SensorsandActuatorsAxxx (2011) xxx–xxx
ContentslistsavailableatSciVerseScienceDirect
Sensors
and
Actuators
A:
Physical
j our na l h o me p a g e :w w w . e l s e v i e r . c o m / l o c a t e / s n a
A
3-axis
accelerometer
and
strain
sensor
system
for
building
integrity
monitoring
J.
Santana
a,∗, R.
van
den
Hoven
a, C.
van
Liempd
a, M.
Colin
b, N.
Saillen
c,
D.
Zonta
d,
D.
Trapani
d,
T.
Torfs
e,
C.
Van
Hoof
a,eaimec-HolstCentre,Eindhoven,TheNetherlands bMEMSCAP,Grenoble,France
cThermoFisherScientific,Enschede,TheNetherlands dUniversityofTrento,Italy
eIMEC,Leuven,Belgium
a
r
t
i
c
l
e
i
n
f
o
Articlehistory: Received9August2011 Receivedinrevisedform 10November2011 Accepted11November2011 Available online xxx Keywords: Signal-to-Noiseratio Linearity Bandwidth Sensitivity
Integratednumberofpulses Residualmotion
a
b
s
t
r
a
c
t
AnUltra-Low-PowerreadoutarchitectureforcapacitiveMEMS-basedaccelerometersandstrainsensors
ispresented.Thesystemcanreadbothaccelerometersandstrainsensorsinahalf-bridgeconfiguration.
AnaccurateVerilogAmodelofthesensorwasmadetoimprovesimulations.Thegainofthesystemis
controlledbyintegratingpulsesfromtheexcitationcircuitallowingaccuratecontrolofthe
Signal-to-Noiseratio.AFigure-of-Meritof4.41×10−20F√(W/Hz)wasachievedforasensorrangeof±2.0gand
±20,000 overa100Hzbandwidth.Aminimumof440nWpowerconsumptionwasrecorded.Residual
motionartifactsarealsocancelledbythesystem.
© 2011 Elsevier B.V. All rights reserved.
1. Introduction
Anaccuratesensingofsignalsrequiresinnovative,flexibleand powerefficientreadoutarchitectures. Infieldssuchas building integritywhichuseawiderangeofcapacitiveMEMS/NEMS-based devices,suchasaccelerometersandstrainsensorswithdifferent actuationvoltages,sensitivitiesandresolutions,thespecifications ofthesensorandsystemareincreasinglydemanding.Resolutions of1mgand10arerequiredfortheaccelerometerandstrain sen-sorrespectivelyandarangeof±2.0gand±20,000overa100Hz bandwidthtosenseaccelerationsandstresses.Thisisessentialfor theassessmentofstructuresduringandafterseismicevents.
ThisworkintroducesauniqueUltra-Low-Powersystemwhich canbeappliedtoMEMS-basedcombfingercapacitive accelerome-tersorstrainsensorsinahalf-bridgeconfiguration[1].Anaccurate behavioralmodelofthesensor(inVerilogAlanguage)wasmade inordertosimulatethefullsystemandimproveitsperformance. In comparison with current modulation–demodulation readout techniquesthegainofthesystemcanbesetbythenumberof inte-grationpulsesNcomingfromtheexcitationvoltage,optimizing
∗ Correspondingauthor.Tel.:+31404020548;fax:+31404020699. E-mailaddress:juan.santana@imec-nl.nl(J.Santana).
thenSNRandbandwidthwithpower.Inadditionthearchitecture suppressesmotionartifacts[2,3]suchasresidualmotion.
2. Sensors
Theaccelerometersensorconsistsof2transversecombfinger structures(XandYaxis)and,apendulatingonefortheZaxis(Fig.1). Thesensorsare madeusinga capstructure (Fig.2), its pur-poseistwofold;itprotectstheMEMSstructureandalsoformsthe counterelectrode fortheZsensor.Innovativecapthrough con-nectionswereused.ThecapitselfismountedtotheMEMSwafer byusingametal–siliconeutecticbondingprocesses.Themetalfor thesealingringisalsousedtorealizetheelectricalconnections betweenthecapandtheMEMSwafer.Theaccelerometerwas fab-ricatedwithasurfacemicro-machinedprocessfromaSOIwafer 85mthick.Thesensorhas78fingerswithatotalsensitivityof 2.02pF/g.TheZsensorhasanareaof2.17mm2perplate.
