scieee Science in your language
[en] (orig)

Preprint of "Tracking Structural Evolution in Lithium-ion Batteries via In-Operando Scanning Electron Microscopy"

Author: Hálová, Hana; Klvac, Ondrej; Trochta, David; Paušová, Šárka; Bouzek, Karel
Publisher: Zenodo
DOI: 10.5281/zenodo.15282021
Source: https://zenodo.org/records/15282021/files/VZ1_030_021_VUT_M_0670_v1.pdf
T acking S uc u al E olu ion in Li hium-ion Ba e ies ia In-Ope ando Scanning
Elec on Mic oscopy
Ondřej Kl ača,b*, Da id T och aa,b, Libo No áka, Pe e P iecela, Manuel Bo nhö a, and
Tomáš Kazdab, Zhao Liua*
a The mo Fishe Scien i ic, 5350 NE Dawson C eek D , Hillsbo o, OR 97124, USA
b Depa men o Elec ical and Elec onic Technology, Facul y o Elec ical Enginee ing
and Communica ion, B no Uni e si y o Technology, Technická 10, 616 00 B no, Czech
Republic
* Co esponding au ho
Abs ac :
The s udy o li hium-ion cells is pa amoun o op imizing hei pe o mance, sa e y, and
longe i y, which a e c i ical o applica ions such as po able elec onics, elec ic ehicles,
and enewable ene gy s o age sys ems. Scanning Elec on Mic oscopy (SEM) is
ins umen al in he examina ion o li hium-ion ba e ies, o e ing high- esolu ion imaging
and de ailed insigh s in o he mic os uc u e and mo phology o he cells. In-si u/ope ando
analyses a e in aluable as hey p o ide p ecise desc ip ions o he dynamic phenomena
and hei empo al e olu ion wi hin he ba e y. Howe e , he applica ion o SEM o in-
si u/ope ando analyses is hinde ed by he challenging p epa a ion o samples ha can
unc ion wi hin he SEM en i onmen . The e o e, we in oduces a uni e sally applicable
me hodology ha in eg a es sample p epa a ion using a b oad ion beam polishe wi h he
ans e o samples o he SEM in a specially designed holde unde an ine a mosphe e.
The e icacy o his sys em and wo k low is demons a ed on Nickel Manganese Cobal
Oxide (NMC) and Li hium Ti ana e Oxide (LTO) ba e y cells, e ealing g ain c acking and
expansion, as well as elec ode expansion and con ac ion. Addi ionally, a g aphi e-me al
li hium sys em is analyzed, whe e expansion and c acking o g aphi e g ains we e
obse ed. The s udy delinea es a p ocedu e enabling he in es iga ion o submic on
changes a he g anula le el and a he scale o en i e elec odes o la ge cell
componen s, applicable ac oss a ious chemis ies. We posi ha his wo k p o ides
signi ican insigh s o bo h undamen al esea ch o elec oac i e ma e ials and he
op imiza ion o he manu ac u ing p ocesses o comple e cells.
Keywo ds:
Li-ion ba e ies, elec ochemical cycling, SEM, BIB, in-si u, ope ando, s uc u al e olu ion
Highligh s:
• In eg a ion o b oad ion beam polishe and ope ando SEM
• Ope ando SEM analysis o c oss-sec ional elec ode ma e ials
• Examina ion o submic on and whole-cell changes
1. In oduc ion
Wi h ad ancemen s in he echnology ield, deca boniza ion e o s, and ecological
demands, he need o ad anced elec ochemical powe sou ces is inc easing. Howe e ,
la ge-scale p oduc ion aces challenges connec ed wi h limi ed amoun o aw ma e ials,
ising cos s, and en i onmen al impac s. Resea ch in his ield ocuses on enhancing cell
capaci y, li espan, and possible usage o elec oac i e ma e ials wi h a lowe
en i onmen al bu den.
Ope ando echniques o e eal- ime insigh s in o he kine ics o p ocesses and
mechanisms occu ing wi hin a ba e y du ing ope a ion. Unlike ex-si u o pos -mo em
me hods, hese echniques enable he p ecise iden i ica ion o when a phenomenon
occu s, leading o a clea e unde s anding o i s unde lying cause. A a ie y o ope ando
echniques a e a ailable, each sui ed o di e en ypes o analysis.[1][2][3][4]
X- ay echniques, such as compu ed omog aphy (CT)
[5][6][7][8][9][10][11][12][13][14][15], a e widely used in ope ando s udies o li hium-ion
ba e ies, enabling non-des uc i e 3D analysis du ing ope a ion. These me hods allow
da a collec ion ac oss a ious scales, om he en i e cell down o mic os uc u al de ails,
p o iding aluable insigh s in o elec ode aging and associa ed mo phological changes.
Howe e , a key d awback o CT analysis is i s lowe spa ial esolu ion compa ed o
elec on mic oscopy, as well as he ex ended ime equi ed o comple e each scan. To
o e come he esolu ion limi a ions o CT, X- ay di ac ion (XRD)
[16][17][18][19][20][21][22] can be employed. Unlike CT, XRD o e s esolu ion a he
in e -a omic scale, hough i s di ac ion da a s ill o igina es om a la ge sample egion.
In compa ison o X- ay echniques, elec on mic oscopy allows in es iga ion o he
mic os uc u e down o he le el o indi idual a oms. Toge he wi h complemen a y
me hods such as ene gy-dispe si e X- ay spec oscopy (EDS), elec on backsca e
di ac ion (EBSD) and ocused ion beam (FIB) ha can be used o si e-speci ic sample
p epa a ion, he elec on mic oscopy can be used o in es iga e many o he impo an
phenomena in ba e y beha iou such as solid elec oly e in e phase (SEI) o ma ion, Li
pla ing, phase changes, o o ma ion o de ec s in he elec odes[1][2].
T ansmission elec on mic oscopy (TEM) p o ides a omic-scale esolu ion, enabling
de ailed insigh s in o elec ochemical p ocesses. Howe e , i s applica ion is limi ed by
challenging sample p epa a ion and he small olume o ma e ial ha can be analyzed.
