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Tomographic Heating Holder for In Situ TEM: Study of Pt/C and PtPd/Al2O3 Catalysts as a Function of Temperature

Abstract

A tomographic heating holder for transmission electron microscopy that can be used to study supported catalysts at temperatures of up to ~1,500°C is described. The specimen is placed in direct thermal contact with a tungsten filament that is oriented perpendicular to the axis of the holder without using a support film, allowing tomographic image acquisition at high specimen tilt angles with minimum optical shadowing. We use the holder to illustrate the evolution of the active phases of Pt nanoparticles on carbon black and PtPd nanoparticles on ¿-alumina with temperature. Particle size distributions and changes in active surface area are quantified from tilt series of images acquired after subjecting the specimens to increasing temperatures. The porosity of the alumina support and the sintering mechanisms of the catalysts are shown to depend on distance from the heating filament.

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Tomographic Heating Holder for In Situ TEM: Study of Pt/C and PtPd/Al2O3 Catalysts as a Function of Temperature

Author: Cervera Gontard, Lionel; Dunin Borkowski, Rafal E.; Fernández Camacho, Asunción; Ozkaya, Dogan; Kasamac, Takeshi
Publisher: Cambridge University Press
Year: 2014
DOI: 10.1017/S1431927614000373
Source: https://idus.us.es/bitstreams/b9b72200-db1c-4e62-b708-1c98fd08c7e9/download
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Tomog aphichea ingholde  o insi uTEM:
S udyo P /CandP Pd/Al2O3ca alys s
asa unc iono  empe a u e
Lionel C. Gon a d,1,* Ra al E. Dunin-Bo kowski,2 Asunción Fe nández,1
Dogan Ozkaya,3 and Takeshi Kasama4
1 Ins i u o de Ciencia de Ma e iales de Se illa (CSIC), 41092, Se illa, Spain
2 E ns Ruska-Cen e o Mic oscopy and Spec oscopy wi h Elec ons (ER-C) and Pe e
G ünbe g Ins i u e (PGI), Fo schungszen um Jülich, D-52425 Jülich, Ge many
3 Johnson Ma hey Technology Cen e, Bloun ’s Cou , Sonning Common, Reading
RG4 9NH, UK
4 Cen e o Elec on Nanoscopy, Technical Uni e si y o Denma k, DK-2800
Kgs. Lyngby, Denma k
Abs ac : A omog aphic hea ing holde o ansmission elec on mic oscopy ha can
be used o s udy suppo ed ca alys s a empe a u es o up o ~1500 °C is desc ibed. The
specimen is placed in di ec he mal con ac wi h a ungs en ilamen ha is o ien ed
pe pendicula o he axis o he holde wi hou using a suppo ilm, allowing
omog aphic image acquisi ion a high specimen il angles wi h minimum op ical
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shadowing. We use he holde o illus a e he e olu ion o he ac i e phases o P
nanopa icles on ca bon black and P Pd nanopa icles on γ-alumina wi h empe a u e.
Pa icle size dis ibu ions and changes in ac i e su ace a ea a e quan i ied om il
se ies o images acqui ed a e subjec ing he specimens o inc easing empe a u es. The
po osi y o he alumina suppo and he sin e ing mechanisms o he ca alys s a e shown
o depend on dis ance om he hea ing ilamen .
Keywo ds: in si u TEM, TEM specimen holde , pa icle g ow h, he e ogeneous
ca alysis, pla inum, ca bon black, pla inum-palladium, alumina
* email: lionel.ce e [email protected] . Phone: +34 954489576
1. In oduc ion
When s udying he e ogeneous ca alys s, which equen ly comp ise me al nanopa icles
on ca bon black o an oxide suppo , an impo an goal is o obse e he e olu ion o he
ac i e phase wi h empe a u e in he p esence o eac an gases. Ca aly ic ea men can
lead o changes in he su ace a ea o he suppo ed me al pa icles and hence ca aly ic
ac i i y due o p ocesses such as sin e ing. In o de o unde s and and con ol ca alys
p oduc ion, i is necessa y o s udy how he dispe sion and mo phology o bo h he
nanopa icles and he suppo depend on eac ion condi ions. Al hough phase diag ams
o small me al pa icles ha e been p oposed heo e ically based on he modynamics
(Ajayan & Ma ks, 1988), hey a e incapable o p edic ing nanopa icle shapes ha esul
om pu ely kine ic conside a ions. Recen ly, Ba na d e al. (2009) p oposed a
quan i a i e phase map o gold nanopa icles based on ab ini io calcula ions. Howe e ,
a u he complica ion is ha such he modynamic models do no ake in o accoun he
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ole o he suppo , which de e mines he s eng h o a achmen and he eby pa icle
mobili y and also he posibili y o phase ans o ma ions (Be e al., 1974; Taus e ,
1987; Sepúl eda e al., 1998; Gónzalez e al., 2009).
In si u ansmission elec on mic oscopy (TEM) e e s o echniques ha allow di ec
