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Anodic TiO2 nanotube layers decorated by Pd nanoparticles using ALD: An efficient electrocatalyst for methanol oxidation

Bawab, Bilal; Thalluri, Sitaramanjaneya Mouli; Rodriguez Pereira, Jhonatan; Sopha, Hanna Ingrid; Zazpe Mendioroz, Raúl; Macák, Jan

Abstract

Herein, we report the performance of Pd nanoparticles (NPs) prepared by Atomic Layer Deposition (ALD) as a catalyst for methanol electro-oxidation. Pd NPs were decorated onto anodic TiO2 nanotube (TNT) layers as supporting material that possess a large available surface area and direct electrical contact via the underlying titanium foil. Different Pd loadings (150 - 300 - 450 - 600 ALD cycles) show different particles sizes ranging between 7 and 12 nm, as revealed by transmission electron microscopy. Coalescence dominated visibly from 450 ALD cycles, which led to a porous Pd layer all along the TNT walls rather than the growth of individual particles. Electrocatalytic performance was investigated by cyclic voltammetry (CV), where the catalytic activity increased proportional with Pd loading up to the highest values for 400 and 450 cycles, whereas a further increase in the number of ALD cycles (N-ALD) did not show any additional improvement in methanol oxidation current densities. TNT layers decorated with 400, 450 and 600 Pd ALD cycles show featureless curves suggesting complete anti-poisoning ability or possibly a proof of a direct conversion from CH3OH to CO2 (without any intermediate byproducts). The lack of an oxidation peak during the anodic scan and therefore a reduction peak during the cathodic scan, confirms Pd NPs (stabilized by TiO2) efficiently utilize OHads and chemisorbed CH3OH in a way that its CO poisoning was inhibited. As a result, the tuned high surface area TNT layers exhibited excellent performance as a supporting material for Pd NPs against formation of electrochemical poisoning species. Finally, the mechanism of the TNT layers interaction with Pd NPs, which led to the propelling methanol oxidation reaction without loss in performance over cycling is postulated.

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Elec ochimica Ac a 429 (2022) 141044 A ailable online 15 Augus 2022 0013-4686/© 2022 The Au ho s. Published by Else ie L d. This is an open access a icle unde he CC BY-NC-ND license (h p://c ea i ecommons.o g/licenses/by- nc-nd/4.0/). Anodic TiO 2 nano ube laye s deco a ed by Pd nanopa icles using ALD: An e icien elec oca alys o me hanol oxida ion Bilal Bawab a , Si a amanjaneya M. Thallu i a , b , Jhona an Rod iguez-Pe ei a a , b , Hanna Sopha a , b , Raul Zazpe a , b , Jan M. Macak a , b , * a Cen al Eu opean Ins i u e o Technology, B no Uni e si y o Technology, Pu kyno a 123, 61200 B no, Czech Republic b Cen e o Ma e ials and Nano echnologies, Facul y o Chemical Technology, Uni e si y o Pa dubice, Nam. Cs. Legii 565, 53002 Pa dubice, Czech Republic ARTICLE INFO Keywo ds: TiO 2 nano ube laye s Pd nanopa icles A omic Laye Deposi ion Elec oca alysis Me hanol elec o-oxida ion ABSTRACT He ein, we epo he pe o mance o Pd nanopa icles (NPs) p epa ed by A omic Laye Deposi ion (ALD) as a ca alys o me hanol elec o-oxida ion. Pd NPs we e deco a ed on o anodic TiO 2 nano ube (TNT) laye s as suppo ing ma e ial ha possess a la ge a ailable su ace a ea and di ec elec ical con ac ia he unde lying i anium oil. Di e en Pd loadings (150 – 300 – 450 – 600 ALD cycles) show di e en pa icles sizes anging be ween 7 and 12 nm, as e ealed by ansmission elec on mic oscopy. Coalescence domina ed isibly om 450 ALD cycles, which led o a po ous Pd laye all along he TNT walls a he han he g ow h o indi idual pa icles. Elec oca aly ic pe o mance was in es iga ed by cyclic ol amme y (CV), whe e he ca aly ic ac i i y inc eased p opo ional wi h Pd loading up o he highes alues o 400 and 450 cycles, whe eas a u he inc ease in he numbe o ALD cycles (N ALD ) did no show any addi ional imp o emen in me hanol oxida ion cu en densi ies. TNT laye s deco a ed wi h 400, 450 and 600 Pd ALD cycles show ea u eless cu es sugges ing comple e an i- poisoning abili y o possibly a p oo o a di ec con e sion om CH 3 OH o CO 2 (wi hou any in e media e byp oduc s). The lack o an oxida ion peak du ing he anodic scan and he e o e a educ ion peak du ing he ca hodic scan, con i ms Pd NPs (s abilized by TiO 2 ) e