As a esul , TEM s udies a e o en es ic ed o model sys ems, such as minia u ized
ba e y se ups o hal -cells c ea ed on dedica ed TEM biasing holde s [23][24][25].
Addi ionally, TEM s udies may be a ec ed by adia ion damage and local sample
o e hea ing. Despi e hese challenges, TEM emains a powe ul ool o in es iga ing
elec ochemical p ocesses a a undamen al le el, making i well-sui ed o basic
esea ch.[26][27][28][29][30][31][32]
The la ge specimen chambe o a Scanning Elec on Mic oscope o e s he possibili y o
ope ando s udies o whole ba e ies a he cos o lowe image esolu ion compa ed o
TEM, s ill eaching spa ial esolu ion o uni s o nanome e s on sample su ace. A he
same ime SEM allows us o moni o a eal-size ba e y in la ge-scale, cap u ing s uc u al
changes in all he pa s and in e aces. SEM ope ando s udies can be applied o ba e ies
a di e en le els o de elopmen , including quali y con ol o samples esul ing om he
manu ac u ing p ocess. [33]
Fo scanning elec on mic oscopy (SEM) imaging, he ba e y mus be pa ially opened
on one side o allow elec on access o he su ace o in e es . O e he pas decades,
a ious app oaches ha e been explo ed o achie e his geome y [25][34]. Addi ionally,
since he ba e y is exposed o he acuum o he SEM chambe , a acuum-compa ible
elec oly e is equi ed—one ha emains s able and does no e apo a e a p essu es as
low as 10-6 Pa.
One o he ea lies ope ando SEM expe imen s was conduc ed by Baud y in 1988 [35],
u ilizing a solid-s a e elec oly e. Since hen, a ious acuum-compa ible solid-s a e
elec oly es ha e been employed in subsequen ope ando SEM s udies
[35][36][37][38][39][40][41]. The lowe ionic conduc i i y o solid-s a e elec oly es can be
mi iga ed by hea ing he sample wi hin he SEM chambe [38][41][37][35]. Addi ionally,
he design o he SEM holde mus accoun o he comp ession o he solid-s a e ba e y
bo h du ing ope ando analysis and h oughou he ans e p ocess. Depending on he
ype and size o he solid-s a e ba e y, his can esul in high o ces o be handled by he
SEM biasing holde .
Va ious ypes o ionic liquids wi h low apo p essu e a e commonly used as elec oly es
in SEM ope ando s udies [42][43][44][45][46][47][48][49][50][51][52]. Howe e , eplacing
a con en ional elec oly e wi h an ionic liquid can al e ce ain ba e y p ope ies. Fo
ins ance, he composi ion o he solid elec oly e in e phase (SEI) laye may di e due o
he absence o o ganic componen s [53].
A cooled hyb id polyme -based elec oly e can also be used in SEM s udies [54]. When
employing an elec oly e wi h a apo p essu e exceeding he SEM acuum h eshold is
una oidable, encapsula ion wi hin an elec on- anspa en memb ane can p e en
e apo a ion. Silicon ni ide windows, ypically se e al ens o nanome e s hick, a e
commonly used o his pu pose[55]. Al e na i ely, sligh e apo a ion o a con en ional
elec oly e can be managed wi hou ull encapsula ion by u ilizing en i onmen al SEM
(ESEM) mode, whe e he chambe p essu e is main ained a se e al hund ed pascals
[56]. Howe e , bo h he memb ane encapsula ion and ESEM app oaches esul in
educed SEM esolu ion due o elec on sca e ing wi hin he memb ane, gas, o he
elec oly e laye ha may o m on he ba e y su ace.
In a quasi-in-si u app oach, he ba e y is cycled unde s anda d high-p essu e condi ions
and subsequen ly exposed o he elec on beam o imaging a selec ed s a es o he
cha ge-discha ge cycles [57]. Howe e , his me hod necessi a es epea ed ba e y
disassembly and eassembly, which can in oduce ep oducibili y challenges.
Fo di ec SEM imaging o he ba e y su ace, he ba e y can be opened om he side
o enable plana imaging o one elec ode. Al e na i ely, a pe pendicula c oss-sec ion
can be p epa ed, allowing SEM imaging o all in e nal in e aces wi hin he ba e y.
In a plana geome y ha enables imaging o he ou e su ace o one elec ode, an
elec on beam- anspa en cu en collec o is ypically used o allow SEM imaging o he
elec ochemically ac i e ma e ial h ough he modi ied collec o . This is mos commonly
achie ed by deposi ing he ac i e ma e ial on o a me al g id [56][42][43][44][46][48][52] o
by c ea ing a small hole in a me al oil se ing as he collec o [36]. Howe e , in his
con igu a ion, SEM imaging is limi ed o he ou e su ace o one elec ode and may no
accu a ely ep esen bulk beha io . Fo ins ance, i does no allow o he assessmen o
a ia ions in li hia ion dep h as a unc ion o dis ance om he coun e elec ode.
Fo he c oss-sec ional geome y p esen ed in his s udy, ca e ul su ace p epa a ion is
essen ial o p e en a i icial ea u es in SEM images caused by su ace opog aphy. The
ba e y can be opened and polished using a ious me hods, wi h mechanical cu ing
commonly employed as an ini ial s ep [54][37]. To enhance su ace quali y a e ough
cu ing, ion beam polishing echniques—such as b oad ion beam (BIB) polishing o FIB
milling in a FIB-SEM sys em—a e ypically used. Al e na i ely, c yomic o omy [47][41] o
lase milling [58] can be u ilized o c oss-sec ion p epa a ion. C oss-sec ioning mus be
pe o med ca e ully o a oid sho -ci cui ing o mechanically damaging he ba e y.
Addi ionally, special a en ion should be gi en o p e en ing he de achmen o indi idual
pa icles, pa icula ly om he elec ode laye s, du ing he cu ing and polishing p ocess.
