapping
Fig.1.Schematicofthecomplementarydevice.
agent.ThenNaOH(1mol)solutionwasslowlymixedintothis
solu-tionwhilerigorously stirringuntilthepHvalueof thesolution
reached1.5.For thepurposeofcomparison, asolutionwithout
adding cappingagentwas alsoused.Theas-prepared solutions
weretransferredintoautoclavesasprecursorsforhydrothermal
treatments.TheFTOglassescoatedbyWO3seedlayerswereput
intoautoclavesandthehydrothermalprocesswaskeptat180◦C
for18h.
2.2. ElectrodepositionofPBandpreparationofelectrochromic
device
TheelectrodepositionofPBfilmwascarriedoutbyastandard
three-electrodesystem,wherea cleanFTOservedasthe
work-ingelectrode, a platinum sheetasthecounter electrode, and a
40 35 30
No salt
With CH
3COONH
4W 4f
5/2Intensity (a.u.)
Binding Energy (eV)
W 4f
7/2(b)
60 50 40 30 20 10With CH
3COONH
4(440)
(044)
(400)
(420)
(331)
(113)
(222)
(202)
(220)
(022)
(200)
(002)
(111)
Intensity (a.u.)
2
θ(deg.)
(020)
Without CH
3COONH
4(a)
Fig.2.XRDpatterns(a)and(b)tungsten4fregionXPSspectraoftheas-synthesized thinfilmsgrownwithandwithoutCH3COONH4.
Fig.3.FESEMimagesof(a)and(b)thenanobrick3WO3·H2OthinfilmgrownwithoutCH3COONH4;and(c)and(d)nanostick/nanoparticlefilmwithCH3COONH4.Insets: cross-sectionalandHRTEMimage.
Ag/AgCl/sat’dKCl solutionas thereference electrode. The
elec-trodepositionbathofPBcontained10mmolK3Fe(CN)6,10mmol
FeCl3 and 0.1mol KCland theelectrodepositionof PBthin film
wascarriedoutbyapplyingaconstant cathodiccurrentdensity
of50A/cm2for300s.Thethicknessoftheas-depositedPBfilmis
about450nm(measuredbyaTENCORP-10SurfaceProfiler).Then
theWO3workingelectrodeandPBcounterelectrodewere
sand-wichedtogetherwithhot-meltSurlynspacers.Aliquidelectrolyte
composedof0.2molLiClO4in␥-butyrolactone(␥-BL)was
intro-ducedbetweenthetwoelectrodesbycapillaryaction.Finallythe
cellwassealedwithepoxy,whichisschematicallyshowninFig.1.
2.3. Characterization
ThephasesofthesynthesisproductswereidentifiedbyX-ray
powderdiffraction(XRD,Siemens),usingCuK␣1(=0.15406nm)
radiation. X-ray photoelectron spectroscopy (XPS) data were
obtained on a Kratos AXIS spectrometer with monochromatic
AlK␣(1486.71eV)X-rayradiation.Themorphologiesofthe
as-prepared thin films were observed by field emission scanning
electron microscope (FESEM, JSM6340). High-resolution
trans-mission electron microscopy (HRTEM) image was obtained by
aJEM-2100 microscopeusinganacceleratingvoltageof200kV.
Theopticalabsorbanceandtransmittancespectraweremeasured
usingaUV/Visspectrophotometer(JESCO V670).
Electrochemi-calmeasurements wereperformedbya three-electrodesystem
(VersaSTAT3FPotentiostat/Galvanostat)withLiClO4 (0.2mol)in
␥-BL as the electrolyte, Pt sheet as the counter electrode and
Ag/AgCl/sat’dKClasthereferenceelectrode.
