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Dynamic approximate entropy electroanatomic maps detect rotors in a simulated atrial fibrillation model

Abstract

There is evidence that rotors could be drivers that maintain atrial fibrillation. Complex fractionated atrial electrograms have been located in rotor tip areas. However, the concept of electrogram fractionation, defined using time intervals, is still controversial as a tool for locating target sites for ablation. We hypothesize that the fractionation phenomenon is better described using non-linear dynamic measures, such as approximate entropy, and that this tool could be used for locating the rotor tip. The aim of this work has been to determine the relationship between approximate entropy and fractionated electrograms, and to develop a new tool for rotor mapping based on fractionation levels. Two episodes of chronic atrial fibrillation were simulated in a 3D human atrial model, in which rotors were observed. Dynamic approximate entropy maps were calculated using unipolar electrogram signals generated over the whole surface of the 3D atrial model. In addition, we optimized the approximate entropy calculation using two real multicenter databases of fractionated electrogram signals, labeled in 4 levels of fractionation. We found that the values of approximate entropy and the levels of fractionation are positively correlated. This allows the dynamic approximate entropy maps to localize the tips from stable and meandering rotors. Furthermore, we assessed the optimized approximate entropy using bipolar electrograms generated over a vicinity enclosing a rotor, achieving rotor detection. Our results suggest that high approximate entropy values are able to detect a high level of fractionation and to locate rotor tips in simulated atrial fibrillation episodes. We suggest that dynamic approximate entropy maps could become a tool for atrial fibrillation rotor mapping.

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Dynamic approximate entropy electroanatomic maps detect rotors in a simulated atrial fibrillation model

Author: Ugarte, Juan P.,Orozco-Duque, Andrés,Tobon Zuloaga, Catalina,Kremen, Vaclav,Novak, Daniel,Saiz Rodríguez, Francisco Javier,Oesterlein, Tobias,Schmitt, Clauss,Luik, Armin,Bustamante, John
Publisher: Public Library of Science
Year: 2014
DOI: 10.1371/journal.pone.0114577
Source: https://riunet.upv.es/bitstream/10251/59810/1/Juan%20P%20Ugarte%3bAndres%20Orozco-Duque%3bTob%c3%b3n%20-%20Dynamic%20approximate%20entropy%20electroanatomic%20maps%20detect....pdf
RESEARCH ARTICLE
Dynamic App oxima e En opy
Elec oana omic Maps De ec Ro o s in a
Simula ed A ial Fib illa ion Model
Juan P. Uga e
1
*, And e´s O ozco-Duque
1
, Ca alina Tobo´n
2
, Vacla K emen
3,4
,
Daniel No ak
3
, Ja ie Saiz
5
, Tobias Oes e lein
6
, Clauss Schmi
7
, A min Luik
7
,
John Bus aman e
1
1. Cen o de Bioingenie ı´a, Uni e sidad Pon i icia Boli a iana, Medellı´n, Colombia, 2. GI
2
B, Ins i u o
Tecnolo´gico Me opoli ano, Medellı´n, Colombia, 3. Czech Ins i u e o In o ma ics, Robo ics and Cybe ne ics,
Czech Technical Uni e si y in P ague, P ague, Czech Republic, 4. Depa men o Cybe ne ics, Facul y o
Elec ical Enginee ing, Czech Technical Uni e si y in P ague, P ague, Czech Republic, 5. I3BH, Uni e si a
Poli e`cnica de Vale`ncia, Valencia, Spain, 6. Ins i u e o Biomedical Enginee ing, Ka ls uhe Ins i u e o
Technology (KIT), Ka ls uhe, Ge many, 7. Medizinische Klinik IV, S aed isches Klinikum Ka ls uhe, Ka ls uhe,
Ge many
*[email p o ec ed].edu.co
Abs ac
The e is e idence ha o o s could be d i e s ha main ain a ial ib illa ion.
Complex ac iona ed a ial elec og ams ha e been loca ed in o o ip a eas.