icien ly u ilize OH ads and chemiso bed CH 3 OH in a way ha i s CO poisoning was inhibi ed. As a esul , he uned high su ace a ea TNT laye s exhibi ed excellen pe o mance as a suppo ing ma e ial o Pd NPs agains o ma ion o elec ochemical poisoning species. Finally, he mechanism o he TNT laye s in e ac ion wi h Pd NPs, which led o he p opelling me hanol oxida ion e- ac ion wi hou loss in pe o mance o e cycling is pos ula ed. 1. In oduc ion The e e -inc easing global ene gy demand, along wi h he en i on- men al issues o igina ed om he use o ossil uel, igge ed an in ense sea ch o sus ainable and clean ene gy al e na i es. Di ec me hanol uel cells (DMFCs), in which he chemical ene gy s o ed in me hanol is con e ed o elec ical ene gy, ha e been explo ed in he las yea s. Unlike hyd ogen uel cells, DMFCs use liquid uel ha allows easie handling and anspo a ion. The wo main eac ions ha de e mine he ac i i y o DMFCs a e he anodic me hanol oxida ion eac ion (MOR) and ca hodic oxygen educ ion eac ion (ORR) [1]. The ca aly ic eac- ion kine ics du ing he uel cell ac i i y is dependen on he elec ode su ace mo phology and/o nanopa icles (NPs) sizes. La ge NPs can ela i ely inc ease he NPs su ace exposed o he su ounding elec o- ly e as compa ed o he in e ac ed subs a e su ace [2]. In con a y, smalle NPs a e less likely o ha e CO poisoning specially a high em- pe a u es, due o oxygen bond b eak esul ing in oxygen deso p ion a his le el, which shows mo e esis an o CO poisoning [3]. Noble me al-me al oxide–suppo in e ac ions gene ally play a signi ican ole in elec oca alysis, as hey main ain a high ca aly ic ac i i y o noble me al NPs due o hei ole ance owa ds poisoning om eac ion byp oduc s. The use o me al oxide suppo s, such as MnO 2 [4], SnO 2 [5], o TiO 2 [6], p o ed o be e y bene icial as hey a e highly s able and main ain consis en con e sion e iciency in uel cells. Suppo ing ma e ials, deco a ed by NPs as a ca alys , enhance he elec on anspo a he ca alys /elec oly e in e ace. The p esence o oxide as a sup- po ing ma e ial, whe he i is a educible me al oxide, such as TiO 2 o FeO x , o a non educible oxide such as Z O 2 [7], can di ec ly a ec he ca aly ic ac i i y. Fo ins ance, in ca aly ic con e e s used in he au omo i e indus y, CO in e ac s wi h oxygen on he ca alys su ace * Co esponding au ho . E-mail add ess: [email p o ec ed] (J.M. Macak). Con en s lis s a ailable a ScienceDi ec Elec ochimica Ac a jou nal homepage: www.jou nals.else ie .com/elec ochimica-ac a h ps://doi.o g/10.1016/j.elec ac a.2022.141044 Recei ed 20 Ma ch 2022; Recei ed in e ised o m 3 Augus 2022; Accep ed 14 Augus 2022 Elec ochimica Ac a 429 (2022) 141044 2 p oducing CO 2 . Hence, he eac ion can p oceed in wo di ec ions. In case he suppo ing ma e ial p o ides oxygen, as i happens wi h TiO 2 , hese oxygen a oms will subs i u e he missing oxygen on he su ace. O he wise, CO mos likely subs i u es oxygen a oms and deac i a es he su ace [8]. In pa allel, app oaches based on a ia ions in he elec ode mo phology (nano-, meso-, and mac opo ous ma e ials) ha e shown a huge impac o p e en he de elopmen and accumula ion o in e - media e p oduc s on he ac i e elec ode su ace. In addi ion, he use o alkaline elec oly es showed highe ca aly ic ac i i y owa ds he anodic egime compa ed wi h acidic elec oly es [9]. One mus bea in mind ha es ing noble me als, such as Pd, unde in ense anodic condi ions in alkali medium can esul in o al deac i a ion, due o he o ma ion o Pd hyd oxyla es. Also he elec oly e concen a ions can di ec ly in luence he MOR a e [10]. Rega ding he noble me al NPs used as ca alys owa ds me hanol elec o-oxida ion, he inhe en s abili y o P makes i a g ea ca alys choice as an anode in DMFCs. Howe e , aking in o conside a ion he P sca ci y and he co esponding high cos s o la ge scale P p oduc ion, a sea ch o al e na i e ca alys s has been ini ia ed. Alloys o P wi h o he noble me als, such as Pd, a e conside ed o be used on DMFCs elec odes in o de o educe o subs i u e P mass. While a comple e me hanol (CH 3 OH) oxida ion du ing he elec ochemical p ocess in ol es he ans e o 6 elec ons o ob ain CO 2 as an end-p oduc , incomple e oxida ion can esul in o he undesi ed p oduc s such as o maldehydes, o mic acids, and CO [11]. Pd has he endency o bond wi h CO mol- ecules, which leads o poisoning o he ac i e su ace. E en a lowe empe a u es, he p ocess