FIB echnology can also be u ilized o addi ional plana - iew analysis [42][49][40], such
as cu ing h ough li hium dend i es o med du ing ope ando expe imen s in a FIB-SEM
sys em [43]. A speci ic case is he usage o he FIB oge he wi h a mic omanipula o . The
mic omanipula o can se e as a cu en collec o o small amoun s o elec oac i e
ma e ial ixed mechanically and elec ically by FIB-assis ed deposi ion o conduc i e
ma e ials [50][51]. In his case, a e y small amoun o ma e ial is su icien o
cha ac e iza ion, and i is assu ed ha measu ed elec ochemical da a co esponds o he
in es iga ed a ea. Howe e , his single a ea may no always show he same beha io o
a ious easons. Fo example, he cycling cu en s o such a sys em a e e y small, which
ca ies he isk o da a dis o ion by elec omagne ic in e e ence [59].
BIB polishing enables he p epa a ion o c oss-sec ions o en i e elec odes o e en ull
ba e y cells in a ela i ely sho ime. Compa ed o mechanical me hods, BIB polishing
in oduces minimal a i ac s; o ins ance, cu aining a i ac s can be signi ican ly educed

by ocking he sample du ing he milling p ocess [60][33].
We p opose a wo k low o ope ando ba e y cha ac e iza ion in SEM ha combines he
ad an ages o he p e iously discussed app oaches. This me hod p o ides a obus
es ing en i onmen , ensu ing epea able esul s while minimizing he ime and e o
equi ed o ba e y sample p epa a ion p io o SEM analysis. The c oss-sec ional iew
is achie ed by placing he ba e y in a biasing holde wi hin he SEM. The sample su ace
is p epa ed using a b oad ion beam polishe [61] o ensu e smoo h c oss-sec ions. To
main ain sample in eg i y, all ans e s eps—be ween he glo e box and he CleanMill
polishe , as well as be ween he glo e box and he SEM—a e acili a ed by he
CleanConnec (CC) ans e de ice [62]. The wo k low is demons a ed on an examples
o li hium nickel manganese cobal oxide (NMC) – li hium- i ana e oxide (LTO) and
g aphi e – me allic li hium sys ems wi h a acuum compa ible ionic liquid elec oly e and
can be applied o a ious acuum compa ible ba e y ma e ials.
Mo eo e , apa om ex-si u echniques ypically analyzing p is ine and cycled elec odes
sepa a ely (Figu e 1a), ou echnique can examine he same loca ion con inuously,
p o iding a mo e consis en and de ailed obse a ion o he p ocesses (Figu e 1a).
Da a pos -p ocessing co ela ing he SEM image in o ma ion wi h ba e y cha ge s a e in
ime allows o sys ema ic cha ac e iza ion and di ec compa ison o indi idual ba e y
samples.
Figu e 1: Compa ison o da a ob ained du ing ex-si u (a) and in-si u (b) analysis. Ex-si u SEM analysis o NMC ca hode
c oss-sec ion, p is ine and cycled elec ode - due o he des uc i e na u e o his analysis, i is no possible o examine
he same egion and i s changes o e ime; Ope ando SEM analysis o selec ed NMC g ain c oss-sec ion a di e en
cha ging s ages – obse a ion o c ack e olu ion du ing i s o ma ion cycle
5 μm
20 μm
p is ine cycled
0.13 V 2.31 V 2.32 V 2.80 V
a
b
2. .Expe imen al me hod
2. 1 Ma e ials
Comme cially a ailable elec ode shee s om Cus omCells we e used in his s udy. We
used NMC 111 coa ed on an aluminum cu en collec o , LTO coa ed on an aluminum
cu en collec o , and g aphi e on a coppe cu en collec o . The capaci y o he
elec odes is speci ied in he da ashee as 1 mAh/cm². In he supplemen a y expe imen ,
me allic li hium (99.9%; Sigma-Ald ich) was used as he coun e elec ode. A Wha man
GF/C glass ibe il e wi h a hickness o 260 µm was used as he sepa a o .
Fo NMC – LTO sys ems, an ionic liquid elec oly e was p epa ed using a mix u e o 1-
me hyl-1-p opylpy olidinium bis( i luo ome hylsul onyl)imide (Py ₁₃-TFSI, >99%; Sigma-
Ald ich) and li hium bis( i luo ome hanesul onyl)imide sal (LiTFSI, >99%; Sigma-Ald ich)
a a concen a ion o 0.5 M.
Fo g aphi e – Li me al sys em, mix u e o LiTFSI: 1-p opyl-1-me hylpy olidinium
bis( luo osul onyl)imide (PYR13FSI), 1:9 mol (Sol ionic >99.5%) was used.
2.2. Cells assembly and placemen in o SEM
In his publica ion, he esul s o h ee expe imen s a e p esen ed. In he i s expe imen ,
he hickness o he en i e NMC elec ode in he NMC-LTO sys em (deno ed as sample 1)
was measu ed. In he second expe imen , he expansion and mo phological changes o
indi idual NMC g ains in a newly cons uc ed NMC-LTO sys em (sample 2) we e analyzed.
The hi d expe imen (sample 3) se es as a supplemen a y e i ica ion o he unc ionali y
o sys em wi h di e en ma e ials. G aphi e s Li me al was used.
Fi s ly, pieces o app oxima ely 5 mm x 8 mm we e cu om he elec ode shee s wi h
scisso s. A sligh ly la ge piece o app oxima ely 7 mm x 12 mm was cu om he
sepa a o wi h a azo blade.
The in es iga ed elec ode was consequen ly mo ed o CleanMill polishe and a c oss-
sec ion was p epa ed using A ion beam. Fo he NMC elec ode, 16 kV and 3.5 mA we e
used o one hou ; o he g aphi e elec ode, 10 kV and 3.5 mA we e used o 1.5 hou s.
Sample ocking +- 40° was used o educe cu aining a i ac . The esul ing a ea size o
he comple ely polished egion was abou 500 um. The simila me hod can be used o
p epa e a c oss-sec ion o bo h elec odes indi idually o he whole cell a once.
The in es iga ed elec ode was hen aligned oge he wi h coun e elec ode and
sepa a o . F om ou expe ience, i has been ound o be ad isable o place he
in es iga ed elec ode in a ew mic ome e s o e lap abo e he sepa a o o a oid looding
he inspec ed a ea wi h elec oly e du ing he SEM ope ando expe imen . The alignmen
and mechanical ixa ion was done in ou designed clamping ool. I con ains wo clamping
pla es, which can be p essed oge he using a sc ew. In addi ion o mechanical clamping,
hese pla es also se e as an elec ical con ac o he pins on he edge o he clamping
ool.