Howe e , he concep o elec og am ac iona ion, de ined using ime in e als, is
s ill con o e sial as a ool o loca ing a ge si es o abla ion. We hypo hesize ha
he ac iona ion phenomenon is be e desc ibed using non-linea dynamic
measu es, such as app oxima e en opy, and ha his ool could be used o
loca ing he o o ip. The aim o his wo k has been o de e mine he ela ionship
be ween app oxima e en opy and ac iona ed elec og ams, and o de elop a new
ool o o o mapping based on ac iona ion le els. Two episodes o ch onic a ial
ib illa ion we e simula ed in a 3D human a ial model, in which o o s we e
obse ed. Dynamic app oxima e en opy maps we e calcula ed using unipola
elec og am signals gene a ed o e he whole su ace o he 3D a ial model. In
addi ion, we op imized he app oxima e en opy calcula ion using wo eal mul i-
cen e da abases o ac iona ed elec og am signals, labeled in 4 le els o
ac iona ion. We ound ha he alues o app oxima e en opy and he le els o
ac iona ion a e posi i ely co ela ed. This allows he dynamic app oxima e en opy
maps o localize he ips om s able and meande ing o o s. Fu he mo e, we
assessed he op imized app oxima e en opy using bipola elec og ams gene a ed
o e a icini y enclosing a o o , achie ing o o de ec ion. Ou esul s sugges ha
high app oxima e en opy alues a e able o de ec a high le el o ac iona ion and
OPEN ACCESS
Ci a ion: Uga e JP, O ozco-Duque A, Tobo´n C,
K emen V, No ak D, e al. (2014) Dynamic
App oxima e En opy Elec oana omic Maps De ec
Ro o s in a Simula ed A ial Fib illa ion
Model. PLoS ONE 9(12): e114577. doi:10.1371/
jou nal.pone.0114577
Edi o : Alexande V. Pan ilo , Gen Uni e si y,
Belgium
Recei ed: June 13, 2014
Accep ed: No embe 11, 2014
Published: Decembe 9, 2014
Copy igh : ß2014 Uga e e al. This is an open-
access a icle dis ibu ed unde he e ms o he
C ea i e Commons A ibu ion License, which
pe mi s un es ic ed use, dis ibu ion, and ep o-
duc ion in any medium, p o ided he o iginal au ho
and sou ce a e c edi ed.
Da a A ailabili y: The au ho s con i m ha all da a
unde lying he indings a e ully a ailable wi hou
es ic ion. The da a a e a ailable a h ps://gi hub.
com/and es od/A ial_Elec og ams_ApEn.
Funding: JPU, CT, and JB we e pa ially
suppo ed by Depa amen o Adminis a i o de
Ciencia, Tecnologı´a e Inno acio´n de la Republica
de Colombia (www.colciencias.go .co), p ojec
#121056933647; AO was suppo ed by he
P og ama de Fo macio´n de In es igado es
F ancisco Jose de Caldas (www.colciencias.go .
co); VK and DN we e pa ially suppo ed by
esea ch p ojec #MSM6840770012
In e disciplina y Biomedical Enginee ing Resea ch
II om he Minis y o Educa ion (www.msm .cz),
You h and Spo s o he Czech Republic, and VK
was pa ially suppo ed by pos -doc o al esea ch
p ojec GACR #P103/11/P106 o he Czech
Science Founda ion (www.gac .cz). The unde s
had no ole in s udy design, da a collec ion and
analysis, decision o publish, o p epa a ion o he
manusc ip .
Compe ing In e es s: The au ho s ha e decla ed
ha no compe ing in e es s exis .
PLOS ONE | DOI:10.1371/jou nal.pone.0114577 Decembe 9, 2014 1/19
o loca e o o ips in simula ed a ial ib illa ion episodes. We sugges ha dynamic
app oxima e en opy maps could become a ool o a ial ib illa ion o o mapping.
In oduc ion
Ca he e abla ion based on mapping p ocedu es has e olu ionized he ea men
o a ial ib illa ion (AF). Elec oana omical mapping o guided AF abla ion
p o ides a 3D econs uc ion o he ca diac chambe s oge he wi h elec ical
in o ma ion ob ained om elec og ams (EGM). Mappings o ac i a ion wa es,
ol age, dominan equency and complex ac iona ed a ial elec og ams (CFAE)
a e used o localize a ge si es o abla ion. Howe e , he e a e limi a ions wi h
hese echniques, which depend hea ily on he expe ise o he elec ophysiologis
[1].
