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Intensity and Dose of Neuromuscular Electrical Stimulation Influence Sensorimotor Cortical Excitability

Abstract

Neuromuscular electrical stimulation (NMES) of the nervous system has been extensively used in neurorehabilitation due to its capacity to engage the muscle fibers, improving muscle tone, and the neural pathways, sending afferent volleys toward the brain. Although different neuroimaging tools suggested the capability of NMES to regulate the excitability of sensorimotor cortex and corticospinal circuits, how the intensity and dose of NMES can neuromodulate the brain oscillatory activity measured with electroencephalography (EEG) is still unknown to date. We quantified the effect of NMES parameters on brain oscillatory activity of 12 healthy participants who underwent stimulation of wrist extensors during rest. Three different NMES intensities were included, two below and one above the individual motor threshold, fixing the stimulation frequency to 35 Hz and the pulse width to 300 µs. Firstly, we efficiently removed stimulation artifacts from the EEG recordings. Secondly, we analyzed the effect of amplitude and dose on the sensorimotor oscillatory activity. On the one hand, we observed a significant NMES intensity-dependent modulation of brain activity, demonstrating the direct effect of afferent receptor recruitment. On the other hand, we described a significant NMES intensity-dependent dose-effect on sensorimotor activity modulation over time, with below-motor-threshold intensities causing cortical inhibition and above-motor-threshold intensities causing cortical facilitation. Our results highlight the relevance of intensity and dose of NMES, and show that these parameters can influence the recruitment of the sensorimotor pathways from the muscle to the brain, which should be carefully considered for the design of novel neuromodulation interventions based on NMES. Insausti-Delgado, A.; López-Larraz, E.; Omedes, J.; Ramos-Murguialday, A.

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Intensity and Dose of Neuromuscular Electrical Stimulation Influence Sensorimotor Cortical Excitability

Author: Insausti-Delgado, A.; López-Larraz, E.; Ramos-Murguialday, A.; Omedes, J.
Year: 2021
DOI: 10.3389/fnins.2020.593360
Source: https://zaguan.unizar.es/record/99752/files/texto_completo.pdf
nins-14-593360 Janua y 15, 2021 Time: 14:6 # 1
ORIGINAL RESEARCH
published: 15 Janua y 2021
doi: 10.3389/ nins.2020.593360
Edi ed by:
Julia S ephen,
Mind Resea ch Ne wo k (MRN),
Uni ed S a es
Re iewed by:
Sidney G osp ê e,
Uni e si y o F anche-Com é, F ance
Dipanjan Roy,
Na ional B ain Resea ch Cen e
(NBRC), India
*Co espondence:
Ainhoa Insaus i-Delgado
ainhoa.insaus i-delgado@uni-
uebingen.de
Special y sec ion:
This a icle was submi ed o
B ain Imaging Me hods,
a sec ion o he jou nal
F on ie s in Neu oscience
Recei ed: 10 Augus 2020
Accep ed: 30 No embe 2020
Published: 15 Janua y 2021
Ci a ion:
Insaus i-Delgado A,
López-La az E, Omedes J and
Ramos-Mu guialday A (2021) In ensi y
and Dose o Neu omuscula Elec ical
S imula ion In luence Senso imo o
Co ical Exci abili y.
F on . Neu osci. 14:593360.
doi: 10.3389/ nins.2020.593360
In ensi y and Dose o Neu omuscula
Elec ical S imula ion In luence
Senso imo o Co ical Exci abili y
Ainhoa Insaus i-Delgado1,2,3*, Edua do López-La az1,4, Jason Omedes5,6 and
Ande Ramos-Mu guialday1,7
1Ins i u e o Medical Psychology and Beha io al Neu obiology, Uni e si y o Tübingen, Tübingen, Ge many, 2In e na ional
Max Planck Resea ch School (IMPRS) o Cogni i e and Sys ems Neu oscience, Tübingen, Ge many, 3IKERBASQUE,
Basque Founda ion o Science, Bilbao, Spain, 4Bi b ain, Za agoza, Spain, 5Ins i u o de In es igación en Ingenie ía
de A agón (I3A), Za agoza, Spain, 6Depa amen o de In o má ica e Ingenie ía de Sis emas (DIIS), Uni e si y o Za agoza,
Za agoza, Spain, 7Neu o echnology Labo a o y, TECNALIA, Basque Resea ch and Technology Alliance (BRTA),
Donos ia-San Sebas ián, Spain
Neu omuscula elec ical s imula ion (NMES) o he ne ous sys em has been ex ensi ely
used in neu o ehabili a ion due o i s capaci y o engage he muscle ibe s, imp o ing
muscle one, and he neu al pa hways, sending a e en olleys owa d he b ain.
Al hough di e en neu oimaging ools sugges ed he capabili y o NMES o egula e
he exci abili y o senso imo o co ex and co icospinal ci cui s, how he in ensi y
and dose o NMES can neu omodula e he b ain oscilla o y ac i i y measu ed wi h
elec oencephalog aphy (EEG) is s ill unknown o da e. We quan i ied he e ec
o NMES pa ame e s on b ain oscilla o y ac i i y o 12 heal hy pa icipan s who
unde wen s imula ion o w is ex enso s du ing es . Th ee di e en NMES in ensi ies
we e included, wo below and one abo e he indi idual mo o h eshold, ixing he
s imula ion equency o 35 Hz and he pulse wid h o 300 µs. Fi s ly, we e icien ly
emo ed s imula ion a i ac s om he EEG eco dings. Secondly, we analyzed he
e ec o ampli ude and dose on he senso imo o oscilla o y ac i i y. On he one
hand, we obse ed a signi ican NMES in ensi y-dependen modula ion o b ain ac i i y,
demons a ing he di ec e ec o a e en ecep o ec ui men . On he o he hand,
we desc ibed a signi ican NMES in ensi y-dependen dose-e ec on senso imo o
ac i i y modula ion o e ime, wi h below-mo o - h eshold in ensi ies causing co ical
inhibi ion and abo e-mo o - h eshold in ensi ies causing co ical acili a ion. Ou esul s
highligh he ele ance o in ensi y and dose o NMES, and show ha hese pa ame e s
can in luence he ec ui men o he senso imo o pa hways om he muscle o he
b ain, which should be ca e ully conside ed o he design o no el neu omodula ion
in e en ions based on NMES.