3. Resultsanddiscussion
3.1. Structuresandmorphologiesofas-preparedfilms
Fig.2(a)showstheX-raydiffraction(XRD)patternsofthe
as-preparedthin filmsgrownwithandwithoutCH3COONH4.Both
filmsshowthesamecrystallinestructureandallpeakscanbewell
indexedtotheorthorhombicphaseof3WO3·H2O(JCPDF87-1203)
withthecorrespondinglatticeconstantsofa=7.345,b=12.547and
c=7.737 ˚A.Thesharppeaksindicatethegoodcrystallinequalityof
156 Z.Jiaoetal./ElectrochimicaActa63 (2012) 153–160 1.5 1.0 0.5 0.0 -0.5 -1.0 -3 -2 -1 0 1 2 2 4 6 8 10 -3 -2 -1 0 1 2 Cur re n t de n si ty (m A/ cm 2) Scan rate 1/2 (V1/2/s1/2)
Current d
e
nsity (mA/cm
2)
Potential (V vs. Ag/AgCl)
5mV/s-100mV/s
(b)
1 0 -1 -1.0 -0.5 0.0 0.5 1.0With CH
3COONH
4Without CH
3COONH
4C
u
rrent density (mA cm
-2
mg
-1)
Potential (V vs. Ag/AgCl)
(a)
1.0 0.5 0.0 -0.5 -1.0 -1 0 1 2 4 6 8 10 -2 -1 0 1 2 Scan rate 1/2 (V1/2/s1/2)Current density (mA/cm
2)
(c)
5mV/s-100mV/s
C
u
rrent den
sity (mA/cm
2)
Potential (V vs. Ag/AgCl)
1.5 1.0 0.5 0.0 -0.5 -1.0 -2 -1 0 1As prepared
1000th
2000th
C
u
rrent
density (mA/cm
2)
Potential (V vs. Ag/AgCl)
(d)
400 300 200 100 -5 0 5 1015
(e)
With CH
3COONH
4Without CH
3COONH
4Current densit
y
(mA/cm
2)
Time (s)
Fig.5. (a)Cyclicvoltammograms(CVs)ofthenanostick/nanoparticleandnanobrick3WO3·H2Ofilmsin␥-butyrolactonewith0.2molLiClO4;(b)and(c)CVsofthe nanos-tick/nanoparticleandnanobrickfilmatthescanratesof5,10,25,50and100mV/s,respectively.Insets:thecathodic/anodicpeakcurrentdensityasafunctionofthesquare rootofthescanrates;(d)CVsofthenanostick/nanoparticlefilmafter1st,1000th,and2000thcycles;and(e)chronoamperometry(CA)curveoftheas-synthesizedfilms recordedat±0.5Vfor40s.
theas-fabricatedfilms.TheelectrochromicperformanceofWO3is
closelyrelatedtoitscrystallinity.CrystallineWO3hasabetter
sta-bilitytoendureacidicelectrolytewithoutdegradationforalonger
cyclictimecomparedtoamorphousone,butatthecostofslower
responsetime andsmallercoloration efficiencyarisingfromits
smallerspecificsurfacearea[31].Byincreasingtheporosityand
preciselycontrollingthecrystalsize,crystallineWO3 filmswith
goodstabilityandfastresponsecansimultaneouslybeachieved.
Fig.2(b)showstheX-rayphotoelectronspectroscopy(XPS)dataof
1000 800 600 400 200 0 20 30 40 50 60
Transmittance (%)
Time (s)
(a)
0.036 0.030 0.024 0.018 0.012 0.4 0.6 0.8 1.0 36.8 cm2C-1Optical density
Charge density (C/cm
2)
(b)
1200 800 400 0 20 40 60Transmittance (%)
Time (s)
(c)
0.05 0.04 0.03 0.02 0.01 0.4 0.8 1.2 1.6 45.5 cm2C-1Optical density
Charge density (C/cm
2)
(d)
Fig.6.Insitutransmittanceresponseandcolorationefficiencyat754nmforthenanobrickfilm(aandb)andthenanostick/nanoparticlefilm(candd).
correctedusingavalueof284.5eVfortheC1speakofcarbon.For
bothfilms,twowell-resolvedpeaksatabout35.5and37.6eVin
thespectraareattributedtothespinorbitsplitdoubletpeaksofW
4f7/2andW4f5/2,respectively.Thesetwopeaksarewellseparated
withoutanyshoulders,indicatingthatallWatomsareinthe+6
oxidizationstates.
