ContentslistsavailableatScienceDirect
Materials
Today
Communications
jo u r n al h om ep ag e : w w w . e l s e v i e r . c o m / l o c a t e / m t c o m m
Organic
electrolytes
for
graphene-based
supercapacitor:
Liquid,
gel
or
solid
Evgeniya
Kovalska
∗,
Coskun
Kocabas
DepartmentofPhysics,BilkentUniversity,06800Ankara,Turkey
a
r
t
i
c
l
e
i
n
f
o
Articlehistory: Received26April2016 Accepted27April2016 Availableonline6May2016 Keywords:
Graphene-basedsupercapacitor Organicelectrolyte
Electricalandelectro-opticalfeatures Opticalmodulator
a
b
s
t
r
a
c
t
Theelectrolyteisanimportantanddecisivefactorinbattery,capacitorandsupercapacitorfabrication. Herewereporthowelectrolyte’sprovenanceandstructureeffectontheelectro-opticalpropertiesof thegraphene-basedsupercapacitor.Thethreeorganicelectrolytesweresynthesized:liquidelectrolyte, whichonthebasisofpropylenecarbonate(PC),gelelectrolyte–polyvinylalcohol(PVA)andsolid electrolyte–polyvinylidenefluoride (PVDF).Asanapplication,wedemonstrateanoptical modula-torusingsupercapacitorstructurebuiltbygrapheneelectrodesandpreparedelectrolytes.Allorganic electrolyte-basedsupercapacitorspotentiateopticalmodulationofgrapheneelectrodesoverabroad rangeofwavelengths,underambientconditions.Werevealhighercapacitance(78F/cm2)fora
superca-pacitorwithgelelectrolyteduringvariousbiasvoltages.Werepresenttheincreasingoflighttransmission at3timesusingsolidelectrolyte,incomparisonwithliquidandgelelectrolytesandillustratethe super-capacitorpossibilitywithgelelectrolytetooperateundernegativevoltage.Consequently,wesuggest applyingofsolidelectrolyteasamoreappropriateelectrolyteforfabricationofgraphene-based super-capacitor.Weanticipatethatusingofsolidelectrolyteallowsustogetdesiredelectro-opticalproperties, minimizethesizeofthedeviceandvaryitshape.
©2016ElsevierLtd.Allrightsreserved.
1. Introduction
Thesupercapacitorhistory hasmorethanadozenyears,but
techniquedemandofsuchdevicesstillmakesscientistslookfor
waystoreducethecostoftheirdevelopmentandproduction[1].
Supercapacitor,whichalsowell-knownasultra-orelectric
double-layercapacitorstores energy through reversibleion adsorption
ontoactivematerialswithhighspecificsurfacearea[2]:activated
carbon[3],graphene[4,5],carbonaerogel[6,7],orcarbon
nano-tubes[8,9].Exceptcarbonmaterials,researchersuseelectroactive
oxideorhydroxidefilmsoftransitionmetals(MnO2[10],RuO2[11],
NiO[12],MoO3[13])andconductingpolymers(polypyrrole[14],
polyaniline[15],andpolythiophene[16]etc.).Thecyclicstability
andperformanceofsupercapacitordependonpropertiesof
elec-trolyteaswell.Electrolytes–theseareliquid,gelorsolidsystems
whichmusthavethehighconcentrationofmobileions,low
resis-tance,lowconcentrationofelectricallyactiveimpurities,andbe
chemicallystable[17,18].Forthepurposetogetquality
superca-pacitorwehavetofindtheoptimalcombinationofelectrodeswith
electrolyte.
∗ Correspondingauthor.
E-mailaddress:ikovalska@bilkent.edu.tr(E.Kovalska).
Liquidelectrolytes whichconsist ofwater and organicchains
haveionicconductivityupto1S/cm,highdielectricconstant[18],
andgivehigherspecificcapacitanceofactivematerialsthanthe
organic-basedelectrolyte.Thecellvoltageofsupercapacitorsbased
onaqueouselectrolyteislower(1V)[19]thanorganicelectrolyte
(2.5V)[20].Thus,wewereabletoobtainsignificantlybetterresults
withnon-aqueous[21],biologicalsubstances[22]orpolymersolid
electrolyte[23].Toavoidtheshaperestrictions,leakageordrying
ofelectrolyte(thatinherentofliquids)wecanusegelelectrolyte.