CFAE mapping is s ill a deba ed echnique [2]. CFAE is a physiopa hological
concep ha was in oduced by Nademanee [3]. Howe e , his concep is b oadly
and unclea ly de ined, and in ol es inhe en subjec i i y [4]. This can lead o
inco ec de ec ion o a ge si es o abla ion, mis aking EGM ha a e
ac iona ed and unc ional in na u e [5]. I also makes s udies di icul o
compa e. While he concep o CFAE has made a ele an con ibu ion o he
s udy o AF, i may ail o desc ibe he wide ange o EGM ac iona ion ha
occu s in speci ic cases. In addi ion, inconsis en esul s ha e been ound using he
CFAE concep . Taking his in o accoun , ecen s udies ha e helped o unde s and
he concep o CFAE as a nonlinea phenomenon o quan i ying a ious CFAE
pa e ns, wi hou using cycle leng h c i e ia [6–8].
S udies ha e shown ha si es ep esen ing AF subs a es a e cha ac e ized by a
high deg ee o diso ganiza ion in EGM [9], and, acco dingly, me hods o EGM
signal p ocessing a e being designed o quan i y he deg ee o ac iona ion o
EGM [7,8]. The ela ionship be ween CFAE and he o o ip has been epo ed in
ecen s udies [7,10–13], bu au oma ic o o mapping me hods ha e no been
ully es ablished.
The o o hypo hesis desc ibed in [14] p oposes ha in a signi ican numbe o
pa ien s, a o o o a small numbe o o o s a e d i e s which main ain he
a hy hmia. A o o is a o ex o a spi al wa e o a ing a ound an unexci able
co e. Na ayan e al ha e p o ided e idence ha human AF can be sus ained by
localized o o s [15,16].
Based on he o o hypo hesis, which su mises ha sus ained AF depends on
unin e up ed pe iodic ac i i y o he disc e e een an si e, and on e idence ha
a high deg ee o i egula i y is p esen in EGM signals a he o o ip, we
hypo hesized ha 1) he le el o ac iona ion on EGM can be measu ed using a
non-linea index such as App oxima e En opy (ApEn), and 2) high le els o
ApEn can be used o localize he o o ip.
Dynamic ApEn Maps in A ial Fib illa ion
PLOS ONE | DOI:10.1371/jou nal.pone.0114577 Decembe 9, 2014 2/19
Ma e ials and Me hods
We p esen dynamic ApEn maps as a new ool o o o de ec ion. ApEn alues
o each EGM eco ded om he a ial su ace a e used o cons uc a colo map.
We assess he me hod in a 3D compu a ional model o human a ia. Fig. 1A
schema ically illus a es he me hodology used in his wo k, as ollows. Fi s , wo
AF episodes we e simula ed: a ch onic AF episode in which wo s able o o s we e
ound, and a ch onic AF episode in which a meande ing o o was ound. Second,
ApEn measu emen s, using s anda d pa ame e s, a e calcula ed o e i ual EGM
eco ded om he 3D model o cons uc dynamic ApEn maps. Thi d, he ApEn
pa ame e s we e op imized using eal measu ed bipola EGM om mul i-cen e
da abases. Fou h, dynamic ApEn maps we e gene a ed using op imized
pa ame e s. Nex , he o o s ips a e iden i ied by analyzing local ac i a ion ime
maps and dynamic ApEn maps. The de ails o each s ep a e p esen ed in he
ollowing sec ions.
Ch onic a ial ib illa ion model
A ealis ic 3D model o human a ia including he main ana omical s uc u es,
ibe o ien a ion, elec ophysiological and conduc ion he e ogenei y and aniso-
opy, was de eloped in an ea lie wo k [17]. I includes 52906 hexahed al
elemen s and 100554 nodes. The Cou emanche-Rami ez-Na el-Knelle mem-
b ane o malism [18,19] was implemen ed o ep oduce he human a ial cellula
elec ical ac i i y. The monodomain model o he elec ical p opaga ion o he
ac ion po en ial along he issue is desc ibed by a eac ion-di usion equa ion, and
is sol ed using a ini e elemen me hod [17].