Keywo ds: neu omuscula elec ical s imula ion (NMES), elec oencephalog aphy (EEG), a e en co ical
ac i a ion, senso imo o oscilla o y hy hm, a i ac emo al
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Insaus i-Delgado e al. NMES Pa ame e s In luence Co ical Exci abili y
INTRODUCTION
Neu omuscula elec ical s imula ion (NMES) is an
elec ophysiological echnique ha consis s o applying elec ical
cu en s on he skin o depola ize mo o and senso y ne es
benea h he s imula ing elec odes (Be gquis e al., 2011). NMES
has been used as a neu oscien i ic ool o s udy senso imo o
neu al mechanisms om he muscles o pe iphe al senso y
ecep o s (mechano ecep o s, nocicep o s, e c.) o he spine
and b ain (Collins, 2007;Ca son and Buick, 2020). NMES has
also been u ilized as a neu o ehabili a i e ool o educe muscle
a ophy, and o imp o e muscle one and mo o unc ion in
pa ien s wi h pa alysis a e s oke (Knu son e al., 2015;Yang
e al., 2019) o spinal co d inju y (SCI) (Pa il e al., 2015).
The wo king p inciple o ehabili a i e NMES is based on
he ollowing: (1) he di ec e ec on muscle one and (2) he
ac i a ion o ecep o s and senso y axons ha send a e en
olleys o he senso imo o co ex, a e being p ocessed by
spinal ne wo ks and subco ical s uc u es.
Nume ous s udies using unc ional magne ic esonance
imaging ( MRI) and nea -in a ed spec oscopy (NIRS) ha e
in es iga ed he ac i i y p oduced by NMES in di e en b ain
s uc u es (Kampe e al., 2000;Blickens o e e al., 2009;I ime-
Nielsen e al., 2012;Schü holz e al., 2012;Weg zyk e al.,
2017). These wo ks demons a ed ha he b ain ac i i y is
p opo ionally inc eased wi h he applied s imula ion in ensi y
(Backes e al., 2000;Smi h e al., 2003;Schü holz e al.,
2012). Recen expe imen s ha e also shown ha pe iphe al
s imula ion can modula e co icospinal exci abili y, measu ed
by mo o e oked po en ials (MEP) (Chipchase e al., 2011;
Veldman e al., 2014). As he s imula ion in ensi y inc eases,
he e is a p og essi e ec ui men o mo e a e en ecep o s
(i.e., cu aneous mechano ecep o s, muscle spindles, and Golgi
endon o gans) ha modula e spinal and co ical ci cui s o a
di e en ex en (Ma iule i e al., 2008;Be gquis e al., 2011;
Golaszewski e al., 2012). I has been p o en ha he a e ence
p o ided by muscle spindles and Golgi endon o gans due
o muscle con ac ion a els h ough he spinal co d o he
soma osenso y co ex and can di ec ly p ojec o he mo o
co ex (Ca son and Buick, 2020). The e o e, he p esence o
absence o muscle con ac ion elici ed by NMES has a di ec
impac on soma osenso y co ex and, indi ec ly, on mo o
co ex exci abili y (Sasaki e al., 2017). The neu al exci abili y
depends on he modula ion o ne ous s uc u es, such as
spinal ne wo ks, in ol ed in he a e en ansmission om he
s imula ed muscle o he b ain.
Al hough he e ec o in ensi y on co ical ac i a ion and
co icospinal exci abili y has been in es iga ed, he dose o
ene gy o he s imula ion has no a ac ed much a en ion
and migh play a pi o al ole in modula ing he ac i i y o
senso y egions. The e is e idence showing ha he numbe
o pe iphe al s imula ion pulses (i.e., dose) o e ime and
he in e -pulse in e al in luence ongoing neu al oscilla ions
and ha e a neu omodula o y e ec on he soma osenso y
co ex a ec ing indi ec ly co icospinal connec i i y (Ni sche
and Paulus, 2000;Schawo onkow e al., 2018;Z enne e al.,
2018). The ne ous sys em main ains i s exci abili y wi hin
an equilib ium ange h ough adjus men s de i ed om he
his o y o neu onal ac i i y, p e en ing excessi e inhibi ion
o acili a ion (Pozo and Goda, 2010). P olonged pe iods o
s imula ion-induced exci abili y/inhibi ion ha e been shown o
ac i a e homeos a ic plas ici y mechanisms ha d i e he sys em
owa d a mo e inhibi ed/exci ed s a e, educing he e ec s o he
s imula ion (Gamboa e al., 2010;And ews e al., 2013). Fu he ,
a p og essi e pe cep ual adap a ion (o educ ion o senso y
esponsi eness) has been e idenced a e p olonged in e als
o pe iphe al ib o ac ile and elec ocu aneous s imula ion
(Leung e al., 2005;Buma e al., 2007;G aczyk e al.,
2018), indica ing a neu al compensa ion a e a pe u ba ion
o he oscilla o y neu al sys em. The e o e, i could be
concei able ha p olonged pe iods o NMES esul in changes
o neu al exci abili y, esul ing in a ebalance o he co ical
esponse along ime.
