ContentslistsavailableatScienceDirect
Sensors
and
Actuators
B:
Chemical
j ou rn a l h o m ep 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 b
Detection
of
colorectal
cancer
biomarkers
in
the
presence
of
interfering
gases
夽
G.
Zonta
a,c,∗,
G.
Anania
d,
B.
Fabbri
a,c,
A.
Gaiardo
a,e,
S.
Gherardi
a,
A.
Giberti
a,b,
V.
Guidi
a,b,c,
N.
Landini
a,
C.
Malagù
a,caDepartmentofPhysicsandEarthScience,UniversityofFerrara,ViaSaragat1/c,44122Ferrara,Italy bMISTE-Rs.c.r.l.,ViaP.Gobetti101,40129Bologna,Italy
cCNR-INO–IstitutoNazionalediOttica,LargoEnricoFermi6,50124Firenze,Italy
dDepartmentofMorphology,SurgeryandExperimentalMedicine,UniversityofFerrara,ViaLuigiBorsari,46,44121Ferrara,Italy eMNF–MicroNanoFacility,BrunoKesslerFoundation,ViaSommarive18,38123Trento,Italy
a
r
t
i
c
l
e
i
n
f
o
Articlehistory:
Availableonline18May2015 Keywords: VOC Colorectalcancer Sensor Benzene 1-Iodo-nonane Decanal
a
b
s
t
r
a
c
t
Medicalstudieshaveshownthattumorgrowthisaccompaniedbyproteinchangesthatmayleadtothe peroxidationofthecellmembrane,withconsequentemissionofvolatileorganiccompounds(VOCs). VOCscanbedetectedthroughbreathorintestinalgasesandarebiomarkersforcolorectalcancer(CRC). TheanalysisofVOCsrepresentsanon-invasiveandpotentiallyinexpensivepre-screeningtechnique.An arrayofchemoresistivegassensors,basedonscreen-printedMetalOXide(MOX)semiconductingfilms, hasbeenselectedtoidentifygaseouscompoundsofoncologicalinterest,i.e.benzene,1-iodo-nonane anddecanal,fromthemaininterferersthatcanbefoundintheintestine.MOXsensorsareabletodetect concentrationsdowntoabout10thppb,asexperimentallyproveninpreviousworks,sotheycanidentify veryslightdifferencesinconcentrationamonggasmixtures.Inthisworkithasbeenproventhatthearray usedisabletoidentifytumormarkerssingularlyandincombinationwithothergasesbothinwetand dryconditions.Moreover,thesensorschosencandiscriminatetargetVOCsfrominterferersevenatlow concentrations.
©2015ElsevierB.V.Allrightsreserved.
1. Introduction
Nano-materialscanofferpromisingnon-invasivemethodsto detectand preventcancer[1].It isknownthatVOCs emissions, producedbytheperoxidationofthecellmembraneorbycellular metabolism,arelinkedtotumorpresenceandgrowthandtheycan bedetecteddirectlyfromtheheadspaceofcancercellsorthrough exhaledbreath[2,3].Indeed,changesinthebloodchemistrylead to measurablemodifications in the breath composition due to exchangesinsidethelungs,e.g.intherangeof20–100ppbfor sev-eralVOCs[4],aswellasinfecesfromnormaldigestion[5].Aimof thisworkistostudythedetectionofVOCsindicatorsofCRC, iden-tifyingthemostselectivesensorsforthesecompounds,inorderto analyzeintestinalgasesinwhichthesebiomarkersshouldconvey.
夽 SelectedpaperspresentedatEUROSENSORS2014,theXXVIIIeditionofthe conferenceseries,Brescia,Italy,September7–10,2014.
∗ Correspondingauthorat:DepartmentofPhysicsandEarthScience,University ofFerrara,ViaSaragat1/c,44122Ferrara,Italy.Tel.:+390532974286.
E-mailaddress:giulia.zonta@unife.it(G.Zonta).
ThemostrelevantVOCswhichmayindicateCRCpresenceare ben-zenecompounds,1-iodo-nonane(C9H19I)anddecanal(C10H20O)
[4–6].ThemaingasesthatcaninterfereinthiscontextareH2,CH4,
H2S,SO2,N2,NO2andNO,thesebeingthemaincomponentsofthe
intestinalgasmixture.