The main tradeoff in thedesign of theaccelerometer is the sensitivity–bandwidth–linearityinallthreeaxes,achallengefor thedesigngiventhedifferentusedstructures.
Thestrainsensorisalongitudinalcombfingercapacitor(Fig.3). Thesensorconsistsofthreeparts:theconnectorarea(for connec-tiontothereadout),theflexiblearea(tosustainthestrainandstress ofthebars)andthesensorarea(theactivedevice).Thestrainsensor 0924-4247/$–seefrontmatter © 2011 Elsevier B.V. All rights reserved.
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Fig.1.3-Axisaccelerometerarrangement.
Fig.2.Crosssectionoftheaccelerometersensor.
Fig.3.3Drepresentationofthestrainsensor.
fabricationusesaSOIwaferwitha500mthickhandle,50m thickfingersand2mthickoxidelayerwith400fingersinthe sensorandithasasensitivityof0.133fF/.
Twoanchorswereetched-outofthesurfacetocreatethe neces-saryclampstoattachthesensortotherebarofapillar.Thefingers areprotectedwitha borosilicateclasscap.Thespecificationsof theMEMS-basedsensorsusedinthisworkaregiveninTable1. Thevoltagevs.frequencyresponseoftheaccelerometeras func-tionofpressureisshowninFig.4.Theplotshowsthetransition oftheaccelerometerfromanover-dampedsystem(at820Torr)to anunder-dampedsystem(at3Torr).Thetemperaturedependence oftheaccelerometerandstrainsensoriscompensatedbyusinga temperaturesensorclosetotheaccelerometer/strainsensorand usinglookuptablesforcalibration.Nolongtermdriftisexpected becauseofthegoodagingpropertiesofsiliconinthecapwafer. Fineleakscouldappearinthebondinglayerswhichwillmakethe
Table1
Accelerometerandstrainsensorspecifications.TheX,YaxissensorsandZaxisare givenseparate.
Parameter Accelerometer Strainsensor
Basic 20pF(X,Y) 5.3pF
Capacitance 20pF(Z)
0.34mg(X,Y) –
0.5mg(Z)
Mechanicalsensitivity 0.4–0.06m/g 3nm/ Electricalsensitivity 0.23–2.02pF/g(X,Y) 0.133fF/
0.38–0.94pF/g(Z)
Resonant 785–2080Hz(X,Y) 56kHz
Frequency 780–1015(Z)
Pull-involtage 2.3–5.4V(X,Y) –
0.95–1.3V(Z)
Fingergap 3m 4m
pressuretoriseinsidetheMEMScavitybuttheseissuesarebeyond thescopeofthepaper.
Fig.5 showsthefabricatedsensorsandthereadoutASIC.As mentionedinpreviousparagraphsthesamereadoutASICisused forboththeaccelerometerandstrainsensors,makingthisa cost-effectivesolutionwhencomparedtoothersystems.
3. Behavioralmodelofthesensor
AsmentionedinSection1anaccuratemodelofthesensoris necessaryinordertooptimizethedesignofthereadout.Asthe trendforlow-powercontinuestorequirepowersavingsystems anoptimumtrade-offbetweensensorsandreadoutisnecessary toreachsuchdemandingexpectations,thereforeaccurate mod-elsofthesensorswhichcanbeusedalonginthetransistor-level simulationsarerequired.Suchmodelshavebeenknownfor sev-eralyearsandinseveralforms,look-uptables,behavioralmodels, macro-models,etc.Inthisstudyabehavioraldescriptionlanguage waschosentomodelthesensor,namelyVerilogA,mainlybecause itisatoolincludedintheuseddesignenvironment.