It hasfastcharging/dischargingandhighpowerdensity aswell
[24]. Currently,the majorpolymersfor gelelectrolyte
prepara-tionarepolyethyleneoxide[25],polyacrylonitrile[26],polymethyl
methacrylate[27]polyvinylidenefluoride[28]etc.Relativelynew
electrolyteforsupercapacitordesignissolidelectrolyte[29,30].This
materialoffersmanyadvantages overtheliquidsandgels:
con-ductionofelectricity,duetotheionmovementthroughvoidsor
defects,inowncrystallattice;leakageresistance,duetodispersion
andfixation,intoapolymermatrix;dualfunctionalizationas
sepa-ratorandelectrolyte.Solidelectrolytesimplementinthedesignof
flexibleandnonflexiblesupercapacitorsandshowexcellent
elec-trochemicalperformance[9,31,32].
Inanycase, propertiesofelectrolyteand itsstructure
deter-mine applied aspects of the supercapacitor. Thus, we report
syntheses of liquid, gel and solid organic electrolytes and
http://dx.doi.org/10.1016/j.mtcomm.2016.04.013 2352-4928/©2016ElsevierLtd.Allrightsreserved.
growthwascarriedoutcoolingdownwithH2 flowinguntilthe
temperaturewasbelow100◦C.Grapheneoncopperwastakenout
oftheCVD-reactorwhenthetemperaturereached50–60◦C.
2.2. TransferofmonolayergrapheneusingS1813
A photoresist S1813 (Shipley Company) supported transfer
methodwasutilizedtotransfergraphene(withtheareaaround
1×2cm)tothepolishquartzwafersforsupercapacitor
fabrica-tion.TheetchingprocesseswereperformedbyFeCl3 forCu-foil
andusingacetoneforremovingofphotoresist.
2.3. Fabricationgraphene-basedsupercapacitor
Supercapacitorcellwasformedusingtwocoveredbygraphene
glasswafers.Afterward,thevastnessbetweentwoelectrodeswas
filledwithanelectrolyteaccordingtoitstype.Wehaveusedthe
pipetteforliquidandgelelectrolytesandtweezersforathin
trans-parentfilmofsolidone.
2.4. Preparationoftheelectrolytes
Differenttypesofelectrolytesystemswhichbasedonorganic
chemicalswereprepared.
LiquidelectrolytewithactiveLi+-ionswereobtainedusinga
sol-ventpropylenecarbonate(PC–C4H6O3,99.7%,Sigma-Aldrich)and
thesourceofpositiveions–lithiumbis(oxalate)borate(LiBOB–
LiB(C2O4)2,powderofcrystals,Sigma-Aldrich).Themixturewas
stirredaround2.Atransparentanddilutedmilkcolorelectrolyte
withaconcentrationofLi+-ions10wt.%.werefinallyobtained.
LiBOBwasusedforgelelectrolytepreparationaswell.Polyvinyl
alcohol (PVA – (CH2CHOH)n, Sigma-Aldrich) with an average
molecularweightof20,000wasdissolvedin10%Li+-ionsaqueous
solution.Glycerin(C3H8O3,Birpa,Ankara)wasaddedasastabilizer.
Lastly,wehavegotgoodpellucidgelelectrolyte.
A solid electrolyte was obtained using polyvinylidene
flu-oride, with nominal Mn=130,000g/mol, Mw=400,000g/mol,
melting point 140–145◦C (PVDF) – molecular structure is
[CH2 CF2]n [CF2 CF(CF3)]m ,Sigma-Aldrich.Thepolymer
solu-tionwas preparedby dissolving10wt.%of PVDF inacetone at
70◦C under magnetic stirring for at least 30min until a clear
homogeneoussolutionwasobtained.Theionicliquidintheratio
1:4(polymer:ionicliquid,respectively)wasaddedtothepolymer
solutionundermagneticstirring andtheydissolvedcompletely
ina few minutes.Thefollowing ionicliquid whichsupplied by
Sigma-Aldrichwereused:1-butyl-3-methylimidazolium
hexaflu-orophosphate–C8H15F6N2P.Thefilmswerepreparedbysolution
castingofthepolymer/ionicliquidmixtureinacetoneonaPetri
dishandbysubsequentsolventevaporationatroomtemperature
for24h.Further,thefilmsweredriedat70◦Cfor4htoguarantee
completeremovalofthevolatilesolvent.
range between500and 1100nm.Thegraphene-based
superca-pacitorwasbiasedusingKeithley2400sourcemeasureunitthe
transmittancemeasurements.