The p e-p epa ed cell was hen ans e ed o he A - illed glo ebox. The specimen was
le in he glo ebox an echambe o se e al hou s unde acuum o d y all pa s o he
sys em be o e subsequen applica ion o he elec oly e. The elec oly e was applied o
he sepa a o edges wi h a pipe e un il he cell was soaked p ope ly. The p epa ed cell
was hen ans e ed o he SEM chambe in he A a mosphe e using he CleanConnec
Sample T ans e Sys em.
In he SEM chambe , a s age wi h he con ac pins was p e-ins alled, in o which he pins
on he clamping ool i when inse ed. These pins a e wi ed h ough a acuum
eed h ough o a po en ios a ou side he SEM chambe (Figu e 2).
A BioLogic SP-150 po en ios a was used o elec ochemical measu emen s. The
capaci y o he sys em was es ima ed based on he elec ode size, conside ing he
da ashee alue o 1 mAh/cm2.
Expe imen al wo k low scheme and clamping ool images a e in ol ed in supplemen a y
da a.
2.3 Sample imaging and da a p ocessing
Fo sample imaging, a Qua o ESEM (The mo Fishe Scien i ic) was u ilized. An
au oma ed con ol sc ip (The mo Scien i ic Au oSc ip 4 So wa e) was de eloped o
manage SEM imaging and s age mo emen s, enabling he imaging mul iple a eas +
di e en ho izon al ield wid h (HFW)/magni ica ion/image g ab se ings ha allowed us
o ake bo h de ailed and o e iew images. The acqui ed images we e hen co ela ed
wi h speci ic poin s on he elec ochemical cu e based on he da a om po en ios a . By
composi ing hese images, a ideo was p oduced, whe e he cu en ame is indica ed
by a cu so ( ed c oss) on he cu e.
Fu he analysis o he images was conduc ed using Phenom Pa icleMe ic pa icle
analysis so wa e and Py hon au oma ic edge de ec ion. Fo selec ed NMC g ains,
changes in size we e examined. The Phenom so wa e iden i ies g ain bounda ies and
calcula es he a ea o each g ain. The eal size o he pa icles can be calcula ed om he
known ield o iew o SEM images.
In he simila way elec ode bounda ies (edges) was de ec ed using Py hon sc ip o ack
whole elec ode hickness changes. Fo bo h, changes a e exp essed as pe cen ages
ela i e o he ini ial image aken a he s a o he measu emen .
Figu e 2: Ope ando SEM expe imen al scheme
3. Resul s and discussion
3.1 Sample 1 – moni o ing NMC elec ode hickness
The NMC-LTO ba e y was p epa ed as desc ibed in chap e 2, mo ed o SEM, and
connec ed o a po en ios a . A e wo ini ial o ma ion cycles conduc ed a 0.1C in a
po en ial window o 1.3 – 2.8 V, 15 min es phase, he ba e y was u he cycled in
cons an cu en ollowed by cons an ol age (CCCV) mode a 1.0C, 5 min es phase,
and imaged. No ably, he cycling con inued beyond he usual ope a ional window (0.8 –
3.3 V) o ampli y he obse ed phenomena and e alua e he expansion o he en i e NMC
elec ode (Figu e 3).
The hickness o he elec oac i e laye was con inuously measu ed du ing cycling (Figu e
3). This da a indica es elec ode expansion du ing ba e y cha ging (NMC elec ode
deli hia ion) and con ac ion du ing ba e y discha ging (NMC elec ode li hia ion).
Mo eo e , a e expansion du ing he ba e y cha ging phase, he elec ode does no
e u n o i s o iginal hickness du ing ba e y discha ging. Ins ead, i g adually expands
wi h each subsequen cycle, leading o i e e sible changes in he elec ode. In he i s
cycle, he hickness was app oxima ely 37.9 μm in he ba e y cha ged s a e and 37.0 μm
in he discha ged s a e. By he end o he 13 h cycle, hese alues inc eased o 39.8 μm
and 39.1 μm, espec i ely.
Decla a ion o gene a i e AI and AI-assis ed echnologies in he w i ing p ocess:
Du ing he p epa a ion o his wo k he au ho s used GPT-4o (OpenAI), No ebookLM
(Google), and DeepL T ansla e in o de o enhance ex quali y, ix g amma e o s, and
imp o e eadabili y. A e using hese ools, he au ho s e iewed and edi ed he con en
as needed and ake ull esponsibili y o he con en o he published a icle.
Re e ences:
[1]
D. Liu, Z. Shadike, R. Lin, K. Qian, H. Li, K. Li, S. Wang, Q. Yu, M. Liu, S. Ganapa hy,
X. Qin, Q.‐H. Yang, M. Wagemake , F. Kang, X.‐Q. Yang, Re iew o Recen
De elopmen o In Si u/Ope ando Cha ac e iza ion Techniques o Li hium Ba e y
Resea ch, Ad anced Ma e ials. 31 (2019).
h ps://doi.o g/10.1002/adma.201806620.
[2]
P.P.R.M.L. Ha ks, F.M. Mulde , P.H.L. No en, In si u me hods o Li-ion ba e y
esea ch: A e iew o ecen de elopmen s, Jou nal O Powe Sou ces. 288 (2015)
92-105. h ps://doi.o g/10.1016/j.jpowsou .2015.04.084.
[3]
S.-M. Bak, Z. Shadike, R. Lin, X. Yu, X.-Q. Yang, In si u/ope ando synch o on-based
X- ay echniques o li hium-ion ba e y esea ch, Npg Asia Ma e ials. 10 (2018) 563-
580. h ps://doi.o g/10.1038/s41427-018-0056-z.
[4]
M. Pin, J. Choi, J.H. Chang, A.S. Schenk, J. Han, S. Wacławek, Y. Kim, J.Y. Cheong,
In si u X- ay based analysis o anode ma e ials o li hium-ion ba e ies: Cu en
s a us and u u e implica ions, Ene gy S o age Ma e ials. 73 (2024).
h ps://doi.o g/10.1016/j.ensm.2024.103798.