2. Materialandmethods
2.1. Sensorsproperties
WetestedseveralMOXforthisdedicatedexperiment,andthe selectedsensingmaterials,themostpromisingones,asconfirmed bythereporteddata,arelistedinTable1.Sensorsarepreparedvia screen-printingtechnique,afterthedepositionoftheMOXpaste onaluminasubstrate.Theyareprovided witha heatermadeof platinum onthebackside,whilethecontactsaremadeof gold. Thescreen-printingprocedureisreportedinPrintedfilms:Materials scienceandapplicationsinsensors,electronicsandphotonics[11].
Atypicalscreenconsistsofanetwork offinelytwistedsteel wires(of100m),stretchedoveraframeofaluminum.Sensors havebeenelectricallycharacterizedinalaboratorysetupusinggas http://dx.doi.org/10.1016/j.snb.2015.04.080
Fig.1. Schemeoftheexperimentalsetupforgasesfrombottles.Thebottlesare connectedtomassflowcontrollers.Thefirstlineconveysthetargetgas(e.g.C6H6
orinterferers),thesecondlineconveysdryair,thethirdoneisemployedoncethe measureistakeninwetconditions.Airandgasesarriveatthesensorschamber.
Fig.2. Laboratorysetup.
bottlesasoriginforgastargetsandinterferences.Thesystemis
sketchedinFig.1,whilethesetupfortheacquisitionofthesignal
isshowninFig.2.
WeselectedZnO(withtwodifferentthermaltreatments,650 and850◦C),foursolid solutionsofSnO2 andTiO2,asolutionof
TiO2,Ta2O5andvanadiumoxideandasolutionofSnO2,TiO2and
Nb2TiO7(allthesematerialweretreatedthermallyat650◦C).The
annealingtemperaturessynthesis and structural,morphological and thermal characterizations of these nanostructured materi-als are reported in literature [7–9]. The increase of the firing temperatureis directly related tothe increase of theradius of thenano-spherescomposingthesensingmaterial. Aftertesting MOX sensors, in previous works [10,11], with firing tempera-turesrangingbetween650and950◦C,wehavechosenthefiring
temperatures650◦C (for tin/titanium-oxide-based sensors) and 850◦C (for the zinc-oxide-based sensor) as the ones at which theygivethehighest response. Themost commonformulation forscreen-printablepasteislistedinTab.11.9ofthebookPrinted films:Materialsscienceandapplicationsinsensors,electronicsand photonics[13].Asreportedonpag.298ofthebook,specificpaste compositionsarehighlyproprietary.Thethicknessofthesensing layersisabout30m(thickfilmsensors)andtheywereobtained byscreen-printpastessynthetizedfromthesepowders(byadding aproperamountoforganicvehicles)ontominiaturizedalumina substratesequippedwithpre-depositedelectrodesandtheheater [12].Thegassensingmeasurementswereperformedbymeansof theflow-throughtechnique[13–15].
Responsesfromsensorsaregivenbythedimensionlessformula:
R= Vplateau
Vbaseline,
(1) whichremovesallthedependenceofthesensorsresponseonthe geometry.Fig.3showsanexampleofsensorsresponsetoC6H6
beforenormalization.Thematerialcharacterizationwascarriedout byusingscanningelectronmicroscopy(SEM).ASEMimageofthe filmisshowninFig.4toappreciatethemorphology.
2.2. Experimentalsetup
Thesensorswerelocatedintoagasflowchamber,insidewhich anartificialatmospherewereinjectedandcontrolledbypc-driven mass-flowcontrollers.Thegaseswerefromcertifiedbottlesand
Fig.5.SubtractionbetweensuccessiveplateausofN2anddrysyntheticair
inter-ferences,normalizedovertheirbaseline.Theshowsthedifferenceofresponses forthattemperaturetothevariation,foraddition,of5sccmofO2inthe500sccm
ofthechamber.
Fig.6.SubtractionbetweensuccessiveplateausofN2andwetsyntheticair
inter-ferences,normalizedovertheirbaseline.Theshowsthedifferenceofresponses forthattemperaturetothevariation,foraddition,of5sccmofO2inthe500sccm
ofthechamber.
Fig.7. Analysisofthetotalandpartialresponserates(ratiobetweenresponses)of thesensorsarraytoC6H6(5ppm)inamixtureofCH4(10ppm),H2(60ppm)and
dryair(N2:80%,O2:20%).Humidityisusedasaninterferer.
Fig.8.analysisofthetotalandpartialresponserates(ratiobetweenresponses)of thesensorsarraytoC6H6(2ppm)inamixtureofCH4(10ppm),H2(60ppm)and
wetair(N2:80%,O2:20%,RH:38%).
Fig.9. SensorresponsestoC6H6(2ppm)insideamixtureofwetair(RH∼20%)and
twominorintestinalinterferinggasesNO2(2ppm)andH2S(20ppm).