Al hough mos o he s udies so a ha e used MRI and
NIRS o ack slow b ain co ela es, o TMS-induced MEPs
o asses co icospinal exci abili y, elec oencephalog aphy (EEG)
is a powe ul neu oimaging echnique wi h high empo al
esolu ion ha has been used o s udy senso imo o p ocesses
(including senso y e oked po en ials and hy hms) (Bi baume
e al., 1990;Buzsaki, 2006;Shibasaki and Halle , 2006;Leodo i
e al., 2019). The senso imo o oscilla ions ha mainly comp ise
he olandic alpha [(7–13) Hz] and be a [(14–30) Hz] hy hms
ha e been ho oughly used o s udy co ical in ol emen du ing
senso imo o asks (Ramos-Mu guialday and Bi baume , 2015;
López-La az e al., 2018), being quan i ied as he e en -
ela ed (de)synch oniza ion (ERD/ERS) (P u schelle and Lopes
da Sil a, 1999). Fu he mo e, i has also been used as a
ea u e o neu omodula ion o senso imo o neu al ne wo k
ia p op iocep ion and hap ics (Ray e al., 2020;Sebas ián-
Romagosa e al., 2020). To da e, only a ew s udies ha e epo ed
how oscilla o y ac i i y measu ed wi h EEG is modula ed by
NMES (Vidau e e al., 2016, 2019;Tu-Chan e al., 2017;Co be
e al., 2018). Unde s anding his p ocess is o g ea impo ance
gi en he ele ance o EEG and NMES o neu o ehabili a ion,
especially o EEG-based neu al in e aces. I is impo an o no e
ha , al hough he neu al esponse can be di ec ly in luenced by
e e y s imula ion pa ame e (e.g., equency, pulse wid h, and
pulse wa e o m), we ocused on in es iga ing he in luence o
in ensi y and dose o s imula ion, since hese a e he pa ame e s
ha a e usually pe sonalized o each pa ien .
In his wo k, we acqui ed EEG ac i i y om 12 heal hy
pa icipan s du ing NMES o he w is ex enso muscles a
h ee di e en in ensi ies ( wo below and one abo e he mo o
h eshold) o in es iga e he neu omodula o y e ec o pe iphe al
s imula ion on he ongoing co ical oscilla o y ac i i y, while
he subjec s es ed in a com o able si ing posi ion. Fi s ly,
we wan ed o con i m ha as he in ensi y inc eases, he e is
a p opo ional neu al exci a ion, p obably esul ing om he
ec ui men o mo e a e en ibe s, which p o ide a g ea e
p ojec ion o a e en olleys o he senso y co ex. Secondly, we
wan ed o assess i he dose o s imula ion has an e ec on he
magni ude o neu al exci a ion o e ime, expec ing ha a e
he s imula ion has been p o ided du ing a p olonged ime, he
co ical esponsi eness is lowe .
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MATERIALS AND METHODS
Pa icipan s
Twel e igh -handed heal hy pa icipan s ( ou emales,
age = 27.5 ±3.0 yea s, heigh = 176.3 ±8.6 cm,
weigh = 69.8 ±9.8 kg) we e ec ui ed o pa icipa e in he s udy.
All o hem signed an in o med consen o m. The expe imen al
p ocedu e was app o ed by he E hics Commi ee o he Facul y
o Medicine o he Uni e si y o Tübingen (Ge many).
Pa icipan s we e asked o s ay com o ably sea ed on a chai
wi h hei igh a m es ing on a side able and he hand hanging
wi h he palm acing downwa ds. Neu omuscula elec ical
s imula ion (NMES) elec odes we e placed on he igh -
hand ex enso s (mo e de ailed desc ip ion in “Neu omuscula
Elec ical S imula ion” sec ion), as desc ibed in Figu e 1A. EEG
and muscle ac i i y o wo senso s we e eco ded du ing he
expe imen . The elec ical a i ac eco ded om he muscle
senso s was used o align s imula ion onse du ing he EEG
signal p ocessing.
Expe imen al Design and P ocedu e
The main pu pose o he expe imen was o in es iga e NMES
neu omodula o y e ec s (ins an aneous and cumula i e) on
b ain oscilla o y ac i i y. Wi h his aim, we compa ed he
a e en co ical ac i i y gene a ed by h ee di e en NMES
in ensi ies. Pa icipan s we e passi ely s imula ed, meaning ha
hey we e es ing, and no oli ional mo o command was
gene a ed du ing s imula ion. Each pa icipan unde wen one
session consis ing o nine blocks, each comp ising 18 ials.
One o he h ee NMES in ensi ies was andomly assigned o
each block (de e mina ion o he cu en in ensi ies explained
in “Neu omuscula Elec ical S imula ion” sec ion), esul ing in
h ee blocks pe in ensi y. A eady cue was p esen ed 2.6–
3 s be o e he NMES in e al, which had a andom du a ion
be ween 3.4 and 3.8 s. F om he o se o he NMES o he
nex eady cue, a 3 s in e - ial pe iod was in oduced (see
Figu e 1B). Audi o y cues announced he beginning o each
in e al. The ime be ween blocks was used as b eaks, las ing
a ound 150 s (i.e., 2.5 min). The en i e session including se up
did no exceed 90 min.
Da a Acquisi ion
The elec oencephalog aphic ac i i y was eco ded wi h a
comme cial 32-channel ac iCAP sys em (B ain P oduc s GmbH,
Ge many) and a monopola B ainAmp ampli ie (B ain P oduc s
GmbH, Ge many). The eco ding elec odes we e placed a FP1,
FP2, F7, F3, Fz, F4, F8, FC3, FC1, FCz, FC2, FC4, C5, C3, C1, Cz,
C2, C4, C6, CP5, CP3, CP1, CPz, CP2, CP4, CP6, P7, P3, P4, P8,
O1, and O2, ollowing he in e na ional 10/20 sys em. G ound
and e e ence elec odes we e placed a AFz and Pz, espec i ely.
Muscle ac i i y o he igh o ea m o he pa icipan s
was eco ded by an MR-compa ible B ainAmp ampli ie
(B ain P oduc s GmbH, Ge many) using wo Ag/AgCl bipola
senso s (Myo onics-No omed, Tukwila, Wa, Uni ed S a es).
The senso s we e placed la e ally o he s imula ion pads (see
Figu e 1A), using he igh colla bone as g ound. Bo h EEG
and muscle ac i i y we e synch onously acqui ed a a sampling
a e o 1,000 Hz.
Neu omuscula Elec ical S imula ion
A p og ammable neu omuscula s imula o Bones im (Tecnalia,
Se bia) was used o deli e he s imula ion. The ca hode
(3 ×3.5 cm, sel -adhesi e elec ode) was placed o e he muscles
in ol ed in w is ex ension (ex enso digi o um and ex enso
ca pi ulna is), a one hi d o he dis ance be ween he la e al
epicondyle o he hume us and he Lis e ’s ube cle a he w is .
The anode (5 ×5 cm, sel -adhesi e elec ode) was placed
5 cm dis al o he ca hode. To ensu e he co ec loca ion
o he elec odes, indi idually de e mined o each pa icipan ,
s imula ion abo e he mo o h eshold was applied un il a
comple e w is ex ension was induced.