To ep oduce a ial elec ical emodeling, changes in he maximum
conduc ance and kine ics o di e en ionic channels o human a ial cells
obse ed in expe imen al s udies o ch onic AF [20–22] ha e been inco po a ed
in o he a ial cellula model. The ollowing pa ame e s we e al e ed [23]: he
maximum conduc ance o IK1was inc eased by 100%, while he maximum
conduc ance alues o ICaL and I o we e dec eased by 70% and by 50%,
espec i ely.
Simula ion p o ocol
Two AF episodes we e gene a ed by he S1–S2 p o ocol as ollows: a ain o
s imuli wi h a basic cycle leng h o 1000 ms was applied o a pe iod o 5 seconds
in he sinus node a ea o simula e he sinus hy hm (S1). A e he las bea o he
sinus s imulus, a bu s o 6 ec opic bea s (S2) o high equency we e deli e ed
in o he igh supe io pulmona y ein, o he i s AF episode; and hey we e
deli e ed in o he pos e io wall o he le a ium nea o he igh pulmona y
eins, o he second episode.
Vi ual elec og ams
Unipola EGM in di e en poin s o he a ia su ace unde condi ions o uni o m
in acellula aniso opic esis i i y was simula ed, as p e iously desc ibed [24].
Dynamic ApEn Maps in A ial Fib illa ion
PLOS ONE | DOI:10.1371/jou nal.pone.0114577 Decembe 9, 2014 3/19
The ex acellula po en ial (we) is gi en by he ollowing equa ion:
we( )~{
1
4p
si
seððð+Vm( ’):+1
’{

d ð1Þ
whe e +Vmis he spa ial g adien o ansmemb ane po en ial Vm,siis he
in acellula conduc i i y, seis he ex acellula conduc i i y, is he dis ance
om he sou ce poin (x,y,z) o he measu ing poin (x’,y’,z’)and d is he
di e en ial olume. EGM signals we e eco ded a 1kHz. Bipola EGM we e
calcula ed by sub ac ing wo 1-mm-spaced adjacen unipola EGM.
Nume ical and compu a ional me hods
A hexahed al mesh was buil om he h ee-dimensional ana omical model using
Femap om Siemens PLM so wa e. Equa ions we e nume ically sol ed using
EMOS so wa e [25]. EMOS is a pa allel code (mpibased) ha implemen s he
ini e elemen me hod and Ope a o Spli ing o sol ing he monodomain model.
The ime s ep was ixed o 0.001 ms. Simula ion o 10 seconds o a ial ac i i y
ook 14 hou s on a compu ing node wi h wo 6-co e In el Xeon X5650 clocked a
2.66 GHz and 48GB DDR3 RAM.
Isoch one ac i a ion maps
A me hod was de eloped as an a angemen o he isoch one map me hod [26],
whe e he local ac i a ion imes (LAT) a e ep esen ed in a colo map. To build an
ac i a ion map, i is necessa y o de ec he local ac i a ion wa es. An algo i hm
based on he Con inuous Wa ele T ans o m was implemen ed o de ec local
ac i a ion wa es. A e a peak has been de ec ed, an isoch one map is cons uc ed
wi h he LAT in o ma ion. In o de o ensu e ha one comple e ac i a ion cycle is
scanned, i is necessa y o isualize he LAT minimum o a pe iod o 100 ms. The
Fig. 1. Expe imen al se up. A: Simula ed episode o ch onic AF in a 3D model o human a ia. A local ac i a ion ime map was cons uc ed as an al e na i e
me hod o de ec ing o o s. A pseudo-EGM signal was calcula ed om he 3D model. ApEn was calcula ed in pseudo-EGM signals eco ded o e he whole
a ial su ace. ApEn maps we e cons uc ed in o de o obse e he ela ion be ween ApEn alues and o o loca ions. B: Examples o EGM signals o DB-
CZ-DE. Rep esen a i es om he ou le els o complexi y p oposed o he pu poses o he s udy a e shown om C0 o C3. These signals we e used o
ApEn pa ame e op imiza ion.
doi:10.1371/jou nal.pone.0114577.g001
Dynamic ApEn Maps in A ial Fib illa ion
PLOS ONE | DOI:10.1371/jou nal.pone.0114577 Decembe 9, 2014 4/19
poin s a which he ac i a ion wa es a e spinning can be obse ed; hese poin s
co espond o he o o ip. This p ocedu e was used as a gold s anda d o
compa ison wi h ou esul s.