Avariablecapacitorwiththreeterminalswasmadeto simu-latethesensors;thethirdterminalsimulatesthedisplacementof themasswhenanexternalforceisappliedtotheaccelerometer, suchasthatcomingfromanearthquake,orstressinthecaseofthe stresssensor.Ineithercasethemodelcanbeeasilycustomizedto eachsensor,aparameterizedmodelwasdevelopedsotobeeasily adaptedtodifferentrequirements.
J.Santanaetal./SensorsandActuatorsAxxx (2011) xxx–xxx 3
Fig.5.Microphotographoftheaccelerometer,strainsensorandreadoutASICchip.
4. Readoutarchitecture
Thereadoutarchitectureofthesystemhasbeendescribed else-where[10].Itsmaincharacteristicsaresummarizedinthenext paragraphs.Theprincipleofoperationisbasicallytheonedepicted inFig.6.Whenanaccelerationforceappearsinthesensor,Fig.6(a), theanti-phaseactuationvoltagesappliedtothecapacitorsshown inFig.6(b)aremodulated.Currentpulsesflowintwodirections,as showninFig.6(c).AteveryrisingedgetheswitchesS1andS2are openwhiletheINTEGRATEswitchisclosed(Fig.7).
Thecurrent pulseis integrated inthefeedback capacitorCf, showninFig.6(d).Thesystemhasseveraladvantagesthathelpto compensateproblemsrelatedwiththesensorsuchasoffsets, non-linearity,intrinsicgain,sensor’smismatch,etc.Varyingtheduty cycleoftheactuationvoltage,forexample,cansettheoptimum SNRandgainforthesensorsinvolved.Varyingtheamplitudeofone oftheexcitationvoltageswithrespecttotheothercancompensate foroffsetsornon-linearities.Forthecaseofthestrainsensorsimilar behaviorissimulatedwiththeonlydifferencethatthefrequency ofthesignalisclosetoDCandthemassofthesensorissmall.
Fig.6. Variablecapacitorelectricalmodelresults.(a)Proof-massdisplacementattheinputofthemodel,(b)excitationvoltages,(c)currentpulsesatoutputofhalf-bridge, and(d)onlypositivepulsesareintegrated.
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Fig.7.ArchitectureofasinglechannelofthereadoutASICandsin(x)/xresponseofthesystem(inset).
Fig.7showssinglechannelarchitecturereadoutaswellasthe sin(x)/xsystemresponse.Itdiffersfromcommonlyuseddesigns
[2,3]bydecouplingtheoutputofthesensorfromtheinputofthe
chargeamplifier(OTA)byaseriescapacitorC1andswitches con-nectedtoarbitraryvariablereferencevoltagesVREF1andVREF2. Thefunctionof C1is levelshifting, toallowa different operat-ingpotential betweentheoutput of thesensors and theinput of the OTA. In this way the excitation voltages of the sensor canbeunipolar, while still allowingDC signalprocessing from thesensorssignals.Thearchitecturedifferssignificantlyfromthe modulation–demodulationapproach,whichisregularlyusedfor similardevicesandusesmorepower.
Architectureshavebeenreported[1–4]inwhichlinearity, res-olution,bandwidthor gain isalwaysmatched totheparticular typeof device.In somedesignsthechannel architectureis tai-loredtothepropertiesofthesensorand,althoughsomeflexibility is added as shown in [7–9], its performance is not optimum (FOM=1.0×10−18F√(W/Hz)).
Inthisworkthenumberofpulses(N)canhoweverbe arbitrar-ilysetdependingonthedesiredSNR,bandwidthorgain.Tofirst ordertheseparametersarerelatedbythefollowingrelationships: thegainisproportionalwithN,sinceallNintegratedpulsesare added.ThebandwidthisproportionaltotheinverseofN,sincethe samplingtimeisproportionaltoNandtheSNRisproportionalto thesquarerootofNbecausegainisincreasingwithNandnoiseis onlyincreasingwithsquarerootofN.Thisisoneofthekeyissuesof theproposedarchitecture,itsolvestheissueofsettingthegainof thesystembyincreasing/decreasingthenumberofpulsesinstead ofswitchingbetweenintegratingcapacitorsofdifferentsizes.The readoutgainhaslittletemperaturedependency,non-linearityand hysteresis,sincetheintegratedcapacitorCf,theOTAperformance andclockfrequencyareverystable.