Tempera-turechosenaretheonesatwhichthesensorresponsestoNO2becomenegligible.
Benzeneiswelldetectedintothispartialinterferingambient.
Fig.10.SensorresponsestoC6H6(2ppm)insideamixtureofwetair(RH∼34%)and
twominorintestinalinterferinggasesNO(2ppm)andSO2(2ppm).Temperature
chosenaretheonesatwhichthesensorresponsestoNObecomenegligible.Benzene iswelldetectedintothispartialinterferingambient.
thevaporsof1-iodo-nonaneanddecanalweresuppliedbymeans ofabubblerwiththeproperamountoftheliquids.Theschemeof theexperimentalsetupisshowninFig.5publishedinourprevious workMalagùetal.[1].
Fig.11.Sensorresponses,asafunctionoftime,toSO2(1stpeak),C6H6+SO2+NO(2ndpeak),C6H6+SO2+NO+wetair(3rdpeak),C6H6(4thpeak)indryconditions.
TemperaturechosenaretheonesatwhichthesensorresponsestoNObecomenegligible.
Fig.12.Sensorresponses,asafunctionoftime,toH2S(1stpeak),C6H6+H2S+NO2(2ndpeak),C6H6(3rdpeak)inwetconditionsRH:20%.Temperaturechosenaretheones
atwhichthesensorresponsestoNO2becomenegligible.
Theresponse to thetarget gaseswasobserved for different workingtemperaturesbothindry(RH∼0%)andinwetconditions (18%<RH<60%).Choosingthemostfavorabletemperaturesofeach sensorforbenzenedetection,theintestinalstandardgasmixture
wasapproximatelyreproducedintothesensorschamber.CO2 is
notconsideredbecauseitiswellknownthatitishardlydetectedby chemoresistivesensors[13].Duringtheexperimenttesting mea-surementsweredoneondryandwetairwiththepurposetocheck
Fig.14.SensorresponsestoC9H19Iindryconditions.Temperaturesrangesbetween350and600◦Cwithstepsof50◦C.Underparenthesisisshownthequantityofreagent
(moles)takenforeachmeasure.
thedifferencesofresponseonthevariationofhumidity, operat-ingtemperature,andoxidationofthefilms.Itisimportanttostate theeffectsofthevariationsofoxygenonthesensorsresponsesfor threemainreasons:(i)intheintestinetherearevariationsof oxy-genproductionduetothedigestive,bacterialandcellularactivity; (ii)therearesomechemicalreactionthatoccurbetweenoxygen andothercompoundsbothintheintestineandinthe experimen-talsetup;(iii)somebottlesusedintheexperimentaltestscannot containoxygenforsafetyreasonsbutcontainN2(i.e.H2).Forthese
reasonsthetotalvolumeofthechamberwasfilledwithN2andO2
indifferentconcentrations,usingatfirstaflowofsyntheticdry orwetair with20%O2 and80%N2.Then,withtheadditionof
aflowofpureN2andtheloweringofthesyntheticairflow,the
ratiobetweenO2andN2inthechamberwasmodified(increasing
O2volumeconcentrationof1%),obtainingsoadetailedanalysis
ofthedisturbancefromenvironmentalchangesand differences onmetaloxidefilms(Figs.5and6).Wedefinedwiththesymbol
thedifferencebetweenresponsesinthetwocasesdescribed before.
Regardingdecanaland1-iodo-nonane,itisimportanttonotice that thereported number of moles represents an upper limit, obtainedfromthesubtractioninweightofthedropsofcompounds fromthepipette;duetotheuncontrollabilityoftheevaporative processandthenon-hermeticallockupofthegasbubbler,partof thedosecanbeassumednottohavereachedthesensorsatall.
Testswith1-iodo-nonaneweremadeindryconditions,usingan emptygasbubblertoevaporateit;nosolventswereusedtohaste theevaporationofC9H19I,duetothehighresponsesofsensorsto
alcoholsandotherorganicreagentslikedichloromethane(CH2Cl2).
Theweightofthereagentwasmeasuredwithaprecisionbalance, tocalculatethenumberofmolesandtoobtainanaveragevalueof theconcentration.Toidentifythebestdetectingtemperaturefor eachtypeofsensingmaterial,wetestedtheresponseatseveral workingtemperatures(350,400,450,500,550,600◦C).