The equency o he NMES was se o 35 Hz, and he pulse
wid h o 300 µs (Lynch and Popo ic, 2008). The indi idual
in ensi ies o each subjec we e ob ained by a scan o cu en s,
s a ing a 1 mA and inc easing in s eps o 1 mA. The pa icipan s
we e asked o epo he ini ia ion o he ollowing sensa ions:
(i) ingling o he o ea m (i.e., senso y h eshold—STh), (ii)
wi ching o he inge s (i.e., mo o h eshold—MTh), and (iii)
comple e ex ension o he w is (i.e., unc ional h eshold—FTh).
Acco ding o hese h esholds, he h ee NMES in ensi ies ( wo
below and one abo e he mo o h eshold) we e calcula ed,
ollowing he equa ions de ined in he s udy o Smi h e al.
(2003). Low in ensi y was de ined as one hi d be ween he
STh and MTh; medium in ensi y as wo hi ds be ween he
STh and MTh; and high in ensi y as he FTh (see Eq. 1–3 and
Figu e 1C). These in ensi ies we e kep cons an h oughou he
expe imen , and he comple e ex ension o he w is induced
by unc ional s imula ion was isually e i ied. None o he
pa icipan s epo ed pain o any ha m ul e ec due o he
s imula ion.
Low in ensi y =MTh −STh×0.33 +STh (1)
Medium in ensi y =MTh −STh×0.66 +STh (2)
High in ensi y =FTh (3)
Da a P ep ocessing and Analysis
A i ac Remo al P ocedu es
One impo an limi a ion o he quan i ica ion o EEG ac i i y
du ing con inuous s imula ion is he con amina ion o he
signals due o he elec ical cu en s deli e ed o he body.
The EEG is easily pollu ed by hese cu en s, and a i ac
emo al me hodologies a e essen ial o p ope ly es ima e co ical
ac i a ion. Wi h his aim, di e en echniques o con amina ion
emo al in in asi e and non-in asi e b ain ac i i y eco dings
ha e been p oposed, such as in e pola ion, blanking, o linea
eg ession e e ence (LRR) (Wal e e al., 2012;I u a e e al.,
2018;Young e al., 2018). Blanking o he da a is he mos
es ic i e me hod as con amina ed da a a e ejec ed and signals
ha could be o in e es a e neglec ed o u he analysis.
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Insaus i-Delgado e al. NMES Pa ame e s In luence Co ical Exci abili y
Bones im
In ensi y
Senso y
h eshold Mo o
h eshold Func ional
h eshold
33% 66%0
Low in ensi y
Medium in ensi y
High in ensi y
S a ReadyReady
NMES
3 s2.6 ~ 3 s 0.8 s 3.4 ~ 3.8 s
AB
C
FIGURE 1 | Expe imen al design and p ocedu e. (A) Rep esen a ion o he loca ion o s imula ion elec odes and senso s o measu e muscle ac i i y placed on igh
w is ex enso s. (B) Timeline o he h ee phases included in each ial: p epa a ion, NMES, and in e - ial pe iod. (C) De e mina ion o NMES in ensi ies: low in ensi y
as one hi d be ween he senso y h eshold and mo o h eshold, medium in ensi y as wo hi ds be ween he senso y h eshold and mo o h eshold, and high
in ensi y as unc ional mo o h eshold.
Howe e , i he emo al is implemen ed using ha dwa e, he
a i ac has less in luence on he eco e y pe iod o he ampli ie ,
p e en ing i om being sa u a ed and allowing he use o o he
me hods o compensa e o he missing da a (Ken and G ill,
2012). Ano he app oach is o linea ly in e pola e he co up ed
da a, connec ing he las poin be o e he a i ac and he i s
poin a e he a i ac . Howe e , in e pola ion induces a bias
in he es ima ion o powe spec um o he signals (Wal e
e al., 2012). LRR e- e e ences he signals h ough weigh s ha
a e assigned o each channel. The weigh s a e calcula ed in a
aining block acco ding o he noise o each channel gene a ed
by he elec ical s imula ion. This me hod e ec i ely educes
a i ac s, bu i ixes he weigh s and assumes no changes in
channel noise du ing he in e en ion. So a , he easibili y
o his me hod has only been p o en in in asi e eco dings
(Young e al., 2018), in which impedances a e less likely o
change wi hin sessions and a e mo e simila among channels
(Ball e al., 2009). No mally, impedances de e io a e and noise-
in luence inc eases h oughou an EEG session, complica ing
he implemen a ion o LRR in non-in asi e eco dings o b ain
ac i i y. The e o e, we implemen ed an al e na i e wo-s ep
a i ac emo al me hod and demons a ed i s easibili y. The aw
EEG signals we e p e-p ocessed using cus om-de eloped sc ip s
in MATLAB (Ma hWo ks, Na ick, MA, Uni ed S a es).
Channel emo al based on powe -line noise
Du ing an EEG session, pa icula ly du ing se up and du ing
pe iods be ween expe imen al blocks, special ca e is equi ed
o main ain EEG signal clean (i.e., aw da a inspec ion and
impedance check). Howe e , ou empi ical expe ience
shows ha , some imes, ce ain EEG elec odes p esen
highe con amina ion due o he s imula ion han o he s
(see Figu e 2A). These elec odes p esen b oadband a i ac s
ha impede u he analyses e en a e applying he median
il e p ep ocessing desc ibed below. We hypo hesized ha his
e ec migh be due o deg aded impedances, which occasionally
de e io a e e en when du ing he se up we e se below 5 kOhm.
Despi e we did no s o e he impedances o each elec ode o
check his and disca d he elec odes wi h high impedance, we
idea ed an au oma ized me hod o de ec and disca d hem
o line. This way, we could au oma ically elimina e con amina ed
channels wi hou he human bias ha would cons i u e a
manual ejec ion.