App oxima e en opy and pa ame e op imiza ion
App oxima e En opy (ApEn) is a nonlinea s a is ic p oposed by Pincus [27]. I
quan i ies he deg ee o complexi y o signals. The calcula ion o ApEn depends
on h ee pa ame e s: numbe o da a poin s N, embedding dimension mand
h eshold .ApEn(m, ,N)allows o measu e egula i y by calcula ing he
p obabili y ha pa e ns o leng h m emain close on nex inc emen al
compa isons wi hin a signal o leng h N, wi h m N[28].
ApEn is heo e ically de ined as he alue dependen on mand , conside ing
N??. This alue canno be eached bu can be app oxima ed. The
app oxima ion is well sui ed when a signi ican numbe o pa e ns, de e mined
by m, a e acqui ed [29]. Pincus s a ed ha small alues o ma e needed in o de
o con e ge o he eal alue o ApEn [28]. Speci ically, he sugges ed m~2,
[½0:1,0:25as s anda d pa ame e s.
We e alua e ApEn(2,0:1,1000)and ApEn(2,0:1,500) om s anda d pa ame e s.
Fu he mo e, we p opose mand alues de i ed om an op imiza ion p ocedu e
using a da ase o EGM. This da ase has al eady been applied o o he s udies
aimed a de eloping signal p ocessing ools o CFAE [30,31].
Da ase
We used wo di e en EGM da abases, independen ly eco ded om AF pa ien s,
and independen ly e alua ed. The da abases we e anked by di e en elec o-
physiology eams, wi h di e en equipmen , om wo di e en coun ies. The 542
signals in he da abases we e classi ied using he same c i e ia di ided in o ou
classes: ac iona ed signals we e ca ego ized by expe s in o h ee le els o
ac iona ion (C1, C2 and C3), and non ac iona ed EGM signals we e conside ed
as le el 0 (C0). The ou ac iona ion classes, see Fig. 1B, a e:
NC0: Non ac iona ed EGM and also high equency EGM.
NC1: F ac iona ed EGM wi h pe iodic ac i i y.
NC2: A mix u e o pe iodic ac iona ed and pe iodic non ac iona ed EGM.
NC3: High equency EGM wi h con inuous ac i i y. No egula ac i a ion can
be seen.
The en i e da abase cons i u es a e ospec i e-o line analysis. Fo u he
in o ma ion abou he acquisi ion and classi ica ion o his da abase, e e o
[32,33]. The da abase is a ailable a h ps://gi hub.com/and es od/A ial_
Elec og ams_ApEn.
Op imiza ion p ocess
ApEn pa ame e s mand we e se using eal da a om he da abase, o ob ain
op imal alues. The a ia ion o mwas limi ed o 5, as ecommended by Pincus
[27]. Pa ame e a ied om 0.02 o 0.6, inc easing in s eps o 0.02. The da abase
Dynamic ApEn Maps in A ial Fib illa ion
PLOS ONE | DOI:10.1371/jou nal.pone.0114577 Decembe 9, 2014 5/19

was o ganized in o ou le els o ac iona ion (C0, C1, C2 and C3). Each le el
con ains he en i e se o signals o he co esponding le el o ac iona ion. The
i s 500 and 1000 ms o each EGM we e conside ed. The numbe s o EGM signals
we e as ollows: 175 signals in C0, 117 signals in C1, 184 signals in C2, and 66
signals in C3. F om now on, we e e o his da abase o ganiza ion as DB-CZ-GE.
Fo each combina ion o mand ,ApEn was calcula ed o each EGM om DB-
CZ-GE and a boxplo was cons uc ed, assigning a box o each le el.
In he in e es o minimizing he sca e o each class and maximizing he
dis ances be ween he ApEn measu es o he classes, wo c i e ia we e conside ed
in he op imiza ion p ocedu e: in e class pe cen ile dis ance d1and in e class
minimum-maximum dis ance d2, which we e de ined as ollows:
d1~X
3
i~1
Q1(Ciz1){Q3(Ci)½ ð2Þ
d2~X
3
i~1
min(Ciz1){max(Ci)½ ð3Þ
whe e Q1and Q3a e he i s and hi d quan ile, espec i ely.