3. Resultanddiscussion
The choice of graphene as an electrode caused by its high
absorptioncoefficientinbroadspectralrange,excellenttransport
propertiesandgate-tunablecarrierdensity.Theabilitytoproduce
high-qualitysingle-layergraphene[33,34],andtransferitonto
sub-stratemakespracticalapplicationofgrapheneforoptoelectronic
devices.Nowadaysgrapheneintegratedwithsiliconphotonicsis
especiallyinteresting[35]andwouldbeofuseforoptical
commu-nicationapplications[36].Forthispurposegraphene-on-graphene
optical modulator with parallel plate geometry was described
[37,38]. However, we would like to consider broadband
opti-calmodulatorwhichconsistsoftwographeneelectrodesonthe
glass/PVCwafersandelectrolytebetweenthem.Thedeviceshave
simpleparallelplategeometryandbasedonthesupercapacitor
structure.
3.1. Graphene-basedsupercapacitor
We present graphene-based supercapacitor which was
fab-ricated using glass wafers, covered with single-layergraphene
(Fig.1),andliquidorgelelectrolytes(Fig.2a);flexible
supercapac-itor,whereissolidelectrolytebetweentwographeneelectrodes
(Fig.2b).
Graphene-based device works on the principle of a typical
supercapacitor(Fig.2c),whichstoreselectricchargedirectlyacross
theinterface.Themechanismofsurfacechargegenerationcanbe
enumeratedassurfacedissociationandionadsorptionfromthe
electrolytesolution.Thecapacitancearisesfroman
electrochemi-caldoublelayeranditsthicknessdependsontheconcentrationof
theelectrolyteandsizeofactiveions.
3.2. Electrolytesforgraphene-basedsupercapacitor
Wetestedelectrolytesofvariouscompositionandstate:thefirst
electrolyteisliquid,thefollowingfive–gelsandremaining–are
solids(Table1).Toavoidleakageofelectrolyteandshape
limita-tionofthedeviceweusepolymericmatrixes:polyvinylalcohol
(PVA)andpolyvinylidenefluoride(PVDF);asasourceofionswe
uselithiumsaltorinorganicacids.Herein,wedistinguishand
com-parethreeelectrolytes,whichinouropinionaremostsuitablefor
supercapacitorsasanopticalmodulators[39].
3.3. Liquidelectrolyte–PC/LiBOB
We prepared the solutionof lithium bis (oxalate) borate in
propylene carbonate (PC/LiBOB) [40]. The choice fell onLiBOB
Fig.1.SEMimage(a)andtypicalRamanspectra(b)ofsinglelayergraphenefilmcoatedonSi/SiO2substrate.
Fig.2.Schematicexplodedviewofthenon-flexible(a)andflexible(b)opticallytransparentsupercapacitorsformedbytwoparallelgrapheneelectrodestransfer-printed onglass(a)orPVC(b)substratesandtheelectrolytemediumbetweenthem;schematicdrawingofbehaviorofthesupercapacitor(c).
Table1
Electrolytesforgraphene-basedsupercapacitor.
N TypeofEL Ratio Voltage(V) Modulation(%)
1 PC/LiBOB 1/1.1 0–2.0 1.0 2 PVA/H3PO4 1/1.5 0to−3.0/0to3.0 1.6/1.8 3 PVA/H2SO4 1/1.5 0to−3.0/0to3.0 2.3/2.5 4 PVA/LiBOB 3/1 0to−2.8/0to2.8 0.4/2.9 5 PVA/LiBOB/Eth/Ac 1/1 0to−2.4/0to3.0 2.7/3.2 6 PEO – 0to−3.0/0to3.0 1.0/2.3 7 PVDFinacetone/ionicliquid 1/4 0to2.8 3.2 8 PVDFinacetonitrile/ionicliquid 1/4 0to−2.8/0to3.0 1.3/1.5 9 PVDF/PEO 9/1 0to−3.5/0to3.0 2.3/1.3
Fig.3.Schematicbehaviorbetweenpropylenecarbonateandlithiumbis(oxalate) borate:lithiumcationfindsitselfsurroundedbynegativelychargedoxygenatomsof propylenecarbonate;[BOB]−anionsarelocatedintheelectrolytesolution,thereby determiningitsmobility.