[5]
M. Goloza , R. Gau in, K. Zaghib, In Si u and In Ope ando Techniques o S udy Li-
Ion and Solid-S a e Ba e ies: Mic o o A omic Le el, Ino ganics. 9 (2021).
h ps://doi.o g/10.3390/ino ganics9110085.
[6]
W. Du, R.E. Owen, A. Jnawali, T.P. Ne ille, F. Iaco iello, Z. Zhang, S. Lia a d, D.J.L.
B e , P.R. Shea ing, In-si u X- ay omog aphic imaging s udy o gas and s uc u al
e olu ion in a comme cial Li-ion pouch cell, Jou nal O Powe Sou ces. 520 (2022).
h ps://doi.o g/10.1016/j.jpowsou .2021.230818.

[7]
P. Blazek, P. Wes enbe ge , S. E ke , A. B inek, T. Zikmund, D. Re enwande , N.P.
Wagne , J. Keckes, J. Kaise , T. Kazda, P. Vy oubal, M. Macak, J. Tod , Axially and
adially inhomogeneous swelling in comme cial 18650 Li-ion ba e y cells, Jou nal
O Ene gy S o age. 52 (2022). h ps://doi.o g/10.1016/j.es .2022.104563.
[8]
C.L.A. Leung, M.D. Wilson, T. Connolley, S.P. Collins, O.V. Magdysyuk, M.N. Boone,
K. Suzuki, M.C. Veale, E. Lio i, F. Van Assche, A. Lui, C. Huang, Co ela i e ull ield
X- ay comp on sca e ing imaging and X- ay compu ed omog aphy o in si u
obse a ion o Li ion ba e ies, Ma e ials Today Ene gy. 31 (2023).
h ps://doi.o g/10.1016/j.m ene .2022.101224.
[9]
L. Willenbe g, P. Dechen , G. Fuchs, M. Teube , M. Ecke , M. G a , N. Kü en, D.U.
Saue , E. Figgemeie , The De elopmen o Jelly Roll De o ma ion in 18650 Li hium-
Ion Ba e ies a Low S a e o Cha ge, Jou nal O The Elec ochemical Socie y. 167
(2020). h ps://doi.o g/10.1149/1945-7111/aba96d.
[10]
A. P ang, A. Ke sys, A. K is on, D.U. Saue , C. Rahe, S. Käbi z, E. Figgemeie ,
Geome ical Inhomogenei ies as Cause o Mechanical Failu e in Comme cial
18650 Li hium Ion Cells, Jou nal O The Elec ochemical Socie y. 166 (2019) A3745-
A3752. h ps://doi.o g/10.1149/2.0551914jes.
[11]
O.O. Taiwo, D.P. Finegan, J.M. Paz-Ga cia, D.S. Eas wood, A.J. Bodey, C. Rau, S.A.
Hall, D.J.L. B e , P.D. Lee, P.R. Shea ing, In es iga ing he e ol ing mic os uc u e
o li hium me al elec odes in 3D using X- ay compu ed omog aphy, Physical
Chemis y Chemical Physics. 19 (2017) 22111-22120.
h ps://doi.o g/10.1039/C7CP02872E.
[12]
X. Lu, A. Be ei, D.P. Finegan, C. Tan, S.R. Daemi, J.S. Wea ing, K.B. O’Regan,
T.M.M. Heenan, G. Hinds, E. Kend ick, D.J.L. B e , P.R. Shea ing, 3D
mic os uc u e design o li hium-ion ba e y elec odes assis ed by X- ay nano-
compu ed omog aphy and modelling, Na u e Communica ions. 11 (2020).
h ps://doi.o g/10.1038/s41467-020-15811-x.
[13]
C. Zhao, T. Wada, V. De And ade, D. Gü soy, H. Ka o, Y.-chen K. Chen-Wiega ,
Imaging o 3D mo phological e olu ion o nanopo ous silicon anode in li hium ion
ba e y by X- ay nano- omog aphy, Nano Ene gy. 52 (2018) 381-390.
h ps://doi.o g/10.1016/j.nanoen.2018.08.009.
[14]
J. Gonzalez, K. Sun, M. Huang, J. Lamb os, S. Dillon, I. Chasio is, Th ee
dimensional s udies o pa icle ailu e in silicon based composi e elec odes o
li hium ion ba e ies, Jou nal O Powe Sou ces. 269 (2014) 334-343.
h ps://doi.o g/10.1016/j.jpowsou .2014.07.001.
[15]
P. Pie sch, V. Wood, X-Ray Tomog aphy o Li hium Ion Ba e y Resea ch: A
P ac ical Guide, Annual Re iew O Ma e ials Resea ch. 47 (2017) 451-479.
h ps://doi.o g/10.1146/annu e -ma sci-070616-123957.
[16]
N.A. Cañas, S. Wol , N. Wagne , K.A. F ied ich, In-si u X- ay di ac ion s udies o
li hium–sul u ba e ies, Jou nal O Powe Sou ces. 226 (2013) 313-319.
h ps://doi.o g/10.1016/j.jpowsou .2012.10.092.
[17]
<di class="csl-bib-body"><di class="csl-en y">S. Schweidle , L. de Biasi, A.
Schiele, P. Ha mann, T. B ezesinski, J. Janek, Volume Changes o G aphi e Anodes
Re isi ed Ope ando X- ay Di ac ion and In Si u P essu e Analysis S udy: A
Combined Ope ando X- ay Di ac ion and In Si u P essu e Analysis S udy, The
Jou nal O Physical Chemis y C. 122 (2018) 8829-8835.
h ps://doi.o g/10.1021/acs.jpcc.8b01873.</di ></di >
[18]
D. Au bach, Y. Ein‐Eli, The S udy o Li‐G aphi e In e cala ion P ocesses in Se e al
Elec oly e Sys ems Using In Si u X‐Ray Di ac ion, Jou nal O The Elec ochemical
Socie y. 142 (1995) 1746-1752. h ps://doi.o g/10.1149/1.2044188.
[19]
C.-K. Lin, Y. Ren, K. Amine, Y. Qin, Z. Chen, In si u high-ene gy X- ay di ac ion o
s udy o e cha ge abuse o 18650-size li hium-ion ba e y, Jou nal O Powe
Sou ces. 230 (2013) 32-37. h ps://doi.o g/10.1016/j.jpowsou .2012.12.032.