To selec he pa ame e s o be used o ApEn, an op imiza ion unc ion Jbp was
cons uc ed by equal weigh ing o c i e ia d1and d2 om (2) and (3):
Jbp~d1zd2ð4Þ
In o de o alida e he ApEn pa ame e s ob ained in he op imiza ion
p ocedu e and o a oid o e aining, K-c oss alida ion was pe o med.
Randomly gene a ed pa i ions we e selec ed om ull DB-CZ-GE. K~10 subse s
we e o med.
Dynamic ApEn mapping
In o de o gene a e a dynamic ApEn map o e he su ace o he a ial model, he
s anda d ApEn pa ame e s m~2and ~0:1, as sugges ed by Pincus [27,28,34]
and he pa ame e s o ApEn ob ained in he op imiza ion p ocedu e, we e used.
ApEn was calcula ed o i ual unipola EGM signals, using mo ing windows o
500 and 1000 poin s, wi hou o e lapping. The ange o ApEn, o e he en i e se
o i ual EGM, was applied o a colo scale, whe e ed colo co esponds o
max (ApEn)and blue colo co esponds o 0. Each i ual EGM is ela ed o an
elemen in he model. A 1000-poin window was applied o acking s able
o o s. A 500-poin window was applied o acking meande ing o o s. Unipola
EGM o e he en i e su ace o he a ia we e analyzed, wi h he excep ion o he
meande ing o o case, in which an obse a ion a ea was selec ed in o de o
e alua e he beha io o he op imized ApEn du ing he p esence and absence o
he ip o he o o .
Dynamic ApEn Maps in A ial Fib illa ion
PLOS ONE | DOI:10.1371/jou nal.pone.0114577 Decembe 9, 2014 6/19
Bipola -EGM based dynamic ApEn maps we e also cons uc ed o he s able
o o case. An obse a ion a ea, in which he o o ip is ancho ed, was selec ed.
The ApEn alues o bipola EGM we e calcula ed using he op imized pa ame e s
and he 1000-poin window. Shannon En opy (ShEn) maps we e also gene a ed,
h ough a 4-second window and bins o 0.01 mV, in acco dance wi h he wo k o
Ganesan e al [7]. The ShEn pe o mance in unipola EGM was also assessed.
Resul s
CFAE mapping o s able o o s du ing AF simula ion applying
ApEn wi h s anda d pa ame e s
An AF p opaga ion pa e n o e he a ia was gene a ed in he 3D model o
human a ia, see he ac ion po en ial p opaga ion in S1 Video. Du ing AF ac i i y
ini ia ed by an ec opic ocus applied in o he igh supe io pulmona y ein, wo
s able o o s we e obse ed in he simula ion. One is loca ed in he pos e io wall
o he le a ium, nea he le pulmona y ein, named R1, and he o he is
loca ed in he supe io ena ca a, named R2. Fig. 2A shows he ac ion po en ial
wa e on s delimi ed by con ou lines om he in e al be ween 1 s and 2 s o AF
simula ion. Ro o s R1 and R2, and a block line loca ed o e he in e io igh
pulmona y ein, named B1, ha e been ma ked. 42835 EGM we e calcula ed in he
whole a ial su ace o he 3D model, o e a ou -second window.
Fo all EGM signals, he ApEn measu emen s we e calcula ed using he
s anda d pa ame e s (m~2, ~0:1). The ApEn alues we e used o gene a e a
colo map o e he ana omic s uc u e o he a ia in a 3D model. In his manne ,
a dynamic ApEn map was ob ained and he ame co esponding o he ime
in e al om 1 s o 2 s is depic ed in Fig. 2B. Red colo a eas, co esponding o
high ApEn alues (0:3285+0:0202), include B1 and he co ona y sinus (CS) and
also R1 and R2.