Fig.3shows themorphologiesoftheas-synthesizedfilms. It
canbeseenthatthefilmgrownwithoutCH3COONH4consistsof
irregularaggregatednanobrickswithsizesrangingfromtensto
hundredsofnanometers(seeFig.3(a)and(b)),whilethinfilmmade
upofstackednanosticksandnanoparticlesisobtainedbyadding
CH3COONH4 asthecappingagent(Fig.3(c)and(d)).The
nanos-tickswithanaveragelengthof∼50nmarehorizontallystacked
together,leading to a coarsesurface. A lot of small
nanoparti-cleswithsizesoftensofnanometersareaccumulatedunderneath
thesesticks.Clearlatticefringesofthehigh-resolution
transmis-sionelectronmicroscopy(HRTEM)imagefromananostick(inset
ofFig.3(d))indicateitssinglecrystallinequality.Theinset
cross-sectionalimageshowsthatthefilmwithathicknessof∼560nm
hasagood adherencetothesubstrate.Accordingtotherecent
report[32],orthorhombic3WO3·H2Oactuallycontainstwotypeof
corner-sharingWO6octahedras.Onetypeisconductedbya
cen-traltungstenatomthatissurroundedbysixoxygenatoms,while
inthesecondtype, twoof theoxygenatomsarereplaced bya
shorterterminalW ObondandlongerW (OH)2 bond,
respec-tively.Finally,the3WO3·H2Olatticeisformedbystackinguplayers
consistingofthesetwostructuralunits.Herein,theCH3COONH4
hasacappingeffectonthestackingofthesetwostructuralunits,
resultingintheformationofnanosticks.Fig.4schematically
illus-tratestheformationprocessofthefilmsgrownwithandwithout
CH3COONH4.
3.2. Electrochemicalandelectrochromicpropertiesofthe
as-prepared3WO3·H2Ofilms
Cyclicvoltammograms(CVs)wereinvestigatedforbothfilms
andshowninFig.5(a).TheseCVswerenormalizedwithrespect
tothegeometricareaandtotheweightof3WO3·H2Ofilmwithin
thatarea.Duringeachscan,thefilmsundergotypicalreversible
colorchangesfrombluetocolorless.Therecordedcurrentisdue
toLi+intercalation/deintercalationandelectrontransferbetween
W6+andW5+accordingtothefollowingreaction:
WO3·0.33H2O(bleach)+xLi++xe−↔LixWO3·0.33H2O(blue).
(1)
Theintegratedcathodic/anodiccurrentequatestotheamountofLi+
intercalation/deintercalation.Itcanbeclearlyseenthatthe
nano-stick/nanoparticlefilmgrownwithCH3COONH4 showsahigher
currentdensityforbothintercalationanddeintercalationprocesses
overthesametimeperiodthanthenanobrickone,indicatingfaster
Li+intercalation/deintercalationkinetics.Thetotalcathodiccharge
for the nanostick/nanoparticle film is about 4.2mCcm−2mg−1,
compared to only about 2.0mCcm−2mg−1 for nanobrick
films.
TheCVsofnanostick/nanoparticleandnanobrickfilmsrecorded
between−1.0and1.2VatvariousscanspeedsareshowninFig.5(b)
and(c),respectively.ItcanbeseenfromFig.5(b)thatwhenthe
scanspeedis5mV/s,therearetwooxidationpeaksthatappearat
about−0.83and−0.56V,andtworeductionpeaksthatappearat
−0.45and−0.85V.Withtheincreasedscan speed,thefirst
oxi-dationpeaksdisappear,whilethesecondpeaksgetbroaderand
158 Z.Jiaoetal./ElectrochimicaActa63 (2012) 153–160 800 700 600 500 400 0.4 0.8 1.2 1.6
PB+WO
3(hydrate)
PB
Absorbance (a.u.)