[20]
J. Li, J.R. Dahn, An In Si u X-Ray Di ac ion S udy o he Reac ion o Li wi h
C ys alline Si, Jou nal O The Elec ochemical Socie y. 154 (2007).
h ps://doi.o g/10.1149/1.2409862.
[21]
J. Pa k, S.S. Pa k, Y.S. Won, In si u XRD s udy o he s uc u al changes o g aphi e
anodes mixed wi h SiOx du ing li hium inse ion and ex ac ion in li hium ion
ba e ies, Elec ochimica Ac a. 107 (2013) 467-472.
h ps://doi.o g/10.1016/j.elec ac a.2013.06.059.
[22]
S.-W. Lee, D.-H. Jang, J.-B. Yoon, Y.-H. Cho, Y.-S. Lee, D.-H. Kim, W.-S. Kim, W.-
S. Yoon, C ys al S uc u e Changes o LiNi 0.5 Co 0.2 Mn 0.3 O 2 Ca hode Ma e ials
Du ing he Fi s Cha ge In es iga ed by in si u XRD, Jou nal O Elec ochemical
Science And Technology. 3 (2012) 29-34.
h ps://doi.o g/10.5229/JECST.2012.3.1.29.
[23]
A. Bha ia, S. C e u, M. Hallo , N. Folas e, M. Be he, D. T oadec, P. Roussel, J.‐P.
Pe ei a‐Ramos, R. Baddou ‐Hadjean, C. Le hien, A. Demo iè e, In Si u Liquid
Elec ochemical TEM In es iga ion o LiMn 1.5 Ni 0.5 O 4 Thin Film Ca hode o
Mic o‐Ba e y Applica ions, Small Me hods. 6 (2022).
h ps://doi.o g/10.1002/sm d.202100891.
[24]
C.-M. Wang, In si u ansmission elec on mic oscopy and spec oscopy s udies o
echa geable ba e ies unde dynamic ope a ing condi ions: A e ospec i e and
pe spec i e iew, Jou nal O Ma e ials Resea ch. 30 (2015) 326-339.
h ps://doi.o g/10.1557/jm .2014.281.
[25]
J. Wu, M. Fenech, R.F. Webs e , R.D. Tilley, N. Sha ma, Elec on mic oscopy and
i s ole in ad anced li hium-ion ba e y esea ch, Sus ainable Ene gy & Fuels. 3
(2019) 1623-1646. h ps://doi.o g/10.1039/C9SE00038K.
[26]
J.M. Yuk, H.K. Seo, J.W. Choi, J.Y. Lee, Aniso opic Li hia ion Onse in Silicon
Nanopa icle Anode Re ealed by in Si u G aphene Liquid Cell Elec on Mic oscopy,
Acs Nano. 8 (2014) 7478-7485. h ps://doi.o g/10.1021/nn502779n.
[27]
Z. Zeng, W.-I. Liang, H.-G. Liao, H.L. Xin, Y.-H. Chu, H. Zheng, Visualiza ion o
Elec ode–Elec oly e In e aces in LiPF 6 /EC/DEC Elec oly e o Li hium Ion
Ba e ies ia in Si u TEM, Nano Le e s. 14 (2014) 1745-1750.
h ps://doi.o g/10.1021/nl403922u.
[28]
M.T. McDowell, S.W. Lee, J.T. Ha is, B.A. Ko gel, C. Wang, W.D. Nix, Y. Cui, In Si u
TEM o Two-Phase Li hia ion o Amo phous Silicon Nanosphe es, Nano Le e s. 13
(2013) 758-764. h ps://doi.o g/10.1021/nl3044508.
[29]
Y. Zhang, Y. Li, Z. Wang, K. Zhao, Li hia ion o SiO 2 in Li-Ion Ba e ies: In Si u
T ansmission Elec on Mic oscopy Expe imen s and Theo e ical S udies, Nano
Le e s. 14 (2014) 7161-7170. h ps://doi.o g/10.1021/nl503776u.
[30]
H. Asayesh‐A dakani, W. Yao, Y. Yuan, A. Nie, K. Amine, J. Lu, R. Shahbazian‐
Yassa , In Si u TEM In es iga ion o ZnO Nanowi es du ing Sodia ion and Li hia ion
Cycling, Small Me hods. 1 (2017). h ps://doi.o g/10.1002/sm d.201700202.
[31]
X.H. Liu, L.Q. Zhang, L. Zhong, Y. Liu, H. Zheng, J.W. Wang, J.-H. Cho, S.A. Dayeh,
S.T. Pic aux, J.P. Sulli an, S.X. Mao, Z.Z. Ye, J.Y. Huang, Ul a as Elec ochemical
Li hia ion o Indi idual Si Nanowi e Anodes, Nano Le e s. 11 (2011) 2251-2258.
h ps://doi.o g/10.1021/nl200412p.
[32]
J.Y. Huang, L. Zhong, C.M. Wang, J.P. Sulli an, W. Xu, L.Q. Zhang, S.X. Mao, N.S.
Hudak, X.H. Liu, A. Sub amanian, H. Fan, L. Qi, A. Kushima, J. Li, In Si u
Obse a ion o he Elec ochemical Li hia ion o a Single SnO 2 Nanowi e Elec ode,
Science. 330 (2010) 1515-1520. h ps://doi.o g/10.1126/science.1195628.
[33]
T. Waldmann, A. I u ondobei ia, M. Kaspe , N. Ghanba i, F. Aguesse, E. Bekae , L.
Daniel, S. Genies, I.J. Go don, M.W. Löble, E. De Vi o, M. Wohl ah -Meh ens,
Re iew—Pos -Mo em Analysis o Aged Li hium-Ion Ba e ies: Disassembly
Me hodology and Physico-Chemical Analysis Techniques, Jou nal O The
Elec ochemical Socie y. 163 (2016) A2149-A2164.
h ps://doi.o g/10.1149/2.1211609jes.