Ha ing high impedance be ween he eco ding elec ode and
he skin esembles an open ci cui , whe e he elec ode beha es
like an an enna and cap u es ou side elec ic equencies (like he
powe -line noise). Ou me hod exploi s his e ec and iden i ies
he EEG elec odes wi h unusually high powe -line noise (50 Hz
in Eu ope). Since all he elec odes should be app oxima ely
equally exposed o elec omagne ic signals a 50 Hz, we assume
ha e y high powe a his equency is an indi ec indica o
o high skin-elec ode impedance. The p ocedu e was applied
block-wise, meaning ha i was used o de ec and emo e
con amina ed channels wi hin each indi idual EEG block. The
EEG ac i i y was high-pass il e ed a 0.1 Hz wi h a 4 h-o de
Bu e wo h. The powe spec al dis ibu ion a 48–52 Hz was
es ima ed using Welch’s me hod, a e aging he pe iodog am
o 1 s Hamming windows wi h 50% o e lapping. The powe
mean and s anda d de ia ion (SD) o all he EEG channels we e
calcula ed om all ials in each block. Channels whose powe
was highe han 4 SD abo e he mean we e disca ded om ha
speci ic block. The emaining channels we e used o e-compu e
he mean and SD. The p ocedu e was i e a i ely epea ed un il no
channels exceeded he ejec ion h eshold (see Figu e 3 dashed
box, Supplemen a y Figu es 1,2, and Supplemen a y Table 1).
Median il e ing o emo al o elec ical s imula ion
con amina ion
I is well known ha applying elec o-magne ic cu en s o
s imula e he neu al sys em can in oduce undesi ed noise o
he eco dings. The NMES con igu a ion used in his s udy
in oduces la ge peaks o sho la ency (∼5 ms) o he eco ded
EEG signal. The e o e, median il e ing was used o minimize
he NMES-induced a i ac s (Insaus i-Delgado e al., 2017). This
il e is sui ed o elimina e high-ampli ude peaks om a ime
se ies (Gallaghe and Wise, 1981) and can emo e he sho -
la ency high-ampli ude a i ac s caused by he NMES. A sliding
window o 10 ms was applied o he EEG signal in s eps o one
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Insaus i-Delgado e al. NMES Pa ame e s In luence Co ical Exci abili y
0123-1-2-3 44- Time (s)
C3
C1
Cz
CP3
CP1 120 µV
Con amina ion o channels wi h bad impedances
Time (s)
2.10 2.12 2.14 2.16 2.18 2.20
C1
NMES a i ac emo al by median il e
Raw signal
Median il e ed
15 µV
AB
FIGURE 2 | Cha ac e iza ion o con amina ion induced by NMES. (A) EEG o a ep esen a i e ial showing non-con amina ed channels (C3, C1, CP3, and CP1) and
one con amina ed channel (Cz) du ing high-in ensi y s imula ion. Channels wi h bad impedances a e mo e p one o be con amina ed by elec ical s imula ion.
(B) Zoom in 100-ms segmen o a ep esen a i e EEG ial in a non-con amina ed channel ha p esen s NMES a i ac s ( ed line). The e ec o s imula ion a i ac s is
minimized by median il e (g een line).
Time- equency
analysis
HP il e 0.1 Hz
Powe o EEG
channels [48-52] Hz
Compu e mean and SD
powe o e all
channels
Powe EEG
Ch > Mean
powe + 4SD ?
EEG channels wi h
good impedances
Disca d EEG
channel
YES
NO
Quan i ica ion o b ain oscilla o y ac i i y
Es ima ion o powe
in alpha (7-13) Hz
and be a (
14
-30) Hz
Non-s imula ion (-3, -1) s
Low NMES (0.5, 2.5) s
Med. NMES (0.5, 2.5) s
High NMES (0.5, 2.5) s
Raw da a
Channel emo al
Median il e
BP il e
0.1-45 Hz
T ial ex ac ion
(-4, 4) s
Common a e age
e- e e encing
Subsampling o
100 Hz
FIGURE 3 | Flowcha wi h he s eps o he quan i ica ion o b ain oscilla o y ac i i y. The whole se o da a is i s ly p ep ocessed by a wo-s ep p ocedu e based on
channel emo al and median il e ing. In his le el, channels wi h bad impedances and a i ac s due o elec ical s imula ion a e emo ed. Then, he emaining clean
da a a e il e ed and di ided in o ials. Finally, powe is es ima ed in alpha (7–13) Hz and be a (14–30) Hz bands o non-s imula ion [(−3, −1) s] and NMES [(0.5, 2.5)
s] in e als, being he baseline (−2.5, −1.5) s.
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Insaus i-Delgado e al. NMES Pa ame e s In luence Co ical Exci abili y
sample, p o iding as ou pu he median alue o each window.
We selec ed a 10 ms window as i ully co e s he elec ical
a i ac . This il e p oduces a equency-dependen a enua ion
ha ollows an exponen ial unc ion om 0 o 100 Hz (i.e., he
equency wi h a pe iod ha comple ely i s wi hin he 10 ms
window), leading o low a enua ion a low equencies and a
comple e a enua ion a 100 Hz (Supplemen a y Figu e 3). Wi h
his window size, he a enua ion o he signal a 10 Hz, 20 Hz,
and 30 Hz is 1.28%, 4.89%, and 10.90% espec i ely. The ela i ely
low a enua ion a low equencies makes his me hod sui able
o analyzing alpha and be a senso imo o oscilla ions. Figu e 2B
displays a zoomed segmen o 100 ms o ac i i y, showing he
e ec o he median il e on he s imula ion a i ac s.
Quan i ica ion o B ain Oscilla o y
Ac i i y
A common a e age e e ence (CAR) was applied o he EEG
signals. The e- e e enced signals we e band-pass il e ed a 0.1–
45 Hz using a 1s -o de Bu e wo h il e . Each block was
immed down o (18×) 8-s ials, om -4 o + 4 s, being 0 he
beginning o he s imula ion. The ials we e down sampled a
100 Hz, and hose belonging o he same le el o NMES in ensi y
we e pooled oge he .