andgoodcharging/dischargingcycles[41],wideelectrochemical
stability window, no erosionto manganese and iron’s cathode
materials,fluorine-free, non-toxic, etc. Furthermore, LiBOB has
weakestcoordinatingability(incomparisonwithcommonlyused
LiPF6[42]),caneffectivelystabilizethegraphiteanodesurfaceeven
inpurePC-basedelectrolytes,and cantolerateashighasabout
100ppmwatercontent[43,44].AproticPChasahighmolecular
dipolemoment(4.9D,duetothiswewereabletoobtain
solu-tionswithvarietysaltsconcentration)andexcellentperformance
atlowtemperatures.Highpolaritypropylenecarbonateallowsto
createaneffectivesolvationshellaroundlithiumcations(Fig.3),
therebyobtainingaconductiveelectrolyte.Accordingly,the
mobil-ityofelectrolytewilldeterminethe[BOB]−anions.
Electricalcharacterizationofa supercapacitorwithPC/LiBOB
electrolyte shows proportional voltage dependence of
capaci-tance/resistance(Fig.4a).Thecapacitance-voltagecurveindicates
highercapacitanceofthedevicearound40F/cm2 andminimal
pointat −0.34V.Theminimum valueof thecapacitance
corre-spondsthecharge neutralitypointsofgrapheneelectrodes and
dependsontheresidualchargedensity.Whilethealmost
asym-metricvoltagedependenceoftheresistancerepresentstwodistinct
peaksat9.4and12.7k.Thetotalresistanceofdevicevariedfrom
13to5.5kasabiasvoltagechangefrom−4.4to4.5V.
investigations.
3.4. Gelelectrolyte–PVA/LiBOB
Whereasexistingaproblemofliquidelectrolyteleakagewe
pro-posetousepolymer-basedgelelectrolyte.Obvious,thatgelplays
theroleofacontainerwhichholdssolventand,asaresult,possesses
thecharacteristicsofboth–liquidsandsolids.
TheadditionofLiBOBintopolyvinylalcohol(PVA)increasesthe
amorphousnessoftheelectrolyte[46].Ithappensduetothe
inter-actionofLi+cationofsaltwiththeoxygenatomofthehydroxyl
groupinPVA(Fig.5).ThePVAisabletosolvatealargeamount
ofsaltandprovidesareasonablyhighconductivity.Owingtothe
decompositiontemperatureofPVA(230◦C)andLiBOB(>290◦C)
theelectrolytecanbemorestableinabroadtemperaturerange.
The electrical characterization of a supercapacitor with
PVA/LiBOB shows symmetric voltage dependence of
capaci-tance/resistancecurves(Fig.6a)withabiasvoltagechangefrom
−2.0to1.0V. Thisoccursdue totheinteractionbetweenmore
activeions(Li+)and graphenesurface.Thegrapheneelectrodes
are neutralityat −1.2V that confirmed by one minimum on a
capacitance-voltagecurve.Thehigher capacitanceofthedevice
observesat78F/cm2.Analysisoftheresistance-voltagecurve(in
modefrom7.5to12k)showsemergingofthesolepeakat12k.
Theelectro-opticaltestdetectsthegradualgrowinginthe
trans-missionat3and0.4%,duringavarietyofthevoltagebetween0to
+2.8Vand−2.8to0V,respectively(Fig.6b).Thereby,the
superca-pacitorisactiveinoppositedirectionsduetoreactivityofbothions
(Li+andBOB−)inthedependenceonsuppliedvoltage.The
modu-lationofeachelectrodeisnegligiblewithawavelengthfrom600
to1100nmanditnormalizesat0V.
Fig.4.Thedependenceofthecapacitanceandresistance(a)andnormalizedchangeofthetransmission(b)ofsupercapacitorwithPC/LiBOBelectrolyteforvariousbias voltages.