Wavelength (nm)
Fig.7.Opticalabsorptionspectraofacomplementaryelectrochromicdeviceanda singlePBlayerdeviceatthecoloredandbleachedstateunder±0.8V,respectively.
Thereductionpeaksshowasimilartrend.Whenthesecondanodic
peakcurrentdensitiesareplottedagainstthesquarerootofscan
rates,1/2,approximatelyalinearrelationshipisobtained(insetof
Fig.5(b)),whichsignifiesadiffusion-controlledprocess[33].The
effectivediffusioncoefficientDforthediffusingspeciesLi+canbe
estimatedfromthepeakcurrentdensity(jp)dependenceonthe
1000 800 600 400 200 0 0 20 40 60
Transmittance (%)
Time (s)
(a)
0.020 0.016 0.012 0.008 0.4 0.8 1.2 1.6151.9 cm
2C
-1Optical density
Charge density (C/cm
2)
(b)
Fig.8. (a)Switchingtimecharacteristicsbetweenthecoloredandbleachedstates forthecomplementaryelectrochromicdevicemeasuredat±0.8Vfor30sand(b) opticaldensityvariationwithrespecttothechargedensityrecordedat754nm.
squarerootofthepotentialscanrate(1/2)assumingasimplesolid
statediffusioncontrolledprocess[34]:
ıip ı√=2.69×10 5n3/2AC√D (2) D=0.1382×10−10n−3A−2C−2
ıip ı√ 2 (3)wherenisthenumberofelectronstransferredinunitreaction,A
istheeffectivegeometricsurfaceareaofthe3WO3·H2Oelectrode,
andCistheconcentrationofthediffusionspecies(Li+).The
effec-tivediffusioncoefficientsDLi+havebeencalculatedfromEq.(3)
tobe2.19×10−11and1.39×10−11cm2/sfortheintercalationand
deintercalationprocess,respectively,comparabletothereported
values[35].Fig.5(c)showstheCVsofthenanobrickfilmrecorded
atdifferentscanrates,showingasimilarprofilebutsmallercurrent
density.ThecalculateddiffusioncoefficientsDLi+are9.60×10−12
and6.101× 10−12cm2/sfortheintercalationprocessand
deinter-calationprocess,respectively,whicharesmallerthanthoseofthe
nanostick/nanoparticlefilm.Thefasteriondiffusionkineticsofthe
nanostick/nanoparticlefilmarisesfromitsmuchroughersurface,
whichincreasesitssurfaceareaandreducestheionsdiffusionpath
length.Thecyclicstabilityofthenanostick/nanoparticlefilmwas
alsomeasuredforthe1st,1000th,and2000thcycleatroom
tem-peratureandtheresultsareshowninFig.5(d).Thecurrentdensity
increasesslightlywithin2000cycles, withoutaclearchangein
theshapeofCVcurve,indicatingexcellentcyclicstabilityofthe
film,whichissimilartothereportedcrystallineWO3nanoparticles
[12].Chronoamperometry(CA)datawererecordedforbothfilms
withthepotentialbeingsteppedfrom−0.5Vto+0.5Vfor40s,as
showninFig.5(e).Duringeachcycle,the3WO3·H2Ofilmschange
frombleachedstatetocoloredstatereversibly.Forbothfilms,the
peakcurrentdensityofbleachingismuchhigherthanthatof
col-oration, and thecurrent densityduring bleaching decaysfaster
thancoloration.ThischaracteristicistypicalforWO3withsmall
ionintercalation/deintercalation[20].Thehigherbleachingcurrent
arisesfromthegoodconductivityoftungstenbronze(LixWO3),
and therapid currentdecay is due totheconductor (LixWO3
)-to-semiconductor(WO3)transition,whilethecoloringkineticsis
alwaysslower than thebleaching one for WO3 filmsowingto
the higher resistance during WO3 toLixWO3 transition.