can s ill acili a e CO o eac , o ming Pd (CO) x compounds [12]. Hyd a ion eac ion ha is mo e p edominan on Pd su ace as compa ed o P , can la e o m OH g oups ha suppo he de-poisoning p ocess o he in e media e “CO” du ing me hanol oxida- ion [13], as shown la e in his pape . The impo ance o ha ing NPs is based on he ac , ha i signi i- can ly imp o es he su ace o olume a io, p o iding mo e ca aly ic ac i e si es. The g ow h o uni o m Pd NPs on high speci ic su ace a ea suppo ing ma e ials is o pa amoun impo ance due o he imp o ed NPs coun pe uni a ea o suppo , hus inc easing he ca aly ic ac i i y o he p ocess. Se e al epo s we e epo ed on he employmen o Pd NPs on di e en subs a es [14–16]. The a ailable li e a u e shows ha he deposi ion o Pd NPs on TNT laye s u ilizing di e en echniques such as elec ochemical milling [17], chemical ba h deposi ion [18,19] and elec odeposi ion [20], su e s om non-uni o m deposi ions wi h a ia ions in co e age densi y all along he su ace. Some o he pub- lished li e a u es ha e ocused on ALD based deposi ion o Pd NPs on TNT laye s o hei applica ions on o ganic molecule deg ada ion [2,15, 21,22]. Well dispe sed Pd NPs o e TNT laye s we e ob ained in hese pape s and hei ac i i ies o di e en ca aly ic eac ions we e p o- posed. Howe e , TNT laye s as a s andalone a e no a good ma e ial o he elec oca aly ics pu poses, knowing i s poo elec ical conduc i i y. Howe e , as a suppo ing ma e ial, high su ace a ea TNT laye s can be de imen al o acili a e he oxida ion o eac an molecules (me hanol). This is due o an eno mous amoun o su ace hyd oxyl g oups ha a e well known o oxidize in e media e p oduc s, majo ly CO gene a ed du ing me hanol elec ooxida ion [23]. The aim o he cu en s udy is o con o maly deco a e TNT laye s by homogeneously dis ibu ed Pd NPs using ALD and o e alua e hei ca aly ic ac i i y p o iles o me hanol elec o-oxida ion. The e o e, he abili y o Pd NPs on TNT (Pd/TNT) laye elec odes o wi hs and agains su ace poisoning is elabo a ed. Pd NPs we e deco a ed by ALD on o 5 µm hick ana ase TNT laye s. The mo phology and he chemical composi ion o he esul ing Pd/TNT laye s we e in es iga ed in de ail by scanning elec on mic oscope (SEM), ansmission elec on mic o- scope (TEM), X- ay di ac ion (XRD), and X- ay pho oelec on spec- oscopy (XPS). The elec oca aly ic ac i i y o Pd/TNT laye s owa ds me hanol elec o-oxida ion was e alua ed by cyclic ol amme y (CV) and ch onoampe ome y (CA) as a unc ion o he numbe o ALD cycles. 2. Expe imen al pa 2.1. TNT laye p epa a ion The de ailed p o ocol o he TNT laye was published in ou p e i- ous wo k [24]. B ie ly, Ti oils (Sigma-Ald ich, 0.127 mm, 99.7% pu i y) we e deg eased and anodized a oom empe a u e using a high- ol age po en ios a (PGU-200 V, IPS Elek oniklabo GmbH) o de elop TNT laye s o ~5 µm hickness and ~230 nm diame e in an e hylene glycol-based elec oly e con aining 10% wa e and 0.15 M NH 4 F a 100 V o 4 hou s. Ti oils and TNT laye s we e annealed in ai o 1 h a 400 ᵒ C. 2.2. A omic laye deposi ion o Pd Pd NPs we e deposi ed on o TNT laye s and on o annealed Ti oils using TFS 200 ALD eac o (Beneq) p o ided wi h s op- low con igu a- ion. Palladium(II)hexa luo oace ylace ona e Pd(C 5 HF 6 O 2 ) 2 (95%, S em Chemicals) and o malin (37% o maldehyde in wa e wi h 10–15% o me hanol, Sigma-Ald ich) we e used as he Pd p ecu so and co- eac an , espec i ely. Pd p ecu so was hea ed up o 65◦C, while he deposi ion p ocess empe a u e was 200◦C. One ALD cycle (N ALD =1) was de ined by he ollowing sequence: Pd pulse (2 s)-exposu e (10 s)-N 2 pu ge (20 s)- o malin pulse (1 s)-exposu e (10 s)-N 2 pu ge (20 s). A p elimina y s ep o enhance he densi y o hyd oxyl unc ional g oups on he su ace subs a e was applied o imp o e he Pd nuclea ion. Such p elimina y s ep consis ed o 5 ALD cycles (wa e pulse (0.5 s)-exposu e (10 s)-N 2 pu ge (20 s)) ollowed by 20 cycles (Pd (0.25 s)-exposu e (10 s)-N 2 pu ge (20 s)) was employed wi h pulse, exposu e, and pu ge du- a ions p og ammed as “5 * (0.5:10:20 s) and 20 * (0.25:10:20 s)” o H 2 O and Pd p ecu so espec i ely p io o he ac ual deposi ion o Pd. The sole necessi y o H 2 O pulse is o c ea e -OH unc ional g oups on he subs a e so ha Pd can nuclea e e icien ly. 2.3. Cha ac e iza ion me hods Blank and Pd deco a ed TNTs (Pd/TNTs) and Pd/Ti oils we e cha ac e ized by scanning elec on mic oscope (SEM) FEI Ve ios 