[34]
S. Zhou, K. Liu, Y. Ying, L. Chen, G. Meng, Q. Zheng, S.-G. Sun, H.-G. Liao,
Pe spec i e o ope ando/in si u scanning elec on mic oscope in echa geable
ba e ies, Cu en Opinion In Elec ochemis y. 41 (2023).
h ps://doi.o g/10.1016/j.coelec.2023.101374.
[35]
P. BAUDRY, In si u obse a ion by SEM o posi i e composi e elec odes du ing
discha ge o polyme li hium ba e ies, Solid S a e Ionics. 28-30 (1988) 1567-1571.
h ps://doi.o g/10.1016/0167-2738(88)90421-3.
[36]
F. Sagane, R. Shimokawa, H. Sano, H. Sakaebe, Y. I iyama, In-si u scanning
elec on mic oscopy obse a ions o Li pla ing and s ipping eac ions a he li hium
phospho us oxyni ide glass elec oly e/Cu in e ace, Jou nal O Powe Sou ces.
225 (2013) 245-250. h ps://doi.o g/10.1016/j.jpowsou .2012.10.026.
[37]
M. Doll, L. Sannie , B. Beaudoin, M. T en in, J.-M. Ta ascon, Li e Scanning
Elec on Mic oscope Obse a ions o Dend i ic G ow h in Li hium/Polyme Cells,
Elec ochemical And Solid-S a e Le e s. 5 (2002).
h ps://doi.o g/10.1149/1.1519970.
[38]
<di class="csl-bib-body"><di class="csl-en y">P. Ho ing on, M. Lagac, A.
Gue i, P. Boucha d, A. Mauge , C.M. Julien, M. A mand, K. Zaghib, New Li hium
Me al Polyme Solid S a e Ba e y o an Ul ahigh Ene gy 4 e sus Nano Li 1.2 V 3
O 8: Nano C-LiFePO 4 e sus Nano Li 1.2 V 3 O 8, Nano Le e s. 15 (2015) 2671-
2678. h ps://doi.o g/10.1021/acs.nanole .5b00326.</di ></di >
[39]
M. Nagao, A. Hayashi, M. Ta sumisago, T. Kane suku, T. Tsuda, S. Kuwaba a, In si u
SEM s udy o a li hium deposi ion and dissolu ion mechanism in a bulk- ype solid-
s a e cell wi h a Li2S–P2S5 solid elec oly e, Physical Chemis y Chemical Physics.
15 (2013). h ps://doi.o g/10.1039/c3cp51059j.
[40]
P. Pe eno , P. Bayle-Guillemaud, P.-H. Jouneau, A. Boulineau, C. Ville ieille,
Ope ando Focused Ion Beam–Scanning Elec on Mic oscope (FIB-SEM) Re ealing
Mic os uc u al and Mo phological E olu ion in a Solid-S a e Ba e y, Acs Ene gy
Le e s. 9 (2024) 3835-3840. h ps://doi.o g/10.1021/acsene gyle .4c01750.
[41]
S. Kaboli, H. Deme s, A. Paolella, A. Da wiche, M. Don igny, D. Clmen , A. Gue i,
M.L. T udeau, J.B. Goodenough, K. Zaghib, Beha io o Solid Elec oly e in Li-
Polyme Ba e y wi h NMC Ca hode ia in-Si u Scanning Elec on Mic oscopy, Nano
Le e s. 20 (2020) 1607-1613. h ps://doi.o g/10.1021/acs.nanole .9b04452.
[42]
X. Xia, C.V. Di Leo, X.W. Gu, J.R. G ee , In Si u Li hia ion–Deli hia ion o
Mechanically Robus Cu–Si Co e–Shell Nanola ices in a Scanning Elec on
Mic oscope, Acs Ene gy Le e s. 1 (2016) 492-499.
h ps://doi.o g/10.1021/acsene gyle .6b00256.
[43]
C.-Y. Tang, S.J. Dillon, In Si u Scanning Elec on Mic oscopy Cha ac e iza ion o he
Mechanism o Li Dend i e G ow h, Jou nal O The Elec ochemical Socie y. 163
(2016) A1660-A1665. h ps://doi.o g/10.1149/2.0891608jes.
[44]
W. Bensch, J. Ophey, H. Hain, H. Gesswein, D. Chen, R. Mönig, P.A. G ube , S.
Ind is, Chemical and elec ochemical inse ion o Li in o he spinel s uc u e o
CuC 2Se4: ex si u and in si u obse a ions by X- ay di ac ion and scanning
elec on mic oscopy, Physical Chemis y Chemical Physics. 14 (2012).
h ps://doi.o g/10.1039/c2cp00064d.
[45]
P. Ho ing on, M. Don igny, A. Gue i, J. T o ie , M. Lagac, A. Mauge , C.M. Julien,
K. Zaghib, In si u Scanning elec on mic oscope s udy and mic os uc u al e olu ion
o nano silicon anode o high ene gy Li-ion ba e ies, Jou nal O Powe Sou ces.
248 (2014) 457-464. h ps://doi.o g/10.1016/j.jpowsou .2013.09.069.
[46]
C.-Y. Chen, T. Sano, T. Tsuda, K. Ui, Y. Oshima, M. Yamaga a, M. Ishikawa, M.
Ha u a, T. Doi, M. Inaba, S. Kuwaba a, In si u Scanning Elec on Mic oscopy o
Silicon Anode Reac ions in Li hium-Ion Ba e ies du ing Cha ge/Discha ge
P ocesses, Scien i ic Repo s. 6 (2016). h ps://doi.o g/10.1038/s ep36153.
[47]
S. Kaboli, P. Noel, D. Clmen , H. Deme s, A. Paolella, P. Boucha d, M.L. T udeau,
J.B. Goodenough, K. Zaghib, On high- empe a u e e olu ion o passi a ion laye in
Li–10 w % Mg alloy ia in si u SEM-EBSD, Science Ad ances. 6 (2020).
h ps://doi.o g/10.1126/sciad .abd5708.
[48]
T. Tsuda, K. Hosoya, T. Sano, S. Kuwaba a, In-si u scanning elec on mic oscope
obse a ion o elec ode eac ions ela ed o ba e y ma e ial, Elec ochimica Ac a.
319 (2019) 158-163. h ps://doi.o g/10.1016/j.elec ac a.2019.06.165.