More-over,thepeakcurrentdensitiesofcoloration/bleaching(−4.9and
14.1mA/cm2)ofthenanostick/nanoparticlefilmarehigherthan
those(−2.4and7.5mA/cm2)ofthenanobrickfilm.Theresponse
time(definedas70%decreaseofcurrentdensity)forcoloration
(tc)andbleaching(tb)arecalculatedfromcurrent–timetransient
datafromFig.5(e).Thenanostick/nanoparticlefilmshowsfaster
coloration/bleachingresponses(tc∼7.0sandtb∼3.0s)thanthose
(tc∼9.0sandtb∼3.5s)ofthenanobrickfilm,inwellagreement
withtheresultsinFig.5(a–c).Thefastresponsesforbothfilmsare
comparabletothespray-pyrolysisdepositedamorphousWO3film
[36].
The in situ transmittance responses of the
nanos-tick/nanoparticle and nanobrick film for a 90% transmittance
changewere alsoinvestigated at 754nm bya ±0.8V bias (see
Fig. 6(a) and (c)). For thenanostick/nanoparticle film, the
col-orationtimetc isfoundtobe7.9s, andthebleachingtime tb is
4.8s. However,for thenanobrick film,thecoloration time tc is
foundtobe7.3s,andthebleachingtimetbis7.1s.Thebleaching
speedofthenanostick/nanoparticlefilmismuchfasterthanthe
nanobrick film, butthe coloration speed is a little slower.It is
worth tomention that a larger optical modulationof ∼45% of
the nanostick/nanoparticle film is achieved, compared to that
only38%ofthenanobrickfilm.Colorationefficiency(CE)values
ofboth filmswerealsostudiedand shownin Fig.6(b)and (d),
Fig.9.Photographsofacomplementaryelectrochromicdeviceatthebleachedstate(a)and(b)thecoloredstateunder±0.8V,respectively.
linearregionofthecurve.It canbeseenthat thecalculated CE
ofthenanostick/nanoparticlefilmis45.5cm2/C,largerthanthat
ofthenanobrickfilm(36.8cm2/C).Theimprovedelectrochromic
performanceofthenanostick/nanoparticlefilmisduetoitslarge
surfacearea.
3.3. Opticalandelectrochromicpropertiesofthecomplementary
device
Tofurtherimprovetheopticalcontrast,colorationefficiencyand
switchingstability,thenanostick/nanoparticlefilmisincorporated
inanelectrochromicdevicewithananodicallycoloredPBfilmas
acomplementaryelectrochromiclayer.ThemorphologyandCV
curveoftheas-depositedPBfilmwerealsoinvestigatedandshown
inFigs.S1andS2,respectively(seesupplementaryinformation).
Fig.7showsopticalabsorptionspectraofthecomplementary
elec-trochromicdeviceandasinglePBlayerdeviceatthebleachedand
coloredstateundera±0.8Vbias.ComparedwiththesinglePBlayer
device,thecomplementarydeviceshowsalargeroptical
modu-lationabove410nm,especially inthenearIRregion,indicating
ahighercolorcontrastandlargerheatregulation.Moreover,the
complementarydevicedepictsahigherabsorptioninthenearUV
regionatbothcoloredandbleachedstatesduetotheabsorptionof
3WO3·H2Ofilms.Theaboveresultishighlydesiredinsmart
win-dowapplicationssincemoreheatcanbeprohibitedfromentering
theinteriorbuildings,resultinginareductionofcoolingloads.
Fig.8(a)showstheinsitucoloration/bleachingtransmittance
responseofthecomplementarydevicemeasuredat754nm.The
maximumtransmittancemodulation(T)ofcoloration/bleaching
wasfoundto beabout 54% afterapplying a ±0.8V voltage for
30s,agreeingwellwiththeabsorbancespectrashowninFig.7.
Obvious color changes can be observed during the switching.