460L. Pd/TNTs we e also cha ac e ized bya high- esolu ion ansmission elec on mic oscope (HRTEM) The mo Fishe Scien i ic Ti an Themis 60-300, ope a ed a 300 kV and equipped wi h a C s image abe a ion co ec o , a high angle annula da k ield de ec o o scanning ans- mission elec on mic oscopy (STEM-HAADF) imaging, and Supe -X en- e gy dispe si e X- ay (EDX) spec ome e wi h ou 30 mm 2 windowless de ec o s o STEM-EDX analysis o check he mo phology and Pd NPs size/dis ibu ion. The c ys alline s uc u e o Pd/TNT laye s was assessed using X- ay di ac ion XRD (Rigaku Sma lab 3 kW di ac- ome e equipped wi h Cu-K α 1 adia ion sou ce). Su ace chemical s a e o Pd NPs be o e and a e elec ochemical measu emen s we e s udied using X- ay pho oelec on spec oscopy (XPS) K a os Analy ical Axis Sup a ins umen , wi h Al-K α monoch oma ic X ay sou ce (h ν = 1486.69 eV). The spec a we e decon olu ed using CasaXPS so wa e and e e enced o he Femi Le el cu o , which means a 0 eV on he binding ene gy scale. Pd 3d spec a we e decon olu ed wi h asymme ic Lo en zian unc ion LA (1.5, 4, 45) o me allic s a e (Pd 0 ), mixed Gaussian-Lo en zian unc ions GL (30) o Pd oxides o hyd oxides and Pd plasmon loss. 2.4. Elec ochemical analysis The elec ochemical measu emen s we e ca ied ou in a no mal h ee elec odes elec ochemical cell a oom empe a u e. Au olab VIONIC po en ios a suppo ed by INTELLO so wa e was used o his pu pose. Two solu ions o 1M KOH and 1M KOH/CH 3 OH we e used as elec oly es. The e e ence elec ode was Ag/AgCl 3M KCl (E ֯ =0.210 V s RHE). A P oil was used as coun e elec ode, whe e Pd deco a ed Ti B. Bawab e al. Elec ochimica Ac a 429 (2022) 141044 3 oils (Pd/Ti) and Pd/TNT laye s we e used as wo king elec odes. Be o e e e y measu emen , degassing o all elec oly es was ca ied ou by bubbling wi h ul a-high pu i y ni ogen o a leas 15 minu es, his o ensu e he emo al o he dissol ed unwan ed oxygen ha can in e e e du ing he elec ochemical oxida ion p ocess. All po en ials gi en in his pape we e ecalcula ed e sus RHE. Cyclic ol amme ic (CV) mea- su emen s we e ca ied a a scanning a e o 10 mV s −1 . Elec ochemical impedance spec oscopy (EIS) was conduc ed using he same se up as abo e, using me hanolic KOH as a solu ion a 0.8 V s. RHE. In o de o check and compa e he s abili y o a ious Pd/TNT laye s and Pd/Ti oils, ch onoampe ome ic (CA) measu emen s we e pe o med a an applied po en ial o 0.9 V s RHE o 2 hou s. The geome ical su ace a ea (0.636 cm 2 ) was used o de e mine he cu en densi ies. In addi- ion, he elec ochemical ac i e su ace a ea (ECSA) has been de e - mined and compa ed wi h he li e a u e esul s. 3. Resul s and discussion Fig. 1 shows SEM op- iew images o TNT laye s (5 µm hick and wi h an inne diame e o ≈250 nm) deco a ed wi h Pd NPs using di e en Figu e 1. SEM op iews o 5 µm hick TNT laye s deco a ed wi h Pd NPs using di e en N ALD : (a) 0, (b) 150, (c) 300, (d) 350, (e) 400, ( ) 450, (g) 600. The scale ba s in all images ep esen 300 nm. B. Bawab e al. Elec ochimica Ac a 429 (2022) 141044 4 numbe o Pd ALD cycles (N ALD ): 0, 150, 300, 350, 400, 450 and 600. Homogenous dis ibu ion o Pd NPs all along he inne and ou e TNT walls was e i ied. As one can expec , an inc ease in he N ALD esul s in a highe densi y o Pd NPs on he TNT laye su ace. F om N ALD ≥450 cycles (Fig. 1d), Pd NPs s a o coalesce esul ing in o a po ous Pd laye . Figu e S1 shows SEM op- iew images o Ti oils deco a ed wi h Pd NPs using di e en numbe o Pd ALD cycles (N ALD ): 0, 150, 300, 350, 400, 450 and 600. The Pd NPs a e al eady coalesced a 300c, which is much ea lie han o he TNT laye s, which o e sligh ly di e en nuclea ion densi y and much highe su ace a ea o hos highe loading o Pd. Conside ing he coalescence, he analyses o NPs size om Pd/Ti has no o limi ed sense. Mo eo e , TEM analysis o hese specimens is no possible, as hey a e oo hick o elec ons o pass h ough. Co esponding EDX analyses o Pd/TNTs p o ided he weigh pe - cen age (w %) dis ibu ion o C, Ti, O, and Pd. Figu e S2 shows an in- c ease in Pd con en on Pd/TNT laye s wi h inc easing N ALD . EDX spec a shown in Figu e S3 app o e he inc easing Pd along wi h inc easing N ALD . The mo phological ea u es o Pd/TNT laye s we e u he cha ac- e ized by HRTEM and compa ed wi h he non-deco a ed Pd laye (0 N ALD ). TEM images in Fig. 2 p o ide an o e iew o high- esolu ion images showing he size and dis ibu