Op imiza ion o ApEn pa ame e s (mand )
The op imiza ion p ocedu e esul ed in m~3, ~0:38, o N~1000 and m~3,
~0:30, o N~500.Fig. 3A shows he boxplo s o ApEn(3,0:38,1000)and o
ApEn(3,0:30,500), espec i ely, applied o DB-CZ-GE. In addi ion, he Spea man
co ela ion coe icien Sbe ween ApEn and he co esponding le el o
ac iona ion was calcula ed.
CFAE mapping o s able o o s du ing AF simula ion applying
ApEn wi h op imized pa ame e s
A dynamic ApEn(3,0:38,1000)map was gene a ed using unipola EGM, and he
ame co esponding o he ime in e al 1 s o 2 s is depic ed in Fig. 2C, see S1
Video. The dynamic ApEn map e eals wo a eas o high ApEn alues
(0:3285+0:0202), co esponding o o o s R1 and R2. In addi ion, he hi d a ea
wi h lowe ApEn alues (0:2724+0:0238) co esponds o B1, aking in o accoun
Dynamic ApEn Maps in A ial Fib illa ion
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ha passi e ac i a ion egions ha e ApEn alues lowe han 0.1. A ShEn map was
also gene a ed and is shown in Fig. 2D. Red colo a eas, co esponding o high
ShEn alues (8:375+0:125), include small icini ies nea o R1 and nea o B1,
along o he zones, e.g. CS, he in e io wall o he le a ia, he le and igh
appendage and he la e al wall nea o he le appendage. The LAT me hod was
applied as a e e ence me hod, see S2 Video.Fig. 3B shows isoch onic maps om
R1 and R2. The o o ip is de ined by he con e ging poin s o he colo ed wa es.
These wa es ep esen he local ac i a ion. G een colo indica es ea ly ac i a ion
poin s. Table 1 shows he spa ial loca ion o R1 and R2 ound using he LAT
me hod and he dynamic ApEn mapping me hod. The las column co esponds o
he Euclidean dis ance be ween he spa ial coo dina es om he o o ip,
iden i ied using bo h me hods. The maximum dis ance is 1.66 mm. Unipola
EGM ex ac ed om o o si es R1 and R2, and nea o block a ea B1, a e shown
in Fig. 3C. ApEn alues a e also p esen ed. The EGM co esponding o o o
ac i i y ( op) ha e low ol age and i egula mo phology. The EGM co e-
sponding o he block line (below le ) p esen s ac iona ion, bu ac i a ion
Fig. 2. Compa ison be ween ools o o o mapping. A. Ac ion po en ial wa e on delimi ed by con ou
lines o e he 3D Human A ia Model ex ac ed om he in e al be ween 1 s and 2 s o simula ion. The
spinning wa e on s a ound one poin de ine s able o o s R1 and R2. Line block B1 can be seen a he igh
in e io pulmona y ein. B. Dynamic ApEn map calcula ed using s anda d pa ame e s and unipola EGM. C.
Dynamic ApEn map calcula ed om he op imized pa ame e s ob ained in ou wo k, using unipola EGM. D.
Shannon en opy map, using unipola EGM. No e ha map C shows be e sensi i i y o localizing o o ips.
E. Dynamic ApEn map calcula ed om op imized pa ame e s using bipola EGM wi h ho izon al and e ical
o ien a ion. The egion co esponds o he icini y o o o R1. F. ShEn map calcula ed using he bipola EGM
ob ained om he icini y o o o R1.
doi:10.1371/jou nal.pone.0114577.g002
Dynamic ApEn Maps in A ial Fib illa ion
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pa e ns a e isible and hei ampli udes a e simila o non- ac iona ed EGM
(below igh ). The highes ApEn alues co espond o R1 and R2.
A ci cula a ea con aining R1 was selec ed. Bipola EGM we e calcula ed using
ho izon al and e ical bipole o ien a ion. 636 EGM we e ob ained o each
o ien a ion. Fig. 2E shows he dynamic ApEn(3,0:38,1000)maps o ho izon al
and e ical bipola o ien a ion, in he ime in e al be ween seconds 1 and 2.