The quan i ica ion o co ical ac i i y was pe o med by
e alua ing he spec um di e ences o he senso imo o hy hms,
by means o he alpha and be a e en - ela ed (de)synch oniza ion
(ERD/ERS), i.e., dec ease o inc ease in powe gene a ed by
an e en compa ed o a baseline (P u schelle and Lopes da
Sil a, 1999). La ge ERD alues (i.e., mo e nega i e powe alues)
ep esen s onge co ical ac i a ion compa ed o baseline
ime in e al, as i ep esen s disinhibi ion/exci a ion o neu al
popula ion ac i i y (Ri e e al., 2009). Fo he quan i ica ion
o b ain ac i i y, we used he FieldT ip oolbox1 o MATLAB.
Time- equency maps we e calcula ed using Mo le wa ele s in
he equency ange om 1 o 45 Hz, wi h a esolu ion o 0.5 Hz.
The powe change was compu ed as he pe cen age o inc ease o
dec ease in powe (i.e., ERS o ERD) wi h espec o he baseline
[(−2.5, −1.5) s], whe e Pj ep esen s he signal powe a he j h
sample, as desc ibed in Eq. 4.
ERD/ERSj(%)=Pj−Baseline
Baseline ×100 (4)
F om he ime- equency maps, we calcula ed he senso imo o
a e aged changes in powe in alpha (7–13) Hz and be a (14–
30) Hz bands o non-s imula ion [(−3, −1) s] and NMES [(0.5,
2.5) s] in e als, using as baseline he (−2.5, −1.5) s in e al
(see Figu e 3). The NMES pe iod was de ined as s a ing a
0.5 s o a oid po en ial bias and in luence o he s imula ion
onse like e en - ela ed b ain po en ials (e.g., soma osenso y
e oked po en ial) a = 0. Fo he opog aphical inspec ion
and he desc ip i e analysis o he en i e b ain ac i i y, all
EEG channels we e analyzed indi idually. Fo he quan i a i e
analysis, we calcula ed he mean change in powe o channels
C1, C3, CP1, and CP3 (i.e., a ea o e he senso imo o co ex
1h p:// ield ip oolbox.o g/
ep esen ing he igh o ea m, con ala e al hemisphe e o he
s imula ed limb), since we conside ed ha a e aged alues o e
hese elec odes could be e quan i y he o e all changes in he
senso imo o a eas.
S a is ical Analysis
The s a is ical es s we e pe o med in IBM SPSS 25.0 S a is ics
so wa e (SPSS Inc., Chicago, IL, Uni ed S a es) and MATLAB.
We used he Shapi o–Wilk es o de e mine he no mali y
o he da a. Acco dingly, a mul i a ia e analysis o a iance
(MANOVA) o epea ed measu es was pe o med o ind
di e ences in he dependen a iables, alpha and be a ERD/ERS,
wi h NMES in ensi y ( ou le els: no s imula ion, low-, medium-,
and high-in ensi y s imula ion) as wi hin-subjec ac o . In o de
o de e mine he o igin o he signi ican e ec , pos hoc es s wi h
Bon e oni co ec ion we e pe o med.
In o de o analyze whe he NMES can induce a dose-
e ec , we s udied he ERD/ERS changes o e ime. Fo ha , we
compu ed he alpha and be a ERD/ERS o each single ial (i.e.,
in Eq. 4, Pjwas he alpha/be a powe o each ial du ing he
NMES pe iod, and he baseline was calcula ed om he g and
a e age o all he ials o each in ensi y). A linea eg ession
was es ima ed o he ERD/ERS alues o e ials o he wo
equency bands (i.e., alpha and be a) and he h ee NMES
in ensi ies (i.e., low, medium, and high). Co ela ion be ween
ERD/ERS and sequence o ials we e calcula ed using Pea son’s
co ela ion coe icien o s udy s imula ion e ec s o e ime.
RESULTS
E ec o A i ac Remo al
The p e-p ocessing o he da a elimina ed sa is ac o ily he
elec ical noise con amina ion coming om he pe iphe al
elec ical s imula ion. I educed he e ec o he a i ac s o an
ex en ha allowed us o pe o m EEG spec al analysis o he
b ain oscilla o y ac i i y.
Channels wi h good impedances a e also in luenced by he
elec ical s imula ion a i ac ha is in oduced in o he signal
as la ge peaks. Figu e 2B illus a es in a 100 ms segmen o
a ep esen a i e ial how he median il e deals wi h hese
undesi ed a i ac s. To p o e he e icacy o he me hod, we
ocused on he wo s -case scena io, as he con amina ion is
la ge o highe s imula ion in ensi ies. This e ec can be
obse ed in Figu e 4, which depic s he EEG ime- equency
ac i i y a he di e en NMES in ensi ies including a i ac s and
a e he median and spa ial il e s a e applied. The NMES
gene a es an inc ease o powe , o ERS, a ound 35 Hz (i.e., he
s imula ion equency), which inc eases as he NMES in ensi y is
inc emen ed (Figu e 4, le column). This powe inc ease in high-
be a/low-gamma band due o s imula ion a i ac was elimina ed
o all in ensi ies a e median il e ing. Applying he median il e
did no change he powe in alpha and be a equencies be o e
he s imula ion onse ( = 0 s), bu elimina ed he ERS du ing
he s imula ion pe iod, minimizing he a i ac s and e ealing he
alpha and be a modula ion. The common a e age e- e e ence
(CAR) a e median il e ing enhanced he powe dec ease o
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Insaus i-Delgado e al. NMES Pa ame e s In luence Co ical Exci abili y
Wi hou median il e Wi h median il e
5
15
25
35
45
0123-1-2-3 Time (s)
F equency (Hz)
5
15
25
35
45
0123-1-2-3 Time (s)
F equency (Hz)
50400102030-50 -40 -30 -20 -10
ERD/ERS (%)
5
15
25
35
45
0123-1-2-3 Time (s)
F equency (Hz)
5
15
25
35
45
0123-1-2-3 Time (s)
F equency (Hz)
5
15
25
35
45
0123-1-2-3 Time (s)
F equency (Hz)
5
15
25
35
45
0123-1-2-3 Time (s)
F equency (Hz)
Medium
in ensi y
Low
in ensi y
High
in ensi y
5
15
25
35
45
0123-1-2-3 Time (s)
F equency (Hz)
5
15
25
35
45
0123-1-2-3 Time (s)
F equency (Hz)
5
15
25
35
45
0123-1-2-3 Time (s)
F equency (Hz)
Wi h median il e and CAR
FIGURE 4 | Compa ison o co ical ac i a ion a e median and spa ial il e ing. Time- equency maps a e aged o e all pa icipan s, ep esen ing ERD/ERS, o he
a e age o channels (C3, C1, CP3, and CP1) loca ed o e he con ala e al senso imo o co ex o he s imula ed limb. A e aged ime- equency maps wi hou
median il e (le column), wi h median il e (cen e column), and wi h median and CAR il e ( igh column) a e emo al o con amina ed channels. Rows show he
di e en NMES in ensi ies: high (uppe ow), medium (middle ow), and low in ensi y (lowe ow). The pe cen age o ERD/ERS is compu ed acco ding o he baseline
(−2.5, −1.5) s. Time 0 s is aligned wi h he onse o he s imula ion.