ion o Pd NPs on TNTs. The Pd Figu e 2. TEM images o single TNT wi h Pd NPs g own a e 0 (a), 150 (b), 300 (c), 450 (d), and 600 (e) Pd N ALD , espec i ely. ( ) A e age NPs size as unc ion o N ALD ( o he same samples as in a) o e)). B. Bawab e al. Elec ochimica Ac a 429 (2022) 141044 5 NPs we e uni o mly dis ibu ed all along he walls o TNT laye s. As men ioned abo e, Pd NPs coalescence s a ed om 450 ALD cycles (Fig. 2d). Rega ding he Pd NPs size dependency wi h he numbe o ALD cycles, Fig. 2 shows he a e age Pd NPs size o each sample wi h di e en numbe o ALD cycles, de e mined using he s a is ical analyses om TEM images. A e age Pd NPs sizes o 150, 300, and 450 ALD cycles we e 7.5, 10.5, and 12.5 nm espec i ely. A highe N ALD (600) ende ed he coalescence o Pd NPs, hus ini ia ing he p ocess o o m a po ous Pd laye along he TNT walls. XRD pa e ns o he blank TNT laye in Fig. 3a show ypical peaks o ana ase TiO 2 phase wi h he majo peaks loca ed a 25.2◦and 48◦ ep- esen ing (101) and (200) ana ase peaks. The addi ional peaks obse ed a 38.4◦and 40.2◦ ep esen he (002) and (101) c ys alline planes o Ti subs a e. The (111) Pd plane di ac ion peak obse ed o highe Pd deco a ed TNTs (450 and 600 N ALD ) should appea a 40.1◦bu due o o e lapping wi h Ti (101) peak i is di icul o disce n. Ha ing a close look a 600 N ALD 40.1ᵒ peak, he peak becomes b oade (compa ed o o he peaks) wi h a lowe in ensi y co e ing bo h 40.1◦and 40.2◦, his is due o he dec easing size o Pd NPs c ys als. A b oad peak de ec ed a ound 46.2◦could be asc ibed as Pd (200), which was isible only in TNT laye s deco a ed wi h 450 and 600 Pd N ALD . This could be due o o ma ion o po ous Pd s uc u e unlike he samples deposi ed wi h a lowe N ALD (150 and 300) e ealing mo e dispe sed Pd NPs wi hin TNT walls, p e en ing X- ay di ac ion de ec ion. Fig. 3b show high esolu ion Pd, Pd 3d XPS spec a ob ained be o e and a e he CA. Bo h spec a show he co esponding spin-o bi spli - ing Pd 3d 5/2 / Pd 3d 3/2 wi h simila shapes. Se en componen s we e used o decon olu e bo h spec a; six associa ed o he spin-o bi spli - ing, which co espond o h ee di e en chemical species, and he le o e o he cha ac e is ic plasmon loss ha appea s as Pd is mos ly me allic. The i s double ( ed peaks) a e cen e ed a 335.3 / 340.6 eV con i ming he p esence o me allic Pd (Pd 0 ) [25]. The binding ene gies co esponding o he second double (blue peaks) a 336.9 / 340.5 eV, we e ela ed o Pd 2+ [26], while hose om he hi d double (g een peaks), loca ed a 338.7 / 344.0 eV we e assigned o Pd 4+ [27]. Pd 2+ and Pd 4+ could be ela ed o co esponding oxides o hyd oxides [28,29]. Since no majo di e ences we e ound om chemical species and/o binding ene gies shi s in Pd spec a be o e and a e he elec ochemical measu emen s, quan i ica ion o he oxida ion s a es was pe o med, as shown in Fig. 3c. Acco ding o hese esul s, i is e iden ha a e CA measu emen s he amoun o me allic Pd dec eases sligh ly (a ound 4.3%), while he con en o Pd 2+ inc eases. The su ace chemical s a e o TNT laye s deco a ed wi h 600 Pd N ALD was in es iga ed be o e and a e he elec ochemical measu emen s by XPS. The su ey spec a (Figu e S4a) in bo h cases e eal he p esence o C, O, Ti, F and Pd. The C signal comes om he ad en i ious ca bon. The p esence o oxygen can be iden i ied om he Auge O KLL signal, since he O 1s has a s ong o e lapping wi h he Pd 3p 3/2 signal. Ti peaks a e due o he subs a e (TNT laye s), while F is a emnan om he Ti oil anodiza ion p ocess. In o de o e i y he chemical na u e o TiO 2 a e he ALD p ocess, addi ional high esolu ion XPS analysis was conduc ed o Pd/TNTs sample p oduced wi h 600c o Pd ALD p ocess (i.e. be o e any elec ochemical expe imen ). This sample spen he longes ime in he ALD educ i e a mosphe e. Figu e S4b shows Ti 2p high esolu ion spec um o he co esponding sample. The spec um e eals only he Ti 4+ s a e, since Ti 2p3/2 is a ~459 eV. Thus, i is clea ha no educ ion o Ti 4+ o Ti 3+ occu ed du ing he ALD p ocess. Fig. 4a exhibi s he elec oca aly ic ac i i y p o ile o Pd/Ti oils in elec oly e o 1 M KOH solu ion. The blank oil shows no esponse along he CV in he po en ial ange (0 o 1.2 V), indica ing no oxida ion e- ac ion occu s. Inc easing Pd N ALD om 150 o 600 enhanced he cu en densi y a lowe po en ials, showing sha p peak a a ound 0.1 V. This peak ep esen s he deso p ion o H on he Pd NPs su ace due o