Fig.5. Schematicinteractionbetweenlithiumbis(oxalate)borateandpolyvinyl alcoholviainteractionoflithiumcationsofsaltwiththeoxygenatomsofthe hydroxylgroupinPVA.
Thus,weachievedconductionwhichprovidesbyfreemobile
lithium cations and obtained following benefits: the polymer
matrixprovidesmechanicalstabilityandhelpstoavoidtheleakage
anddryingproblemsofelectrolyte;thesolventactsasaconducting
medium;thesupercapacitorwithPVA/LiBOBelectrolyteissuitable
forvisibleandnear-IRfrequencyinvestigationsinoppositeregions.
3.5. Solidelectrolyte–PVDF/ionicliquid
Toavoidchallengesofliquidandgelelectrolytes,during
super-capacitorfabricationanditstesting,weproposesolidelectrolyte–
polyvinylidenefluoride(PVDF)withionicliquid(Fig.7).Itisa
per-fectcombinationforthepurposeofthefabricationsolid-stateand
flexibledevice.
The PVDFmatrix is promising and suitable polymer due to
itshighdielectric constant (11.38 D), low crystallinity and low
glass transition temperature [47–49]. The (VDF)-phase makes
polymerchemicallystableandplastically[50],thestrong
electron-withdrawingfunctionalgroups( C F)–highlyanodicallystable
[25].
As a doping agent, we use ionic liquid
(1-butyl-3-methylimidazolium hexafluorophosphate), which have been
recognized as an ideal candidate to substitute the traditional
Fig.7. Schematicmolecularstructureandprotonhoppingmechanismbetween polyvinylidenefluorideand1-butyl-3-methylimidazoliumhexafluorophosphate.
electrolytes.Itpossessesuniqueproperties:low vaporpressure,
non-flammability,excellentelectrochemical/thermalstabilityand
unlikeaqueouselectrolyteshaswider electrochemicalwindows
(>1V)[51].
Theprofounddependenceofcapacitance/resistanceof
super-capacitorwithPVDF/ionicliquidelectrolytedemonstrateshigher
capacitanceofadeviceat15.5F/cm2andtotalresistancevaried
from4.5to13.5k.(Fig.8a).Applyingvoltagefrom−3to3V,we
obtaintwoclearlyneutralitychargedpointsofgrapheneelectrodes
onthecapacitance-voltagecurve(−0.5and0.5V)andtwoadjacent
peaks(13and11k)ontheresistance-voltagecurve.
Thenopticaltransmissionshift(from500to1100nm)appears
inapositiveregionfrom0to2.8V(Fig.8b).Thesearesymmetrically
changesin3.2%thatindicateamodulationoftwoelectrodes;the
transmissionconditionofsupercapacitornormalizedat0V.
Thus,dopingofpolymerwithionicliquidisagoodapproachto
developelectrolyteinthefilmform.Namely,thenonpolarnature
ofthePVDFprovidesstructuralintegrity and,atthesametime,
formshighionicallyconductivechannels,offeringitssuitabilityas
anelectrolyteinsupercapacitors.
4. Conclusions
Insummary,wereportelectro-opticalfeaturesofa
graphene-basedopticalmodulatorwithsupercapacitorstructureusingliquid,
gel,andsolidelectrolytes.Weestablishedthebestcapacitanceat
Fig.6.Thedependenceofthecapacitanceandresistance(a)andnormalizedchangeofthetransmission(b)ofsupercapacitorwithPVA/LiBOBelectrolyteforvariousbias voltages.
Fig.8.Thedependenceofthecapacitanceandresistance(a)andnormalizedchangeofthetransmission(b)ofsupercapacitorwithPVDF/ionicliquidelectrolyteforvarious biasvoltages.
78F/cm2forgelPVA/LiBOBelectrolyteandshowedits
possibil-itytooperateintwodirectionsaswell,duetothesimultaneous
activityofLi+ and[BOB] ions.We demonstratedcapacitance at
15.5F/cm2 and increasingof light transmissionin 3times for
solidPVDF/ionicliquidelectrolyte.Wenotedfollowingchallenges:
leakage/dryingunderanairofliquidPC/LiBOBelectrolyte,
impossi-bilitiesofusingofaqueousgelPVA/LiBOBelectrolyteinmicrowave
frequencyinvestigation.Therefore, wewouldliketodistinguish
mostsuitable electrolyte for graphene-based supercapacitors –
solidPVDF/ionicliquidelectrolytewithsatisfactoryelectro-optical
results,chemical/thermalstability,andflexibility.