obse a ion o dynamic p ope ies a he nanoscale h ough imaging, spec oscopy o
di ac ion. Such echniques can be used o unde s and he kine ics o phase ansi ions
in he e ogeneous ca alys s and he impo ance o sin e ing mechanisms (Bena idez e
al., 2012; Hansen e al, 2013). Possible app oaches in ol e injec ing gas di ec ly in o an
en i onmen al TEM (ETEM) (Hansen e al., 2002) and/ o using dedica ed sample
holde s ha con ain ho s ages, gas o liquid cells, elec ical con ac s, ibe op ics and
lase s o illumina ing o hea ing he specimen while images a e acqui ed wi h a omic
spa ial esolu ion (Kamino e al., 2005; C eeme e al., 2010; Ca alca e al., 2012;
Me ha een e al., 2013). In si u expe imen s ha ha e made use o such ins umen a ion
a e nowadays common. Mos ecen esul s ha e included s udies o he ole o
p omo e s in Ru-based he e ogeneous ca alys s (Hansen e al., 2002), he oxida ion o
In, he eoxida ion o Si and he o ma ion o g aphene on MgO-suppo ed P
nanopa icles (Kamino e al., 2005; Peng e al., 2012), as well as pho odeg ada ion o
Cu2O and pho odeposi ion o P on a GaN:ZnO pho oca alys (Ca alca e al., 2012).
He e, we desc ibe a TEM specimen holde ha p o ides di ec con ac be ween a
specimen and a ilamen ha has a small he mal mass. The ilamen eaches a
empe a u e ha depends on he cu en lowing h ough i . The e is hen no need o use
a suppo ilm, which can p e en e ec i e he mal ans e and deg ade image
esolu ion. Kamino e al. (2005) de eloped a simila specimen holde , which was
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equipped wi h a longi udinal ungs en wi e aligned pa allel o he o a ion axis o he
holde . In con as , he ilamen in ou holde is o ien ed pe pendicula o he holde axis
and has a na ow design, pe mi ing acquisi ion o images a high specimen il angles
(± 80°) wi h minimal op ical shadowing. This capabili y allows elec on omog aphy o
be used o analyse he e ogenous ca alys s in h ee dimensions in combina ion wi h high
empe a u e hea ing expe imen s.
We demons a e he unc ionali y o he holde by imaging he g ow h o P ca alys
nanopa icles on ca bon black in si u in he TEM as a unc ion o empe a u e and by
measu ing he esul ing changes in pa icle size dis ibu ion (PSD) and su ace a ea o
he ac i e phase. We also s udy he o ma ion o bime allic P Pd pa icles on γ-Al2O3
and use high-angle annula da k- ield (HAADF) scanning TEM (STEM) (Gon a d e al.,
2008, 2009) o ob ain h ee-dimensional in o ma ion abou he po osi y o he suppo
a e successi e hea ea men s.
2. Ma e ials and Me hods
2.1. Tomog aphic hea ing holde
The omog aphic specimen holde ha we desc ibe he e con ains a p e-wound ungs en
ilamen aken om a ligh bulb (Fig. 1). We moun he ilamen in a emo able
ca idge, which is clamped on o wo elec ical con ac pads in a specimen holde om
E.A. Fischione Ins umen s, Inc. (Expo , PA). We glue he ilamen on o wo pieces o
a coppe g id using sil e epoxy and place a hin elec ically-insula ing shee o mica
be ween he coppe and he clamp.
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Samples can be deposi ed di ec ly on o he wi e, ei he in he o m o a d y powde o
om solu ion. The ends o he wi e, which has an elec ical esis ance o app oxima ely
5 Ω and can be eplaced be ween expe imen s i equi ed, can be accessed elec ically
om ou side he mic oscope. The wi e empe a u e, which can be calib a ed using an
op ical py ome e be o e inse ion in o he TEM column, p o ed o be highly
ep oducible be ween di e en ilamen s. Fo example, a empe a u e o ~1000 °C was
achie ed by passing a cu en o ~90 mA h ough he wi e. When ope a ed in high
acuum, he ilamen s we e ypically ound o ail a cu en s o ~220 mA,
co esponding o a empe a u e o jus o e 1500 °C. Tungs en wi e has high he mo-
mechanical s i ness and he e o e does no sag signi ican ly a high empe a u e, as
well as a high mel ing poin o 3422 °C and a low apou p essu e. Expe imen s we e
pe o med wi h ilamen s ope a ed o up o 12 hou s a cu en s o up o 150 mA
(co esponding o a empe a u e o ~1300 °C) wi h no signi ican signs o ungs en
e apo a ion.
2.2. P suppo ed on ca bon black
P pa icles wi h high dispe sions (> 75 m2 g-1), which we e suppo ed on mesopo ous
high-su ace-a ea ca bon blacks (Vulcan XC-72R) P (19.1 w %) and had been educed
in a N2 a mosphe e a 900 °C, we e p o ided by he Johnson Ma hey Technology
Cen e in he o m o a d y powde (Ralph & Hoga h, 2002; Ozkaya e al., 2003). The
samples a e used in p o on exchange memb ane uel cells, which equi e high loadings
o elec oca alys s. A small amoun o powde ha had been s o ed in ai was placed
di ec ly on o he ilamen o he hea ing holde , inse ed in o a Philips CM300 TEM