he elec oly e (1M KOH) en iched wi h dissocia ed hyd oxyl g oups. While i is well known ha he Pd su ace ge s g adually oxidized as he anodic scan mo es owa ds highe po en ial egion o E >0.7 V [30], he e e se scan shows a educ ion peak a a ound 0.7 V ep esen ing he deso p ion o oxygen ( educ ion o PdO o Pd), adso bed du ing he p e ious o wa d scan be ween 0.75 and 1.2 V. Fig. 4b depic s he CVs ob ained om he se o Pd/Ti oils es ed in 1 M KOH/CH 3 OH. Figu e 3. (a) XRD pa e ns o 5 µm hick Pd/TNT laye s deco a ed wi h N ALD =0, 150, 300, 450, and 600 Pd. b) Pd 3d XPS high esolu ion spec a o 600c Pd/TNT laye s be o e and a e ch onoampe ome ic (CA) measu emen s. c) A omic concen a ion o Pd deduced by XPS. B. Bawab e al. Elec ochimica Ac a 429 (2022) 141044 6 No iceable oxida ion peaks appea s a ing om Ti oils deco a ed wi h 300 Pd N ALD . The esul s also indica e ha inc easing Pd N ALD deposi ed on Ti oils leads o an inc ease in he me hanol oxida ion peak cu en densi y, and he e o e in he ca hodic scan he CO oxida ion peak cu - en densi y. The highes cu en densi y alue o 8.9 mA cm −2 co e- sponds o he Ti oils deco a ed wi h 450 Pd N ALD , while hose deco a ed wi h 300 and 600 Pd N ALD show compa a i ely lowe alues o 5.8 and 7.8 mA cm −2 a ~0.8 V (no ed om he hi d CV cycle). The elec oca aly ic ac i i y o Pd NPs on Ti oils in me hanolic KOH elec oly e shown in Fig. 4b ollows he end o anodic oxida ion o MeOH and ca hodic oxida ion o CO [31]. The ob ained CV scans a e explained by he ac ha du ing he anodic scan, he sample su ace is being ac i a ed wi hin a ce ain po en ial ange, a e which i becomes deac i a ed by oxide species (such as CO), a ached on Pd NPs su ace p e en ing u he elec o-oxida ion o me hanol. Oxida ion eac ion ini ia es a a ound 0.7 V and he esul ing cu en densi y inc eases o each he elec o-oxida ion limi a 0.8 V. A his poin (0.8 V), he ca aly ic ac i e si es o Pd NPs su ace we e poisoned due o adso p ion o CO in e media e o med du ing me hanol oxida ion, dec easing he cu en densi y un il he su ace is comple ely inac i a ed. Howe e , Figu e 4. CVs showing h ee consecu i e cycles o Pd/Ti oils (a, b) and Pd/TNT laye s (c, d) deco a ed wi h di e en N ALD (0, 150, 300, 350, 400, 450, and 600), eco ded in 1 M KOH (a, c) and me hanolic (1 M KOH +1 M CH 3 OH) elec oly e by applying a scanning a e o 10 mV s −1 . B. Bawab e al. Elec ochimica Ac a 429 (2022) 141044 7 eac i a ion o he Pd NPs su ace occu s du ing he e e se ca hodic scan wi hin a po en ial alue anging be ween 0.7 and 0.6 V, due o oxida ion o he adso bed CO molecules ( o CO 2 ) and educ ion o PdO o me allic Pd. The me allic Pd and Pd hyd oxides a e esponsible o he inc ease in he cu en densi y among samples o Pd/Ti oils. Along he po en ial inc ease in he anodic scan he numbe o neighbo ing OH g oups on Pd also inc eases. Thus, such inc emen o OH g oups a highe po en ials acili a es an addi i e e ec on he emo al o he CO molecules, adso bed du ing he anodic scan. Fig. 4c-d shows he elec oca aly ic pe o mance ob ained om Pd/ TNT laye s, which beha es di e en ly om Pd/Ti oils, when i comes o me hanol oxida ion. TNT laye s es ed in non-me hanolic elec oly e (Fig. 4c) show simila peaks compa ed wi h Ti oils. In he oxygen adso p ion ange (0.7 – 1.2 V), Pd-OH, PdO, and/o PdOx could be o med, while a deso p ion educ ion peak is mo e p onounced in Pd/ TNT laye deco a ed wi h 400, 450 and 600 Pd N ALD compa ed wi h Ti oils due o highe Pd loadings. Fu he mo e, Fig. 4d shows Pd/TNT laye s pe o mance in me hanolic KOH, showing cu en densi ies o 66.7, 64.8 and 62.6 mA cm −2 ob ained a 1.2 V o 400, 450 and 600 Pd N ALD espec i ely. The CVs show no isible anodic and ca hodic peaks, hus ep esen ing a ea u eless pola iza ion cu e wi h an onse po en- ial o 0.5 V. The TNT laye is an oxyphilic oxygen a oms p o ide . I appea s o be an e ec i e oxidize o mi iga e elec o-oxida ion o me hanol on he Pd/TNT laye su ace, ci cum en ing ei he CO poisoning o Pd NPs su ace o a oiding o ma ion o in e media e o ganic species. [8,23,32] Du ing he elec ode deac i a ion, obse ed o Pd/Ti oils, CO species, in addi ion o o he in e media es o med du ing he p ocess o me hanol elec o-oxida ion, a e belie ed o be he main elec ode poisoning species. As a ma e o ac , based on he p e ious li e a u e [33] CO is no he only sou ce o poisoning he ca alys su ace, and emo al o CO is a di usion