he bands o in e es o e e y NMES in ensi y, as i does wi h
non-con amina ed EEG (Wolpaw e al., 2002). Rega dless o he
in ensi y deli e ed, he ini ia ion o he s imula ion gene a ed
ime- and phase-locked ac i i y (i.e., e en - ela ed po en ials—
ERP), p esumably due o he senso y p ocessing o he NMES
(Reynolds e al., 2015). This can be seen as powe inc ease a low
equencies (1–5 Hz).
In luence o S imula ion In ensi y on
Co ical Ac i a ion
To analyze he in luence o s imula ion in ensi y on co ical
ac i a ion, we compa ed he changes in b ain oscilla o y
ac i i y in ou condi ions: non-s imula ion, low-, medium-,
and high-in ensi y s imula ion (see opoplo s o alpha and be a
hy hms in Figu e 5). Topog aphic maps o non-s imula ion
condi ion we e calcula ed using he in e al (−3, −1) s p io o
he s imula ion, while he o he condi ions we e ex ac ed om
he in e al (0.5, 2.5) s a e s imula ion onse . An inc emen
o he s imula ion in ensi y esul ed in an inc easing ERD (i.e.,
la ge dec ease in powe ) in bo h equency bands o e he
senso imo o co ex as expec ed (Backes e al., 2000;Smi h e al.,
2003;Schü holz e al., 2012), while occipi al a eas showed idling
ac i i y. A high-in ensi y s imula ion, he senso imo o co ex
o bo h hemisphe es p esen ed a dec ease o powe , being mo e
p onounced in he con ala e al hemisphe e, as demons a ed
in p e ious wo k s udying b ain oscilla o y signa u es o mo o
asks (Ramos-Mu guialday and Bi baume , 2015).
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Insaus i-Delgado e al. NMES Pa ame e s In luence Co ical Exci abili y
Medium in ensi y y isne nihgiHy isne niwoLNon-s imula ion
Alpha band
(7-13 Hz)
40020-40 -20
ERD/ERS (%)
*
**
0
-10
-20
ERD/ERS (%)
-30
Non-
S im. Low Med. High
0
-10
-20
ERD/ERS (%)
-30
Non-
S im. Low Med. High
*
**
Be a band
(14-30 Hz)
FIGURE 5 | Compa ison o co ical ac i a ion o di e en s imula ion in ensi ies o alpha and be a band EEG ac i i y. Topog aphic maps, a e aged o e all
pa icipan s, showing ERD/ERS o non-s imula ion pe iods (−3, −1) s and NMES pe iods (0.5, 2.5) s belonging o each in ensi y (i.e., low, medium, and high) o
alpha (uppe ow) and be a (lowe ow) equency bands. Ba g aphs show he mean pe cen age o ERD/ERS a e aged om channels (C3, C1, CP3, and CP1) o
each in ensi y and equency band. The s a is ically signi ican di e ences be ween pai s a e exp essed wi h ho izon al lines and s a s. The pe cen age o ERD/ERS is
calcula ed wi h espec o he baseline (−2.5, −1.5) s. The signals a e p ocessed using he wo-s ep p ocedu e (i.e., emo al o con amina ed channels and median
il e ) and a CAR.
Ou MANOVA analysis e lec ed a signi ican e ec
o in ensi y on alpha and be a ERD [F(6, 86) = 4.356,
p= 0.001]. Righ mos panels in Figu e 5 display he
esul s o he pos hoc compa isons. Fo bo h alpha and
be a, he e was a signi ican ly highe ERD (i.e., mo e
nega i e powe alues) induced by high-in ensi y NMES
compa ed o es (p= 0.004 o alpha, p<0.001 o be a),
o low-in ensi y NMES (p= 0.013 o alpha, p= 0.004
o be a), and o medium in ensi y (p= 0.045 o alpha,
p<0.001 o be a).
S imula ion Dose-E ec
To s udy he in luence o s imula ion dose on co ical
ac i i y, we compu ed he ERD/ERS o each single ial and
pe o med a eg ession in ime wi hin session appending
same s imula ion in ensi y blocks in o de o appea ance
(blocks o di e en in ensi ies we e p esen ed andomly).
Figu e 6 shows he a e age ERD/ERS o all pa icipan s in
bo h equency bands du ing he 54 ials (3 blocks ×18
ials, see e ical yellow lines) o each in ensi y and a
linea eg ession o i hem. We also pe o med eg essions
o e ime wi hin each block wi h consecu i e ials (see
Supplemen a y Figu e 4).
The i s hing we obse ed is a clea modula ion based on
s imula ion, educing i s a iabili y wi h s imula ion ampli ude.
Low and medium in ensi ies caused a signi ican educ ion
o alpha ERD o e ime (p= 7.8e-4 o low; p= 0.0053
o medium). In con as , high in ensi y caused a signi ican
enhancemen o be a ERD o e ime (p= 5.12e-5). Fu he mo e,
as can be seen in Figu e 6, we obse ed ha in e e y
block (sepa a ed by yellow e ical lines), he e is a educ ion
o he ERD (inc ease o powe plo ed as linea eg ession
in Supplemen a y Figu e 4) p og essi ely induced pe ial
om he i s o he las ial. The i s ial o he
new block p esen ed a la ge ERD (dec ease o powe ) in
compa ison o he ERD o he las ial o he p e ious block
(i espec i e o he s imula ion in ensi y and o de o he block
wi hin he session).