Thedevelopedsystemhastheaddedadvantagethatthesame readoutcanbeusedtosenseaccelerationandstrainwiththe pur-poseof reducing powerconsumption and making it more cost effective,thereisnoneedtofabricatetwodifferentreadoutsto processtheinformationcomingfromthetwotypesofsensors.In principlethesignalsfromthetwotypesofsensorscouldbe mul-tiplexedattheinputofthereadout,thus usingonlyonesingle channeltoamplifytheirsignalsbyalternatingthereadingofthe sensorsinapredeterminedsequence.Neverthelessthe accelerom-eterhas tobe alwaysswitched-on. One way toovercome this
requirementisbyoperatingthereadoutinalow power(lower bandwidthandSNR)modeandswitchedtohighresolution acqui-sitionmodeincaseofanearthquakeevent.Thestrainsensoris usedforcertainperiodsoftimeandatime-sharingschemewould makethedecisiontoalternatebetweentheaccelerometerandthe strainsensorwithoutjeopardizingthedataacquisitionbandwidth andSNRimmediateafteranearthquakeoccurred.
4.1. Measurements
Forthepurposeofsimulationofthewholesystembothsensors weremodeledinahighleveldescriptionlanguage,namely Ver-ilogA,asapairofvariablecapacitorsproducinga10%Cfullscale. Themodelallowsthedesignertoaccuratelyassessthegain,noise, sensitivityandmotionartifactswithinthecircuitdesign environ-mentwithlesscomputationaleffort.Resultsareingoodagreement withsimulations;thenextparagraphsshowthemeasurements.
Fig.8showsthemeasurementsoftheaccelerometersensorwith theproposedreadout.Inthefigurethreechannelsareplotted cor-respondingtoX,YandZdirectionsandcomparedtocommercially available accelerometers, namely PCB piezoelectric transducers model393-B12and393-B31[11].TheWLdatacorrespondstothe sensorsandreadoutdesignforthisworkwhereastheBdata corre-spondtothecommercialdevices.Bothsystemsandobtaineddata complywithspecificationsforbuildingintegrity monitoringbut thedevelopedreadoutconsumeslesspowerthanthecommercial one.
Asshownin[10]theresolutionis80dB(13-bit)forvibration tonesbetween10and100Hzandnon-linearity<1%.The accelera-tionmeasurementsaremeantforrecordingthebuilding’sresponse during an earthquake event; the measured system noise floor (readoutplussensor)of70g/√Hziswellinlinewiththepurpose oftheapplicationanddoesnotdegradetheexpectedperformance ofthesystemasshownin[13].MEMS-basedaccelerometerslike theSTMicroelectronicsLIS3L02ALhavea50g/√Hznoisefloor fora±2grange[14]andtheCrossbowCXL10TG3a20g/√Hzfor a±2grange[15]buttheirpowerconsumptionisintheorderof mW,smalleraccelerationrangeandarelargerinsize,therefore notsuitableforoperationoverextendedperiodsoftimewithout rechargingorreplacingbatteries.
ThereadoutisDCcoupledthereforeabletoreadverylow fre-quencysignals.Thisrepresentsanadvantagecomparedtostandard
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Table2
PowerconsumptionatVDD=1.6V.
Current Power Amplitude Non-linearity
2.51A 4.00W 57.1mV/g 1.24%
0.44A 0.70W 52.7mV/g 1.05%
0.33A 0.52W 43.5mV/g 1.73%
0.19A 0.30W 21.6mV/g 6.30%
modulation–demodulationschemes,whicharealwayslimitedtoa specificlowfrequencyvalue,thusallowingforthereadoutof sig-nalssuchasthosefromastrainsensor.Fig.9showstheresultsof strainsensormeasurementswhenmountedonatestrebar.