con olled p ocess, which explains he slow deso p ion p ocess. The oxida ion o CO ads is conside ed as he a e de e mining s ep acco ding o he ollowing eac ion, and i is well known ha he comple e MOR can yield CO 2 as end p oduc : CH3OHads +4OH−→COads +4H2O+4e−(Eq. 1) COads +2OH−→CO2+H2O+2e−(Eq. 2) In a ypical anodic scan o MOR (Fig. 4b) he oxida ion s a s and ca ies on un il a ce ain po en ial whe e he adso bed OH g oups can no longe eac wi h he a ailable CO molecules adso bed on he su ace (CO ads ), leading o a cu en densi y d op. CO and OH g oups a e belie ed o be e ol ing du ing he same po en ial window. Howe e , he e ec o highe po en ial excels he ac i i y o OH g oups. To simpli y, CO bonding on he su ace can only lead o a loss o su ace ac i i y as explained be o e and shown in (Fig. 4b), while he CO oxida ion eac ion occu ing wi h he neighbo ing OH g oups, bonded in o he su ace o high su ace a ea TNTs, plays an impo an ole in clea ing CO molecules and he o he adso bed species. The ob ained ea u eless cu es (Fig. 4d) show no decline in he cu en densi y du ing consecu i e CVs wi hin he applied po en ial ange (0 o 1.2 V). In o de o s udy such e ec , he po en ial ange is spli in o wo pa s. A lowe po en ial egion below he peak po en ial alue a ound 0.8 V (Fig. 4b), and a highe egion abo e his alue. A he lowe po en ial egion, adso p ion o me hanol akes place, and Eq. (1) applies esul ing in CO adso bed on he su ace. Following, Eq. (2) ap- plies a highe po en ial, suppo ed by he oxophilic na u e o TiO 2 and i s elec on dono p ope ies, which enhance he CO ads oxida ion ki- ne ics enough o keep he CH 3 OH oxida ion wi hou su ace blockage by in e media es. Thus, CO ads oxida ion eac ion is no conside ed as he a e de e mining s ep anymo e wi h he Pd/TNT laye s. The elec ochemical su ace a ea (ECSA) was de e mined using he in eg a ed educ ion peak o PdO. The alue o cha ge o he educ ion o a PdO monolaye was aken om he li e a u e [34,35] wi h QM = 424 μ C/cm2. The ECSA alue was de e mined using he ollowing o mula. ECSA =Qin QM Since he alue o Q in is scan a e dependen , i is co ec o use di e en scan a es o de e mining he inal alue o cha ge in eg a ed om he educ ion peak. The ECSA o Pd/TNT laye s deco a ed wi h 450 Pd and 600 Pd N ALD we e calcula ed o be 176 cm 2 and 213 cm 2 , a highe as compa ed o 0.636 cm 2 ob ained as he co esponding geome ical a ea (de ined as he dimensional a ea exposed o he elec oly e, wi hou aking he su ace po osi y in o conside a ion). The ECSA alue ob ained o he TNT laye deco a ed wi h 600 Pd N ALD is abou 7 imes la ge han he ECSA alues epo ed in he li e a u e, which we e es ima ed o be 22.3, 29.6, and 7.1 cm 2 o Pd/TNT laye s (500, 700, and 900 Pd N ALD ) [2], and 14.2 cm 2 o palladium suppo ed TiO 2 nano ube a ay (Pd-TNTA) de eloped by elec ochemical milling and ace ing (ECMF) me hod [17]. Elec ochemical impedance spec oscopy (EIS) was used as a powe ul ool o s udy he elec on- ans e kine ics o he me hanol oxida ion eac ion. EIS measu emen s we e ca ied ou a a equency ange (10 −2 and 10 5 Hz), and an AC ampli ude o 10 mV a a po en ial o 0.8 V s RHE in 1M KOH/CH 3 OH elec oly e. In gene al, he cha ge ans e esis ance alue is ep esen ed by he diame e o he semici cle. A smalle diame e co esponds o a smalle cha ge ans e esis ance, which in u n ep esen s a high cha ge ans e a e p o ided he e al- ua ion pe o med o all he samples a he same po en ial. Fig. 5 ep- esen s he Nyquis plo s o Pd/TNT laye s deco a ed wi h di e en N ALD o Pd. The Nyquis plo s o Ti oils and a compa a i e assessmen o cha ge ans e esis ance alues o bo h oils and TNTs wi h Pd a e p o ided in Figs. S5 and S6. The dec ease in cha ge ans e esis ance o TNTs deco a ed wi h N ALD Pd is e iden and no signi ican di e ence among samples wi h 400, 450 and 600 N ALD was obse ed, which aligns wi h obse ed cu en densi ies om CV o he samples. In o de o e alua e he s abili y o Pd NPs in 1M KOH elec oly e wi hin he po en ial ange o 0 – 1.4V, 22 consecu i e CV cycles we e pe o med o TNTs deco a ed wi h Pd NPs using N ALD =600, as shown in Fig. 6. The esul ing CV cu es showed se e al meaning ul egions in he anodic as well as in he ca hodic scan, as desc ibed ahead. The lowe po en ial egion (1) co esponds o hyd ogen deso p ion o adso p ion in addi ion o K + ca ion species [36]. This p ocess akes place as a esul o a p e ious adso p ion