Thecolorationandbleachingtimeextractedas90%transmittance
changesarefoundtobe1.3and5.7s,respectively.Theswitching
responsesofthecomplementarydeviceforboththecolorationand
bleachingprocessesare muchfasterthan thosereportedvalues
[30].For this complementaryelectrochromic device,limitations
of switching response are mainly due to 3WO3·H2O electrode.
The fastcoloration/bleaching kineticsmay beattributed tothe
largeactivespecific areaof theroughsurface, which facilitates
theionsintercalation/deintercalationbyreducingtheirdiffusion
lengths. CEofthe complementarycell wasalsoinvestigated at
its peak absorbance (=754nm) and shown in Fig. 8(b). The
calculated CE value is 151.9cm2/C, comparable to that of the
reported WO3||PB complementary device [30]. And the CE of
thecomplementarydeviceisimprovedbyabout234%compared
witha single3WO3·H2O electrochromic layer(CE=45.5cm2/C).
Photographs ofthe complementarydeviceare shown in Fig.9,
depicting a high contrast between the bleached and colored
states, which leads to the obvious transparence changes. The
deviceshowspromisingapplicationsinenergy-savingsmart
win-dows.
4. Conclusions
Insummary,uniformandwell-adhesive3WO3·H2Ofilms
con-sisted of nanosticks/nanoparticleswere synthesizedvia a facile
andtemplate-freehydrothermalmethodbyaddingCH3COONH4as
thecappingagent.Thinfilmscomposedofaggregatednanobricks
wereobtainedwithoutCH3COONH4.Thenanostick/nanoparticle
film depicts faster charge transfer and greater coloration
effi-ciency (45.5cm2/C) than the nanobrick film (36.8cm2/C). A
complementary electrochromic device based on the
nanos-tick/nanoparticle 3WO3·H2O film and PB film was fabricated
anddemonstrateslargeropticalcontrast(54%at754nm),faster
switchingresponse(tb=1.3sandtc=5.7s)andgreatercoloration
efficiency(151.9cm2/C)thanasingle3WO
3·H2Ofilmdevice.The
complementarydeviceholdsgreatpromiseforpotential
applica-tionsinenergy-savingsmartwindows.
Acknowledgments
The authorswould liketo thank thefinancial support from
the Science and Engineering Research Council, Agency for
Sci-ence,TechnologyandResearch(A*STAR)ofSingapore(projectNos.
0921010057and0921510088),SingaporeNRF-RF-2009-09,and
NationalNaturalScienceFoundationofChina(NSFC)(projectNos.
61006037and61076015).
AppendixA. Supplementarydata
Supplementarydataassociatedwiththisarticlecanbefound,in
theonlineversion,atdoi:10.1016/j.electacta.2011.12.069.
References
[1]C.G.Granqvist,P.C.Lansaker,N.R.Mlyuka,G.A.Niklasson,E.Avendano,Sol. EnergyMater.Sol.Cells93(2009)2032.
[2]R.J.Mortimer,Chem.Soc.Rev.26(1997)147. [3]C.R.Granqvist,Nat.Mater.5(2006)89. [4]C.M.Lampert,Sol.EnergyMater.11(1984)1.
[5]G.A.Niklasson,C.G.Granqvist,J.Mater.Chem.17(2007)127.
[6] C.G.Granqvist,A.Azens,A.Hjelm,L.Kullman,G.A.Niklasson,D.Ronnow,M.S. Mattsson,M.Veszelei,G.Vaivars,Sol.Energy63(1998)199.
[7]R.J.Mortimer,A.L.Dyer,J.R.Reynolds,Displays27(2006)2.
[8]P.Bonhote,E.Gogniat,F.Campus,L.Walder,M.Gratzel,Displays20(1999)137. [9]D.R.Rosseinsky,R.J.Mortimer,Adv.Mater.13(2001)783.
[10]R.Baetens,B.P.Jelle,A.Gustavsen,Sol.EnergyMater.Sol.Cells94(2010)87. [11]C.G.Granqvist,Sol.EnergyMater.Sol.Cells60(2000)201.