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ope a ed a 300 keV and ehea ed in si u by passing a cu en h ough he ilamen . The
empe a u e was g adually inc eased om oom empe a u e o 975 °C in s eps o ei he
25 o 50 °C, allowing he specimen o s abilise be ween each s ep be o e acqui ing a
b igh - ield (BF) TEM image. Measu emen s o PSDs om he eco ded images we e
ob ained using dedica ed image p ocessing so wa e based on adap i e segmen a ion
(Gon a d e al., 2011).
2.3. P Pd suppo ed on alumina
P Pd nanopa icle o ma ion was s udied in si u in he TEM, s a ing om a d y powde
o he p ecu so (P (HN3)4)2 Pd2(EDTA) 2.5 w . % on γ-Al2O3 (SFC-140). γ-Al2O3 is a
me as able poly ype o Al2O3, which is used ex ensi ely as a ca aly ic suppo ma e ial
because o i s high po osi y and la ge su ace a ea. In he p esen specimen, he
o ma ion o P Pd pa icles was expec ed o occu a empe a u es o be ween 600 and
850 °C. The expe imen al p ocedu e was as ollows: (1) The powde was placed on o
he ilamen o he hea ing holde and inse ed in o a Tecnai F20 TEM. A egion o he
specimen ha could be il ed o high angles wi hou shadowing was iden i ied. A il
se ies o HAADF STEM images o he egion o in e es was acqui ed a low
magni ica ion o e a specimen il ange o -52° o +42° using a 4° il inc emen ; (2)
In si u hea ing was pe o med in a Philips CM300 TEM, wi h he empe a u e o he
ilamen inc eased om 500 o 850 °C, allowing he specimen o equilib a e be ween
s eps. BF TEM images we e acqui ed om he same a ea a high magni ica ion a each
empe a u e; (3) The specimen was allowed o cool o oom empe a u e, he holde was
einse ed in o he Tecnai F20 TEM and a new il se ies o HAADF STEM images was
acqui ed om he same a ea. Alignmen and omog aphic econs uc ion using he
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simul aneous i e a i e econs uc ion echnique (SIRT) we e ca ied ou in Inspec 3D
so wa e (15-20 i e a ions). Vol ex isualiza ion o he inal econs uc ions was
pe o med using Ami a V2.3 so wa e. PSDs we e measu ed using image p ocessing
so wa e based on adap i e segmen a ion (Gon a d e al., 2011).
3. Resul s
3.1.
Sin e ing o P pa icles on C
Figu e 2 shows a se ies o BF TEM images, which illus a e he sin e ing o P pa icles
suppo ed on ca bon black du ing in si u hea ing a inc easing empe a u e. E en hough
he specimen had al eady been educed in an ine a mosphe e a high empe a u e,
Fig. 2 shows ha e-sin e ing occu s du ing hea ing in high acuum, beginning a
~550 °C, accele a ing be ween 650 and 850 °C and appea ing o s op a 850 °C.
Face ing o he pa icles can hen be seen, pa icula ly o se e al la ge pa icles. The
shape o he C suppo does no change app eciably du ing sin e ing, al hough i o a es
and ansla es wi hin he ield-o - iew. In Figs. 3A and B, ci cles and a ows a e used o
highligh di e ences be ween he same pa icles iewed a 500 and 900 °C.
Figu e 4 shows PSDs o he nanopa icles measu ed om selec ed images in Fig. 2.
Se e al s a is ical pa ame e s a e plo ed, including mean size, s anda d de ia ion and
maximum size, o i e selec ed empe a u es (500, 650, 725, 875 and 950 °C). The
mean pa icle size was used o es ima e he ac i e su ace a ea . This is an
impo an quan i y in ca alysis, as i desc ibes he su ace a ea o he ac i e phase ha is
exposed o gases and can be used o unde s and ca alys deac i a ion. We made wo
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app oxima ions: (1) Tha he con ac su ace o he nanopa icles wi h he suppo is
exposed o he gas; (2) ha he pa icles ha e sphe ical shapes wi h adii . The su ace
a ea is hen simply gi en by he exp ession
 