Testsweretakenoveratimespanofover2000sunder con-tinuoustensilestrainandreleasetosimulatethestraincondition expectedinthesteelreinforcementofaconcretebuildingduringan
earthquakeaction.Thesteelbarwastakenbeyonditselasticlimit, correspondingtoaloadcapacityofapproximately140kNanda yieldstrainof2000.Thedatawerecomparedtocommercially availablesystemscompliantwiththespecifications.More specif-icallythereferencesensorsareresistivemetalfoilstraingauges HBMmodel LY41-3/700[12].Consistentlywithpreviousresults
[10],thetestconfirmsthatsensorsandreadoutareableto mea-sureoverarangeof±20,000,whichcorrespondstotheultimate designstrainconditionofsteelreinforcementundersevereseismic action.
Fig.10showsthemeasurementsofthesensitivityversusthe integratednumberofpulsesNfortheaccelerometer.Asexpected thesensitivityofthereadoutisproportionaltothenumberofpulses N,whiletheintegratednoiseisproportionalto√N.The measure-mentsweretakenwitharateof200samples/s.
Fig.8.MeasuredaccelerationsignalsforX,YandZchannelscomparedtocommercialdevices(N=24pulses).
Fig.9. (a)Testrebarmountingofthestrainsensoralongwiththereferencegauge(topright).(b)Loadvs.strainplotfortest(WLdata)andreferencesensors(SGdata).(c) Strainvs.timehistorymeasurements.Thepositionofthesensorintherebarisalsoshownintheinset.
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Table3
Comparisonwithstate-of-the-artcapacitivereadouts.
Parameter Denison[5] Paavola[6] Thiswork
Accel/strainsensorrange ∼±1g ±2g ±2.5g
±20,000
Supplyvoltage 1.7–2.2V 1.0V 1.6/3.0V
Power 1.5W 1.5W 440nW/15W
Sensitivity 125mV/g – Variable
Noisefloor(acceler.) 1mg/√Hz 704g/√Hz 70g/√Hz
Non-linearity <1% – <1%(accel.)
<0.6%(strainsensor)
Bandwidth 10Hz 1Hz 100Hz
Figure-of-Merit 8.1×10−22F√(W/Hz) 4.41×10−20F√(W/Hz)
1400Wg/Hz 881Wg/Hz
Technology 0.8mCMOS 0.25mCMOS 0.25mCMOS
Activearea – 2.25mm2 2mm2
Fig.10.Measuredsensitivityandtotalintegratednoisefortheaccelerometervs. numberofpulsesN.
Thesensitivityandrangeofacceleration(orstrain)canbeset accordingtothedeviceandapplicationspecifications.Alternative methodshavebeenreportedelsewhere;thesettingsof reconfig-urablebuildingblockscreateanadaptablegenericarchitecturefora widerangeofcapacitivesensors[9].Neverthelesspower consump-tionremainshighandnotadequateforlowpowerapplications.In thisworkthereadoutwasdesignedtooptimizepower consump-tion.Previousresultsshownin[10],withVDD=3.0Vshowapower
consumptionof15W.Withabiasvoltageof1.6V,improved lev-elsofpowerconsumptionforthereadoutcircuitcanbereachedas showninTable2.
Theamplitudeofthesignaldecreasesbyafactorof10butthe powerconsumption decreasesbyafactorof 100while keeping therestoftheparametersasinthecaseof3.0V.Theresultsin thetableshowalsothenon-linearityvalueswhicharestillwithin specifications.Attheminimumpowerconsumptionof330nWthe non-linearityincreasesto6.30%whichistheextremecaseofthe operatingrangeofthesensorsystem.Theexperimentalresultsare showninFig.11.
Inspiteoftheamplitudeofthesignalbeinglowerthesystemcan compensatebyintegratingmorepulses,asmentionedinprevious paragraphs,andthereforerestoretheDynamicRangetofull rail-to-rail.Thesystemresponsetimewilldecreasebutforthetarget applicationsthisdoesnotrepresentamajorproblem.