p ocess happened du ing he e e se scan a po- en ial anges be ween (0 – 0.2V). The peak in ensi y inc ease wi h cycling could be due o accumula ion o he adso bed species a he su ace du ing cycling. In egion (2), he lowe cu en densi y co e- sponds o he double laye cha ge, bu he cu en densi y inc eases upon cycling. I is shown in e . [37] ha i is unlikely ha he ise o he anodic peak du ing cycling is ela ed o oxide o ma ion. A he same ime, he dec ease in oxygen adso p ion cu en densi y ( egion 3) may indica e he lowe quan i ies o he adso bed OH g oups on he su ace and PdO could be o med al e na i ely. The de ailed oxida ion p ocess is no ye ully unde s ood. The o med OH g oups eac wi h monoxides ob ained du ing dehyd ogena ion p ocess leading o a comple e eac- ion. Then he sligh inc ease in cu en densi y o he sha p ca hodic peak ( egion 4) ep esen s he educ ion o PdO in o Pd, whe e he in- ensi y inc eases wi h inc easing he palladium oxide on su ace. In o de o exploi he s abili y o Pd NPs on TNTs in 1M KOH +1M CH 3 OH elec oly e, 22 consecu i e CV cycles we e pe o med o TNTs deco a ed wi h Pd NPs using N ALD =450, wi hin he po en ial ange o 0 – 1.2V. The esul ing CV cu es shown in Figu e S7 p o e e y good s abili y o he sample es ed. In o de o gain u he insigh in o he s abili y o he Pd/Ti oils and Pd/TNT laye s´elec oca alys , ch onoampe ome ic (CA) measu e- men s we e ca ied ou o 2 hou s a 0.9 V. CA cu es ob ained o Pd/ TNT laye s a e shown in Fig. 7. CA cu es o Pd/Ti oils a e shown in Figu e S8. Pd/Ti oils show a d as ic dec ease in he cu en densi ies B. Bawab e al. Elec ochimica Ac a 429 (2022) 141044 8 du ing he CA analysis con i ming he e ec o CO poisoning ha led o a loss o ac i e si es esponsible o me hanol elec o-oxida ion. Whe eas he esul s ob ained om Pd/TNT laye s con i m he bene i s o noble me al - me al oxide suppo in e ac ion, by p o iding signi ican ly highe ole ance o CO poisoning. The CA esul s depic ela i ely s able cu en densi ies along he CA es o he Pd/TNT laye s deco a ed wi h 600 Pd N ALD , de eloping a cu en densi y o 28.5 mA cm −2 (Fig. 7). In con as , he Pd/TNT laye s deco a ed wi h 450, 400, 350, 300, and 150 Figu e 5. EIS Nyquis plo s o Pd/TNT laye s in me hanolic (1 M KOH +1 M CH 3 OH) elec oly e using di e en N ALD . Figu e 6. CV cu es (22 consecu i e cycles) ob ained in 1M KOH o 5µm TNTs deco a ed wi h Pd NPs using N ALD =600. B. Bawab e al. Elec ochimica Ac a 429 (2022) 141044 9 Pd N ALD show compa a i ely a highe cu en densi y d op (compa ed o he ini ial cu en densi y) a e 2h es , wi h cu en densi ies o 24.8, 16.7, 0.5, 1.07, and 0.07 mA cm −2 , espec i ely. In e es ingly, he d op in cu en densi ies was a enua ed o a highe Pd N ALD . Thus, he pe cen ages o cu en densi y loss we e 16.1%, 23.7%, 32.1%, 42.8%, 49%, and 75.8% o 600, 450, 400, 350, 300 and 150Pd N ALD , espec i ely. The e o e, he esul s indica e ha he Pd NPs size plays a signi ican ole in he elec oca aly ic pe o mance. Thus, he domi- nance o he OH co e age on small Pd NPs will dec ease he ca aly ic ac i e Pd su ace esponsible o me hanol adso p ion, leading o a highe d op in he cu en densi ies unde long e m pe o mance [38]. Hence, based on he esul s ob ained in his wo k, i is sugges ed ha he Figu e 7. Ch onoampe ome ic (CA) cu es demons a ing he s abili y o Pd/TNT laye s wi h di e en N ALD (150, 300, 350, 400, 450, and 600). CA cu es we e eco ded in 1M KOH +1M CH 3 OH a 0.9V RHE o 2 h. Table 1 O e iew o cu en densi ies ob ained om he published li e a u e and compa ed wi h densi y acqui ed in his wo k. All alues de e mined o calcula ed a 0.9V s RHE, i no deno ed o he wise. F om CV F om CA Subs a e Scan a e mV. s ¡1 Cu en densi y (mA cm −2 ) Onse po en ial A ea conside ed omcu en densi y (mA cm −2 ) @ ime@ V Re . E hanol oxida ion SnO 2 /Pd 500 cycles 25 1.19 ECSA -0.465 (ECSA) 0.4 @0s 0.19 @3500s [39] TiO 2 TNTs/Pd 500 cycles 25 0.63 ECSA -0.465 (ECSA) 0.2375 @0s 0.175 @3500s [2] Pd/TiO 2 C 50 18 0.424 Ch onopo en iome ic 3mA/cm 2 @[email p o ec ed] 3mA/cm 2 @28800s@ 0.72V [19] Me hanol oxida ion Smoo h P elec ode 50 3.84×10 −9 A 0.5 NA [40] Pd/C 20 3.1 0.6 NA [30] PdRh/C 20 5 0.6 NA Pd/TiO 2 NTs in H 2 SO 4 50 8.66 A 0.436 NA [41] 60-65% po ous Pd 25 710 0.15 NA [10] Pd/TiO 2 -C 50 2.24 (ECSA) 0.44 (ECSA) 1.83 @7200s [42] TiO 2 /Pd 450 cycles 10 32 ~0.5 (Geome ic) 24.8 @7200sec @0.9V This wo k B. Bawab e al.