[49]
X. Cheng, Y. Li, T. Cao, R. Wu, M. Wang, H. Liu, X. Liu, J. Lu, Y. Zhang, Real-Time
Obse a ion o Chemomechanical B eakdown in a Laye ed Nickel-Rich Oxide
Ca hode Realized by In Si u Scanning Elec on Mic oscopy, Acs Ene gy Le e s. 6

(2021) 1703-1710. h ps://doi.o g/10.1021/acsene gyle .1c00279.
[50]
X. Zhou, T. Li, Y. Cui, Y. Fu, Y. Liu, L. Zhu, In Si u Focused Ion Beam Scanning
Elec on Mic oscope S udy o Mic os uc u al E olu ion o Single Tin Pa icle Anode
o Li-Ion Ba e ies, Acs Applied Ma e ials & In e aces. 11 (2019) 1733-1738.
h ps://doi.o g/10.1021/acsami.8b13981.
[51]
D.J. Mille , C. P o , J.G. Wen, D.P. Ab aham, J. Ba eño, Obse a ion o
Mic os uc u al E olu ion in Li Ba e y Ca hode Oxide Pa icles by In Si u Elec on
Mic oscopy, Ad anced Ene gy Ma e ials. 3 (2013) 1098-1103.
h ps://doi.o g/10.1002/aenm.201300015.
[52]
D. Chen, S. Ind is, M. Schulz, B. Game , R. Mönig, In si u scanning elec on
mic oscopy on li hium-ion ba e y elec odes using an ionic liquid, Jou nal O Powe
Sou ces. 196 (2011) 6382-6387. h ps://doi.o g/10.1016/j.jpowsou .2011.04.009.
[53]
X. Liu, A. Ma iani, T. Dieman , X. Dong, P.‐H. Su, S. Passe ini, Locally Concen a ed
Ionic Liquid Elec oly es Enabling Low‐Tempe a u e Li hium Me al Ba e ies,
Angewand e Chemie. 135 (2023). h ps://doi.o g/10.1002/ange.202305840.
[54]
F. O sini, A. Du Pasquie , B. Beaudoin, J.M. Ta ascon, M. T en in, N. Langenhuizen,
E. De Bee , P. No en, In si u Scanning Elec on Mic oscopy (SEM) obse a ion o
in e aces wi hin plas ic li hium ba e ies, Jou nal O Powe Sou ces. 76 (1998) 19-
29. h ps://doi.o g/10.1016/S0378-7753(98)00128-1.
[55]
G. Rong, X. Zhang, W. Zhao, Y. Qiu, M. Liu, F. Ye, Y. Xu, J. Chen, Y. Hou, W. Li, W.
Duan, Y. Zhang, Liquid‐Phase Elec ochemical Scanning Elec on Mic oscopy o In
Si u In es iga ion o Li hium Dend i e G ow h and Dissolu ion, Ad anced Ma e ials.
29 (2017). h ps://doi.o g/10.1002/adma.201606187.
[56]
P.R. Raimann, N.S. Hochga e e , C. Ko epp, K.C. Mölle , M. Win e , H. Sch ö ne ,
F. Ho e , J.O. Besenha d, Moni o ing dynamics o elec ode eac ions in Li-ion
ba e ies by in si u ESEM, Ionics. 12 (2006) 253-255.
h ps://doi.o g/10.1007/s11581-006-0046-y.
[57]
I. Dienwiebel, M. Win e , M. Bö ne , Visualiza ion o Deg ada ion Mechanisms o
Nega i e Elec odes Based on Silicon Nanopa icles in Li hium-Ion Ba e ies ia
Quasi In Si u Scanning Elec on Mic oscopy and Ene gy-Dispe si e X- ay
Spec oscopy, The Jou nal O Physical Chemis y C. 126 (2022) 11016-11025.
h ps://doi.o g/10.1021/acs.jpcc.2c03294.
[58]
K.L. Jungjohann, R.N. Gannon, S. Go ipa i, S.J. Randolph, L.C. Me ill, D.C.
Johnson, K.R. Za adil, S.J. Ha is, K.L. Ha ison, C yogenic Lase Abla ion Re eals
Sho -Ci cui Mechanism in Li hium Me al Ba e ies, Acs Ene gy Le e s. 6 (2021)
2138-2144. h ps://doi.o g/10.1021/acsene gyle .1c00509.
[59]
L. No ak, P. Glajc, O. Kl ac, Ba e y in si u Elec ical Tes ing in FIB-SEM, Mic oscopy
And Mic oanalysis. 28 (2022) 834-835.
h ps://doi.o g/10.1017/S1431927622003737.
[60]
W. Hau e, S. Menzel, T. Göbel, Ad an ages o B oad Ion Beam (BIB) P ocessing
Compa ed wi h Focused Ion Beam (FIB) Technology o 3D In es iga ion o
He e ogeneous Solids, Mic oscopy And Mic oanalysis. 9 (2003) 148-149.
h ps://doi.o g/10.1017/S1431927603016106.
[61]
Z. S a o a, O. Kl ac, J. Bana, B. Ano humakkool, T. Zikmund, P. Blazek, J. Kaise ,
T. Kazda, Comp ehensi e s udy o apid capaci y ade in p isma ic Li-ion cells wi h
lexible packaging, Scien i ic Repo s. 14 (2024). h ps://doi.o g/10.1038/s41598-
024-77673-3.
[62]
K.K. Neelise y, J. S e ina, J. Vond uška, M. T enz, T. Kazda, M. H ouzek, P.
Wand ol, T ans e o li hium oil unde ine condi ions using CleanConnec ine gas
ans e sys em, Mic oscopy And Mic oanalysis. 27 (2021) 2508-2509.
h ps://doi.o g/10.1017/S1431927621008941.
[63]
F.B. Spingle , S. Küche , R. Phillips, E. Moyassa i, A. Jossen, Elec ochemically
S able In Si u Dila ome y o NMC, NCA and G aphi e Elec odes o Li hium-Ion
Cells Compa ed o XRD Measu emen s, Jou nal O The Elec ochemical Socie y.
168 (2021). h ps://doi.o g/10.1149/1945-7111/ab 262.