5. Conclusions
Results show that the readout architecture can work with Ultra-Lower-Powerconsumptionwhilekeepinglinearityunderthe expectedperformance.Batterylifetimeisthenextended to sev-eralyears’operation.Comparedtothefiguresofmeritproposed
in[5,6]thisworkhas4.41×10−20F√(W/Hz)and881Wg/Hz,
Fig.11.Signalamplitudeat1.6Vforseveralbiascurrentvalues.
respectively.Theproposedarchitecturehasthelowestreported equivalentaccelerationnoiselevel,highestbandwidthandhasthe uniqueadvantageofofferingtradeoffbetweenSNR,bandwidthand power.Whencomparedtocommercialaccelerometersandstrain sensorsthereadoutofferstheusercompetitivespecifications.The designwasfabricatedonTSMC0.25mCMOSwithM-i-M capac-itors.Thetotalpowerconsumptionof the3channelsis15W. The clock and excitation voltages for the sensors are external. Recentmeasurementsshowthatthearchitecturecanworkwith lesspowerconsumption(0.52W)stillwithintheexpectedrange ofaccelerationandstrain(Table1).
Table 3 shows thebenchmarking of the proposed
architec-ture.No similarsystem hasbeenreportedwhich handles both accelerometers and strain sensors with a minimum of power consumption,lownoisefloor,variablesensitivityandlarger band-width.Mostofthesystemsreportedarecustom-madesystemsfor aparticularsensor(whichusuallyhasalargesensitivityina nar-rowband)withlow-powerconsumption.AlsoshowninTable3is thelowestpowerconsumptionmeasurementreported.
The presentedsystem candeal withdifferent sensors with-outjeopardizingthepowerconsumption,importantin building integritymonitoringwhichrequiresbatteryoperatedsystemsfor severalyears.Italsorepresentsaverycosteffectivesolutionsince thesamereadoutcanbeusedforaccelerometersorstrainsensors, makingtheintegrationofthefinalmonitoringsystemsimplerand cheaper.
Flexibilityis alsoa majorassetfor thesystem,sensors with differentsensitivities,offsetsandmismatchcanbeeasilyreadout modifyingthetiminganddutycycleoftheexcitationpulsesand thenumberofintegratedones.Asinglereadoutsystemforboth accelerometersand strain sensorsmakesthesystemmore cost effectiveandpowersaving.
J.Santanaetal./SensorsandActuatorsAxxx (2011) xxx–xxx 7
Acknowledgments
ThisworkispartoftheHuman++Programofimec-HolstCentre, TheNetherlands,andpartiallyfundedbytheMEMSCONproject (EC SeventhFramework ProgrammeGrant Agreement n. CP-TP 212004-2).
References
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Biographies
JuanSantanaobtainedhisPhDinSemiconductorDevicesfromtheUniversityof Lancaster,U.K.andin1992joinedtheengineeringdepartment.In1997hejoined CINVESTAV,aresearchcentreinMexico.From1998to2001hedirectedthe Semi-conductorTechnologyCentre(CTS)ofCINVESTAV.Heworkedasacommissioned engineerinseveralASICprojectsforautomotiveapplicationsforATMELCorp.,in Columbia,Maryland.In2001hejoinedtheMotorolaCenterforSemiconductor Tech-nology.Since2006heworksforHolstCentre,TheNetherlands.Hehaspublished morethan30papersininternationaljournals,supervisedseveralM.Sc.dissertations andholdsonepatent.
RichardvandenHovenstudiedElectronicsattheTechnicalUniversityin Eind-hoven,wherehegraduatedin2006atthegroupMixedSignalMicroElectronics on“Apre-correctionmethodforimprovedstaticlinearityusingparallelDACs”.In
2006hejoinedPhilipsSemiconductors(NXP)inEindhoven,theNetherlands.Since 2007heworksforHolstCentreintheNetherlands,onASICdesignofAnalogto Dig-italconversionandcapacitivereadout.Hehaspublishedtwopapersandholdsone patent.