We anticipate that application of the proposed electrolytes
togetherwithsimplicityandvarietyofthegraphene-baseddevice
geometrywillenableavarietyofadvancedopticaldevices
rang-ingfromplasmonicstooptoelectronics.Graphenesupercapacitor
can be used as a saturable absorber due to graphene
ultra-widebroadbandcapabilityandlowersaturationintensity.Anovel
supercapacitorwithtransparentgrapheneelectrodesfabricatedon
flexiblesubstratecouldapplyaselectricallyreconfigurableflexible
coatingsorsmartwindowsaswell.
Acknowledgement
This work was supportedby the Scientific and
Technologi-calResearchCouncilofTurkey(TUBITAK)grantno.114F052and
113F278.
References
[1]J.EnergyEng.139(2013)72–79.
[2]G.Wang,L.Zhang,J.Zhang,Chem.Soc.Rev.41(2012)797–828. [3]H.Shen,E.Liu,X.Xiang,Z.Huang,Y.Tian,Y.Wu,Z.Wu,H.Xie,Mater.Res.
Bull.47(2012)662–666.
[4]M.D.Stoller,S.Park,Y.Zhu,J.An,R.S.Ruoff,NanoLett.8(2008)3498–3502. [5]L.L.Zhang,R.Zhou,X.S.Zhao,J.Mater.Chem.20(2010)5983–5992. [6]J.Zou,J.Liu,A.S.Karakoti,A.Kumar,D.Joung,Q.Li,S.I.Khondaker,S.Seal,L.
Zhai,ACSNano4(2010)7293–7302.
[7]H.Hu,Z.Zhao,W.Wan,Y.Gogotsi,J.Qiu,Adv.Mater.25(2013)2219–2223. [8]A.Izadi-Najafabadi,S.Yasuda,K.Kobashi,T.Yamada,D.N.Futaba,H.Hatori,
M.Yumura,S.Iijima,K.Hata,Adv.Mater.22(2010)E235–E241. [9]M.Kaempgen,C.K.Chan,J.Ma,Y.Cui,G.Gruner,NanoLett.9(2009)
1872–1876.
[10]G.Yu,L.Hu,M.Vosgueritchian,H.Wang,X.Xie,J.R.McDonough,X.Cui,Y.Cui, Z.Bao,NanoLett.11(2011)2905–2911.
[11]B.J.Lee,S.R.Sivakkumar,J.M.Ko,J.H.Kim,S.M.Jo,D.Y.Kim,J.PowerSources 168(2007)546–552.
[12]Z.Ruifeng,M.Chuizhou,Z.Feng,L.Qunqing,L.Changhong,F.Shoushan,J. Kaili,Nanotechnology21(2010)345701.
[13]W.Tang,L.Liu,S.Tian,L.Li,Y.Yue,Y.Wu,K.Zhu,Chem.Commun.47(2011) 10058–10060.
[14]H.-H.Chang,C.-K.Chang,Y.-C.Tsai,C.-S.Liao,Carbon50(2012)2331–2336.
[15]Y.-Y.Horng,Y.-C.Lu,Y.-K.Hsu,C.-C.Chen,L.-C.Chen,K.-H.Chen,J.Power Sources195(2010)4418–4422.
[16]M.Mastragostino,C.Arbizzani,F.Soavi,J.PowerSources97–98(2001) 812–815.
[17]V.DiNoto,S.Lavina,G.A.Giffin,E.Negro,B.Scrosati,Electrochim.Acta57 (2011)4–13.
[18]B.E.Conway,W.G.Pell,J.SolidStateElectrochem.7(2003)637–644. [19]A.G.Pandolfo,A.F.Hollenkamp,J.PowerSources157(2006)11–27. [20]M.FrankRose,C.Johnson,T.Owens,B.Stephens,J.PowerSources47(1994)
303–312.
[21]W.Xu,C.A.Angell,Electrochem.SolidStateLett.4(2001)E1–E4. [22]M.D.Glasse,R.Idris,R.J.Latham,R.G.Linford,W.S.Schlindwein,SolidState
Ionics147(2002)289–294.