 4
∙4
3

 3
∙


whe e  is he numbe o pa icles,  and  a e he su ace a ea and mass o pa icle 
and  is he densi y o P (i.e., 21.450 kg m
⁄). Figu e 5 shows measu emen s and he
e olu ion o  wi h empe a u e. The a e o loss o ac i e a ea calcula ed om he
slope o a linea i , i.e.,  
⁄910mkg
⁄C.
3.2. Fo ma ion o P -Pd pa icles
Figu e 6A shows TEM images o he p ecu so (P (HN3)4)2 Pd2(EDTA) 2.5 w . % on γ-
Al2O3 (SFC-140) eco ded a oom empe a u e. Figu e 6B shows an image o he same
egion o he specimen eco ded a e hea ing a 850 °C. The images on he le side o
he igu e a e HAADF STEM images, in which he local in ensi y is sensi i e o a omic
numbe (b igh e egions co espond o pa icles). The BF TEM images shown in he
igh column o Fig. 6 we e acqui ed om he egions ma ked using ec angles in he
le column. The images show ha he P Pd pa icles g ow a high empe a u e and ha
he γ-alumina suppo inc easse in po osi y. Figu e 6C shows he measu ed PSDs o he
P Pd nanopa icles.
Figu e 7 shows indi idual HAADF STEM images eco ded a di e en specimen il
angles om he same a ea o he alumina sample be o e and a e hea ing, aken om a
il se ies o images used o elec on omog aphy. Figu e 8A shows a ol ex
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isualisa ion o he h ee-dimensional econs uc ion o his egion o he specimen a e
hea ing, while Fig. 8B shows an o hoslice gene a ed om he econs uc ed olume.
Al hough he il s ep o 4° used o acquisi ion o he il se ies is ela i ely la ge and
educes he spa ial esolu ion o he econs uc ed olume, his alue was chosen o
minimise he o al elec on dose on he specimen. Fo example, i has been obse ed on
samples o Pd suppo ed on alumina ha unde elec on i adia ion Al2O3 can be
educed and a me as able in e me allic compound o Al2Pd can o m (Kamino e al.,
1992). In he p esen expe imen s, he il ange used was smalle han he maximum
ange ha he holde allows (± 80°), which also a ec s he quali y o he inal
econs uc ion, in pa icula in he z di ec ion.
4. Discussion
The esul s shown in Figs. 1 o 8 can be used o discuss he kine ic ou e ha ca alys
nanopa icles ollow when hey g ow on a speci ic suppo and o de e mine he ela i e
impo ance o di e en sin e ing mechanisms (Bena idez e al., 2012; Hansen e al.,
2013). Th ee possible sin e ing mechanisms a e: (1) Coalescence, in ol ing mo ion o
he pa icles o e he suppo and usion (Ruckens ein & Lee, 1984). In gene al, a
empe a u es o 0.5 × he mel ing poin , me allic pa icles a e expec ed o be in a quasi-
mel ed s a e (con inuously luc ua ing be ween di e en s uc u es), which a ou s
coalescence (Ajayan & Ma ks, 1988; Ba na d e al., 2009). (2) Os wald ipening,
in ol ing he mig a ion o indi idual a oms om he pa icles on o he suppo , ac oss
he suppo and on o o he pa icles (Simonsen e al., 2010). Os wald ipening is
s ongly dependen on a omic di usi i y (Linde o h e al., 1997; Ho ch e al., 1999) and
can also happen in ace ed pa icles in he o m o inhibi ed nuclea ion, which a ises
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
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Figu e 1. (A) Modi ied TEM specimen holde wi h ungs en hea ing ilamen o ien ed
pe pendicula o he holde axis. The numbe s co espond o (1) he clamp; (2) an
insula ing mica shee ; (3) Cu elec ic con ac s; (4) sil e epoxy esin. (B-D) Th ee
magni ied images o he ilamen . The la ge a ow in (D) indica es an agg ega e o he
deposi ed specimen.
21
Figu e 2. Se ies o BF TEM images showing sin e ing o P nanopa icles on a ca bon
black suppo as a unc ion o empe a u e be ween 500 and 975 °C. The specimen was
deposi ed di ec ly on o he ungs en ilamen in he modi ied side-en y TEM specimen
holde shown in Fig. 1. The da k con as a he bo om le co ne o he images
acqui ed a 925 and 950 °C a ises om he closes pa o he ilamen o he egion o
in e es .