ChrisvanLiempdisaSeniorResearcheratHolstCentresince2009.Hehasbeen systemarchitectatPhilipsSemiconductors,NXPandSunext.In1998hebecame partofthePhilipsOpticalStoragegroupandplayedamajorroleinseveralprojects inthisgroup.Hehasmorethan30yearsexperienceinanalogelectronics engi-neering.Heis currentlyworkingonDC–DCand AC–DCconvertersforpower managementandenergyharvesting.Hehaspublishedseveralpapersandholds patents.
MikaelColinreceivedaPostgraduatedegreeinOpticsin2000fromthe Univer-sityofSaint-Etienne,France.HesubsequentlyjoinedBookhamTechnologies,UK (2000),andOpsitech,France(2002),asanR&Dengineerwherehemainlyworked indesigningintegratedcomponentsforOpticalNetworks.In2004,hemovedto Memscap,France,asaMEMSdesigner.Hisworkmainlyfocusedonthedesign ofinertialcomponentsforMilitary,Space,BiomedicalandIndustrialapplications andonEnergyscavengingsolutionsusingtheMEMStechnology.Since2011,he worksonthedevelopmentofimplantableenergyscavengersattheTIMAlaboratory, France.
NicolasSaillenisaMEMSProductEngineerwithaM.Sc.degreeinMicroSystems EngineeringfromEPFL,Lausanne.Hehas5yearsexperienceinMSTprocess,product development,andinternationalprojectmanagementatThermoFisherScientific (previouslyC2V).Hisworkinvolves,amongotherthings,thedevelopmentofmicro componentssuchas:aflowsensor,forcesensor,apiezodriveninkjetnozzle,and fluidicvalves.
DanieleZontaachievedhisDoctorateinStructuralMechanicsattheUniversity ofBolognain2000.HeworkedasaPost-DoctoralresearcherattheUniversityof California,SanDiego,intheperiod2000–2001.Hehasbeenvisitingscholaratthe UniversityofMichigan(2010)andatPrincetonUniversity(2009and2011).Since 2001,heisAssistantProfessorofStructuralEngineeringattheUniversityofTrento, teachingprecastconcretebridgedesignandsmartstructures.Hisresearchactivity includes:bridgemanagement;Bayesiandecision-making,structuralhealth moni-toring;fiberopticsandsmartsensortechnologies;allasappliedtocivilstructures. Heisauthorofoveronehundredtechnicalpublications.
DavideTrapanigraduatedin2010incivilengineeringattheUniversityofTrento.He iscurrentlyResearchAssistantintheIntelligentInfrastructuregroupatthesame Universityworkingonthelaboratoryvalidationofsmartsensortechnologies.He authoredfourtechnicalpapers.
TomTorfsreceivedthedegreeofIndustrialEngineerinElectronics,specialization DesignTechnologyin2001fromDeNayerInstitute,Belgium.Heissince2001a systemsdesignengineerinthesensorelectronicsgroupatIMEC.Hehasdesigneda rangeoflowpowerwirelesssensormodules,withafocusonbiopotentialacquisition systemsforbodyareanetworksandautonomoussystems.Hehasalsobeenactive indevelopingdemonstratorsusingIMEC’s3Dand2Dintegrationtechnologyaswell asparticipatinginthedesignofa3Dmodularneedlearrayforinvivoapplications (NeuroprobesEUproject).
ChrisVanHoofisProgramDirectorofMorethanMooreSIPSystemsatIMECin Leuven.HeisalsoAssociateDepartmentDirectorofInterconnect,Packagingand SystemIntegration.HereceivedaPhDinElectricalEngineeringfromtheUniversity ofLeuvenin1992.AtIMEC,hebecamesuccessivelyheadofthedetectorsystems group,DirectoroftheMicrosystemsDepartmentandIntegratedSystems Depart-ment,andProgramDirector.Hisresearchconcernsautonomoussensornodes, focusingonadvancedpackagingandinterconnecttechnologyandsystem integra-tion.Since2000heisaprofessorattheUniversityofLeuvenadvising12doctoral students.