[23]J.Maranas,Solidpolymerelectrolytes,in:V.GarcíaSakai,C.Alba-Simionesco, S.-H.Chen(Eds.),DynamicsofSoftMatter,Springer,US,2012,pp.123–143. [24]A.ManuelStephan,Eur.Polym.J.42(2006)21–42.
[25]J.Y.Song,Y.Y.Wang,C.C.Wan,J.PowerSources77(1999)183–197. [26]G.Feuillade,P.Perche,J.Appl.Electrochem.5(1975)63–69.
[27]S.Ramesh,K.H.Leen,K.Kumutha,A.K.Arof,Spectrochim.ActaA66(2007) 1237–1242.
[28]F.J.BaltáCalleja,A.G.Arche,T.A.Ezquerra,C.S.Cruz,F.Batallán,B.Frick,E.L. Cabarcos,Structureandpropertiesofferroelectriccopolymersof
poly(vinylidenefluoride),in:H.G.Zachmann(Ed.),StructureinPolymerswith SpecialProperties,SpringerBerlinHeidelberg,1993,pp.1–48.
[29]C.Meng,C.Liu,L.Chen,C.Hu,S.Fan,NanoLett.10(2010)4025–4031. [30]C.Meng,C.Liu,S.Fan,Electrochem.Commun.11(2009)186–189. [31]J.J.Yoo,K.Balakrishnan,J.Huang,V.Meunier,B.G.Sumpter,A.Srivastava,M.
Conway,A.L.MohanaReddy,J.Yu,R.Vajtai,P.M.Ajayan,NanoLett.11(2011) 1423–1427.
[32]K.YuJin,C.Haegeun,H.Chi-Hwan,K.Woong,Nanotechnology23(2012) 065401.
[33]X.Li,W.Cai,J.An,S.Kim,J.Nah,D.Yang,R.Piner,A.Velamakanni,I.Jung,E. Tutuc,S.K.Banerjee,L.Colombo,R.S.Ruoff,Science324(2009)1312–1314. [34]E.O.Polat,O.Balci,N.Kakenov,H.B.Uzlu,C.Kocabas,R.Dahiya,Sci.Rep.5
(2015)16744.
[35]B.Jalali,S.Fathpour,J.LightwaveTechnol.24(2006)4600–4615. [36]D.A.B.Miller,Opt.Express20(2012)A293–A308.
[37]S.J.Koester,M.Li,Appl.Phys.Lett.100(2012)171107. [38]M.Liu,X.Yin,X.Zhang,NanoLett.12(2012)1482–1485. [39]E.O.Polat,C.Kocabas,NanoLett.13(2013)5851–5857.
[40]WuXu,C.AustenAngellz,Electrochem.Solid-StateLett.4(2001)E1–E4. [41]S.Wang,W.Qiu,T.Li,B.Yu,H.Zhao,Int.J.Electrochem.Sci.1(2006)250–257. [42]K.Xu,S.Zhang,T.R.Jow,W.Xu,C.A.Angell,Electrochem.SolidStateLett.5
(2002)A26–A29.
[43]L.Yang,M.M.Furczon,A.Xiao,B.L.Lucht,Z.Zhang,D.P.Abraham,J.Power Sources195(2010)1698–1705.
[44]K.Xu,S.Zhang,B.A.Poese,T.R.Jow,Electrochem.SolidStateLett.5(2002) A259–A262.
[45]Y.V.Pleskov,Russ.J.Electrochem.37(2001)871–872.
[46]I.S.Noor,S.R.Majid,A.K.Arof,Electrochim.Acta102(2013)149–160. [47]F.Wu,T.Feng,Y.Bai,C.Wu,L.Ye,Z.Feng,SolidStateIonics180(2009)
677–680.
[48]H.Xie,Z.Tang,Z.Li,Y.He,Y.Liu,H.Wang,J.SolidStateElectrochem.12 (2008)1497–1502.
[49]S.Ramesh,O.P.Ling,Polym.Chem.1(2010)702–707.
[50]M.Ulaganathan,S.Rajendran,J.Appl.Polym.Sci.118(2010)646–651. [51]T.Abdallah,D.Lemordant,B.Claude-Montigny,J.PowerSources201(2012)