22
Figu e 3. (A) and (B) De ail ex ac ed om he BF TEM images shown in Fig. 2,
illus a ing he coalescence o P nanopa icles be ween indica ed specimen
empe a u es o 500 and 975 °C. Red ci cles in bo h images show he ini ial and inal
con igu a ions o selec ed P pa icles ha ha e coalesced. Whi e a ows indica e
pa icles ha emained s ongly a ached o he suppo and expe ienced smalle changes
in hei size. (C) De ail o he a achemen o a ace ed P nanopa icle o he suppo .
(D) Model showing c ys alline ace s and possible P (111) con ac plane o a P
nanopa icle such as ha shown in (E). (E) Expe imen al high- esolu ion TEM image o
one P pa icle on g aphi ised ca bon ( eco ded om a simila specimen) showing
a omic de ec s p esen a he su aces (a ows 1 and 2) (Gon a d e al., 2007).
23
Figu e 4. Top: Pa icle size dis ibu ions (PSDs) o he P pa icles shown in Figs. 2 and
3 measu ed a i e selec ed empe a u es be ween 650 and 950 °C i ed wi h logno mal
cu es. Bo om: Dependence o se e al s a is ical pa ame e s (mean size, s anda d
de ia ion and maximum size) on empe a u e. The alues inc ease wi h empe a u e
because o pa icle sin e ing.
24
Figu e 5. Ac i e su ace a ea o he P pa icles desc ibed in Figs. 2-4, measu ed a i e
selec ed empe a u es be ween 650 and 950 °C (see ex o de ails). Al hough he
e olu ion o su ace a ea is no linea we used he slope o a linea app oxima ion as an
es ima e o he a e o loss o ac i e su ace a ea.
25
Figu e 6. (A, B) ADF STEM images (le ) and BF TEM images ( igh ) o
(P (HN3)4)2Pd2(EDTA) 2.5 w % on γ-Al2O3 acqui ed (A) a oom empe a u e (using
he Tecnai F20) and (B) a e inc easing he empe a u e o 850 °C (using he Philips
CM300) in high acuum condi ions. The P Pd pa icle size and he po osi y o he
alumina di e be ween he ma ked zones. (C) PSDs measu ed om zones 2 and 3 and
om zone 3 alone, illus a ing he o ma ion o wo amilies o pa icles wi h di e en
a e age sizes.