DISCUSSION
This s udy demons a ed he signi ican e ec s o a i ac s,
in ensi y, and dose o neu omuscula elec ical s imula ion
(NMES) o he uppe limb on he ongoing b ain oscilla o y
ac i i y eco ded using EEG. Fi s o all, we deal wi h he
issue o a i ac emo al o allow accu a ely es ima ing he
co ical oscilla o y ac i i y. Reco dings o b ain ac i i y a e easily
pollu ed, especially when elec ical s imula ion in e ac ing wi h
he ne ous sys em is concu en ly used. This con amina ion
can nega i ely a ec he signal- o-noise a io, co e ing he b ain
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Insaus i-Delgado e al. NMES Pa ame e s In luence Co ical Exci abili y
Low in ensi y
0
20
-20
40
-40
ERD/ERS (%)
0504030102
Numbe o ial
y isne nihgiHy isne nimuideM
Alpha band
(7-13 Hz)
0
20
-20
40
-40
ERD/ERS (%)
0504030102
Numbe o ial
0
20
-20
40
-40
ERD/ERS (%)
0504030102
Numbe o ial
0
20
-20
40
-40
ERD/ERS (%)
0504030102
Numbe o ial
0
20
-20
40
-40
ERD/ERS (%)
0504030102
Numbe o ial
0
20
-20
40
-40
ERD/ERS (%)
0504030102
Numbe o ial
Be a band
(14-30 Hz)
R = -0.5222, m = -0.2374, p = 5.12e-05R = -0.1305, m = -0.0687, p = 0.3469R = 0.2189, m = 0.1025, p = 0.1116
R = 0.4433, m = 0.4564, p = 7.8e-04 R = 0.3740, m = 0.3294, p = 0.0053 R = 0.0931, m = 0.0610, p = 0.5030
FIGURE 6 | Compa ison o co ical ac i a ion o e ials o alpha and be a bands. The co ical ac i i y du ing NMES pe iod [(0.5, 2.5) s] quan i ied as ERD/ERS o e
he 54 ials o each s imula ion in ensi y, di ided in o blocks by e ical yellow lines, and a e aged o all he pa icipan s. The pe cen age o ERD/ERS is calcula ed
acco ding o he baseline (−2.5, −1.5) s. Di e en in ensi ies a e compa ed in columns: low (le ), medium (middle), and high ( igh ). Alpha (uppe ow) and be a
(lowe ow) equency bands a e desc ibed. Signi ican co ela ions be ween ERD/ERS and sequence o ials o e session a e ep esen ed wi h black solid linea
eg essions.
ac i i y. Ou indings e idenced ha he median il e enhanced
he de ec ion o senso imo o oscilla o y ac i i y a e emo ing
s imula ion a i ac s.
A e he EEG da a was cleaned, especially o NMES-
induced a i ac s, we analyzed he modula ion o alpha and be a
oscilla ions p oduced by he s imula ion. Powe supp ession,
o desynch oniza ion, o hese equencies has been associa ed
wi h co ical exci a ion, whe eas synch oniza ion e lec s a
s a e o inhibi ion (Klimesch e al., 2007). Du ing high-
in ensi y NMES, he induced desynch oniza ion in alpha
and be a was signi ican ly la ge han du ing s imula ion
a low o medium in ensi ies o no s imula ion. While
below-mo o - h eshold s imula ion in ensi ies only ac i a e
cu aneous mechano ecep o s (e.g., Pacinian co puscles and
Me kel disks) and senso y axons, s imula ion abo e he
mo o h eshold also ec ui s p op iocep i e ecep o s (e.g.,
muscle spindles, Golgi endon o gans, and join a e en s)
(Ma iule i e al., 2008;Be gquis e al., 2011;Golaszewski
e al., 2012). I has been p oposed ha muscle spindles
ansmi inpu s o he spinal co d and can di ec ly in luence
he mo o co ex (M1) h ough he a ea 3a, while he
p ojec ions om a ea 3b ac i a ed by cu aneous eedback
o M1 a e less likely o happen (Ca son and Buick, 2020).
We can he e o e assume ha high-in ensi y NMES leads
o highe neu al exci a ion, p obably by ec ui ing a la ge
numbe o ecep o s de i ed om muscle con ac ions, in
addi ion o he cu aneous and senso y ibe a e ence ha is
also engaged in senso y- h eshold s imula ion, and ha he
ec ui men o muscle spindles esul s in ac i a ion o M1 ia
a ea 3a o he soma osenso y co ex (S1) (Schab un e al.,
2012;Ca son and Buick, 2020). These esul s o in ensi y-
dependen b ain ac i a ion a e in line wi h co icomuscula
esponses (Sasaki e al., 2017), me abolic esponses eco ded
by unc ional magne ic esonance imaging ( MRI) (Backes
e al., 2000;Smi h e al., 2003) and nea -in a ed spec oscopy
(NIRS) (Schü holz e al., 2012), which demons a ed a di ec
quan i a i e associa ion wi h s imula ion in ensi y. No ewo hy,
ou esul s showed ha he co ical ac i i y measu ed wi h EEG,
quan i ied as e en - ela ed (de)synch oniza ion (ERD/ERS),
du ing low and medium in ensi ies was no signi ican ly
di e en o no s imula ion. This sugges s ha below-mo o -
h eshold NMES migh no ec ui enough a e en ibe s o
induce signi ican co ical modula ion and ha mo e a e ence
(p obably h ough muscle con ac ion, p op iocep ion due
o he mo emen , and a la ge numbe o senso y ibe s
ec ui ed) is equi ed o ansmi mo e in o ma ion ha
eaches he b ain and is measu able in he EEG a he
analyzed equencies.
I is well known ha du ing olun a y mo emen , a
s onge co ical ac i a ion is seen in alpha han in be a
(López-La az e al., 2014;Ramos-Mu guialday and Bi baume ,
2015). Such modula ion in alpha and be a co ical ac i i ies
has been ela ed o he con ol o op-down and bo om-
up neu al p ocesses, sugges ing i s ole in he in eg a ion
F on ie s in Neu oscience | www. on ie sin.o g 9Janua y 2021 | Volume 14 | A icle 593360