[12]S.H.Lee,R.Deshpande,P.A.Parilla,K.M.Jones,B.To,A.H.Mahan,A.C.Dillon, Adv.Mater.18(2006)763.
[13]H.D.Zheng,J.Z.Ou,M.S.Strano,R.B.Kaner,A.Mitchell,K.Kalantar-Zadeh,Adv. Funct.Mater.21(2011)2175.
[14] J.M.O-RuedadeLeón,D.R.Acosta,U.Pal,L.Casta ˜neda,Electrochim.Acta56 (2011)2599.
160 Z.Jiaoetal./ElectrochimicaActa63 (2012) 153–160
[16]H.G.Choi,Y.H.Jung,D.K.Kim,J.Am.Ceram.Soc.88(2005)1684. [17]K.Q.Hong,M.H.Xie,H.S.Wu,Nanotechnology17(2006)4830.
[18]D.Z.Guo,K.Yu-Zhang,A.Gloter,G.M.Zhang,Z.Q.Xue,J.Mater.Res.19(2004) 3665.
[19]J.M.Wang,E.Khoo,P.S.Lee,J.Ma,J.Phys.Chem.C112(2008)14306. [20]H.Wang,X.Quan,Y.Zhang,S.Chen,Nanotechnology19(2008)065704. [21]R.A.Batchelor,M.S.Burdis,J.R.Siddle,J.Electrochem.Soc.143(1996)1050. [22] S.H.Baeck,K.S.Choi,T.F.Jaramillo,G.D.Stucky,E.W.McFarland,Adv.Mater.15
(2003)1269.
[23] S.Balaji,Y.Djaoued,A.S.Albert,R.Bruning,N.Beaudoin,J.Robichaud,J.Mater. Chem.21(2011)3940.
[24] Z.H.Jiao,X.W.Sun,J.M.Wang,L.Ke,H.V.Demir,J.Phys.D:Appl.Phys.43(2010) 285501.
[25] J.Zhang,X.L.Wang,X.H.Xia,C.D.Gu,J.P.Tu,Sol.EnergyMater.Sol.Cells95 (2011)2107.
[26] Z.J.Gu,T.Y.Zhai,B.F.Gao,X.H.Sheng,Y.B.Wang,H.B.Fu,Y.Ma,J.N.Yao,J.Phys. Chem.B110(2006)23829.
[27]J.Zhang,J.P.Tu,X.H.Xia,X.L.Wang,C.D.Gu,J.Mater.Chem.21(2011)5492. [28]J.Zhang,J.P.Tu,X.H.Xia,Y.Qiao,Y.Lu,Sol.EnergyMater.Sol.Cells93(2009)
1840.
[29]H.Huang,J.Tian,W.K.Zhang,Y.P.Gan,X.Y.Tao,X.H.Xia,J.P.Tu,Electrochim. Acta56(2011)4281.
[30]A.Kraft,M.Rottmann,Sol.EnergyMater.Sol.Cells93(2009)2088.
[31]M.Deepa,T.K.Saxena,D.P.Singh,K.N.Sood,S.A.Agnihotry,Electrochim.Acta 51(2006)1974.
[32]L.Zhou,J.Zou,M.M.Yu,P.Lu,J.Wei,Y.Q.Qian,Y.H.Wang,C.Z.Yu,Cryst.Growth Des.8(2008)3993.
[33]A.J.Bard,L.R.Faulkner,ElectrochemicalMethods,Fundamentalsand Applica-tions,Wiley,NewYork,2001.
[34]I.Shiyanovskaya,M.Hepel,E.Tewksburry,J.NewMater.Electrochem.Syst.3 (2000)241.
[35]S.R.Bathe,P.S.Patil,SmartMater.Struct.18(2009)025004. [36] S.R.Bathe,P.S.Patil,Sol.EnergyMater.Sol.Cells91(2007)1097.