High ApEn alues co espond wi h he ip o he o o in bo h cases. Fig. 2F
shows he ShEn maps. The e ical bipola o ien a ion map p esen s a egion o
Fig. 3. Localiza ion o s able o o s. A: Resul s o he op imiza ion p ocedu e. Boxplo s o ApEn no malized alues using op imized pa ame e s:
ApEn(1000,3,0:38)(le ) and ApEn(500,3,0:30)( igh ). The Spea man co ela ion coe icien calcula ed o e DB-CZ-GE o each boxplo is shown. B: Ac i a ion
isoch onic maps co esponding o R1 (below) and R2 ( op). The o o ip is indica ed whe e he colo s con e ge. C: EGM gene a ed by he model in he
a eas o s able o o s and he block o he ime in e al be ween 2 s and 3 s. EGM co esponding o he R1, R2, B1 and plane ac i a ion wa e on a eas. D:
Bipola EGM co esponding o R1 and plane ac i a ion wa e on a ea. ApEn alues o each EGM a e shown.
doi:10.1371/jou nal.pone.0114577.g003
Dynamic ApEn Maps in A ial Fib illa ion
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genic mechanisms besides o o s, should be s udied. In o de o ully alida e he
esul s o ou op imiza ion p ocedu e wi h DB-CZ-GE, al hough good
pe o mance has been achie ed o o o de ec ion in he 3D model, u u e s udies
should in ol e collec ing mo e AF EGM samples om o he da abases in o de o
achie e equally dis ibu ed ac iona ion le els. Addi ionally, eal unipola EGM
mus be included.
In conclusion, we ha e p o ided e idence o pos ula ing dynamic ApEn maps
as a suppo ing ool in AF abla ion p ocedu es. ApEn calcula ion o e a ial EGM
signals can be used o build an elec oana omical map wi h con inuous ApEn
alues ep esen ed in colo s ha can iden i y o o ip loca ions wi hou p e-
speci ying h esholds. This p ope y makes he me hod adap able o speci ic
elec ophysiological cases. A combina ion o all his could help o imp o e
abla ion p ocedu es. We sugges ha dynamic ApEn colo maps could become a
ool o AF o o mapping. The me hodology p oposed he e needs o be alida ed
by expe imen al models and by clinical s udies o e alua e abla ion p ocedu es
guided by dynamic ApEn maps.
Suppo ing In o ma ion
S1 Video. S able o o s. Le : Simula ion o an AF episode induced by six
ansi o y ec opic bea s applied in he os ium o he igh pulmona y ein,
sus ained by mul iple een an wa es. Two o o s can be obse ed: in he
pos e io wall o he le a ia pos e io wall, and in he supe io ca a ein. Righ :
A dynamic ApEn map using op imized pa ame e s. Red a eas co espond o he
ips o o o s R1 and R2.
doi:10.1371/jou nal.pone.0114577.s001 (MP4)
S2 Video. Isoch one map. Isoch one maps o o o s R1 and R2 o he ime
in e al be ween 1500 ms and 2000 ms.
doi:10.1371/jou nal.pone.0114577.s002 (MP4)
S3 Video. Meande ing o o . Le : Simula ion o an AF episode induced by six
ansi o y ec opic bea s applied in he pos e io wall o he le a ium nea o he
igh pulmona y eins, sus ained by mul iple een an wa es. One meande ing
o o can be obse ed in he pos e io wall o he le a ia. Righ : A dynamic
ApEn map using op imized pa ame e s. No e ha , when a plane ac i a ion
wa e on is p esen wi hin he obse a ion a ea, he dynamic ApEn map shows
low alues (g een). Red zones appea when he o o ip is wi hin he obse a ion
a ea (e.g. he ime in e al be ween 2500 ms and 3000 ms).
doi:10.1371/jou nal.pone.0114577.s003 (MP4)
Au ho Con ibu ions
Concei ed and designed he expe imen s: JPU AO CT JS JB. Pe o med he
expe imen s: JPU AO CT VK DN JB. Analyzed he da a: JPU AO CT VK DN AL
JB. Con ibu ed eagen s/ma e ials/analysis ools: VK DN JS TO CS AL. W o e he
Dynamic ApEn Maps in A ial Fib illa ion
PLOS ONE | DOI:10.1371/jou nal.pone.0114577 Decembe 9, 2014 16 / 19

pape : JPU AO CT. D a ed he a icle o e ised i c i ically o impo an
in ellec ual con en : JPU AO CT VK DN JS TO CS AL JB.
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