Fig.15.SensorresponsestoC10H20Oindryconditions.Temperaturesrangesbetween350and600◦Cwithstepsof50◦C.Underparenthesisisshownthequantityofreagent
NOweremadebothindryandwetconditions.Theconcentrations oftheseinterfereswere20ppmforH2Sand2ppmforallothers,to
reproducerealconcentrationsintheintestine[16].Measurements weremadeatthebestworkingtemperatureforeachsensor(Tbest)
tohavethehigherselectivityforbenzenewithrespecttothe con-tributionofinterferes.ObservingFigs.11and12itisevidentthat, bothinwetanddryconditions,thesensorsresponsestobenzene isconsiderablyhighercomparedtothatofinterferers.These inter-fererswerechosenbecausetheyaregasotransmitters(NO) [17] normallypresentinhumangut,productsofthebacterialactivity inhumanstomachandintestine(NOxfamily[17–19])orofhighly
reactivedigestionprocesses(H2S).
SO2wastestedtoverifytheoccurringofthechemicalreaction
2H2S+3O2→2H2O+2SO2, (2)
whichrepresentsthecombustionofH2Swhichhappensathigh
temperatures on the surface of the sensing films (H2S
auto-combustionoccursat260◦C)[20,21].Itssignatureisvisiblefrom theinitialpeakofresponse beforereachingtheplateau,then it graduallyreduceswithtime,duetotheincreasingrelative humid-itycausedbythesurfacereaction(1)(Fig.13).
3.2. 1-Iodo-nonane(C9H19I)
ObservingFig.14,theZnO850sensor(zincoxide,firedat850◦C) andSTN(tin,tantalum,niobiumoxides)aretheonesthatgivethe bestresponsestothiscompound,confirmingresultsfortin oxide-basedsensorsofapreviouswork[1],inwetconditions.Humidity doesnotchangethetrendoftheresponsesto1-iodo-nonanebut reducesonly their value. TiTaV, which is selective to benzene, showsalowresponsetothiscompound.1-iodo-nonaneissensitive tolight,soallthedroppingproceduresandweightmeasurements havebeendoneinconditionsofdarknesstopreservetheoriginal stateofthecompound[22].
3.3. Decanal(C10H20O)
Testswithdecanalweremadeindryambientwiththesame pro-cedureusedfor1-iodo-nonaneandwiththesamesensorsarray. ResponsesaresummarizedinFig.15.ThesensorsST20650,STN andST25650arethebestrespondingonestodecanal.This evi-dencehighlightsthepropertyoftinoxide-basedfilmstohaveahigh responsetothisVOC,insteadTiTaVdoesnotshowmuchaffinityto it.Aswith1-iodo-nonane,theweighinganddepositionofthedrops ofdecanalhavebeendoneindarkness;C10H20Oisinfactalsoair
sensitive,butitisstilllightactivatingtheprocessofauto-oxidation leadingtofirstperoxo-acidsproductionandthustoalterationon thecompound[23].
Table2
SensorresponsesattheirbestworkingtemperaturetovariousVOC.Responsesare givenasratesbetweenthetensionsmeasuredfortheplateausovertheiroriginal baseline.
Sensors Temperature(◦C) Gastarget Response
TiTaV 450 Benzene 1.9 ZnO850 450 1-Iodo-nonane 56.9 STN 450 1-Iodo-nonane 45.1 ST20650 450 Decanal 58.4 STN 450 Decanal 41.6 ST25650 450 Decanal 34.8 ZnO650 450 Decanal 31.6
3.4. Interferencetestsinwetair:C9H19IandC10H20O
We made a test with 1-iodo-nonane (2.57×10−4mol) and
decanal (7.46×10−4mol)in combination, in wet conditions,to
checkiftheinterferenceof thetwoVOCs canalterthesensors
responsesobserved in the previousmeasurements.The chosen
workingtemperaturewasthesameforallsensors(450◦C).Results
are shown in Fig.16. The response of tin oxide-based sensors
remainshighwhiletheZnO850,themostsensitivematerialfor 1-iodo-nonane,showsalowresponse.
4. Conclusions
Asetofsensorsmadeofsingleandmixedmetaloxideshasbeen selectedtodetectbenzene,1-iodo-nonaneanddecanal.Anarray ofsensorswasthenobtainedcombiningdifferentmaterials work-ingattheirbesttemperatures,whichprovedtobehighlyselective tothesegases,alsoinabackgroundofrealisticconcentrationsof H2, CH4, H2S, SO2, N2,NO2 and NO,indifferent environmental
conditions.TiTaVshowedthehighestselectivitytoC6H6 against
primaryinterferersasH2andCH4,emergingasthebestsensorfor
thisbiomarker.Testsonaldehydes(1-iodo-nonaneanddecanal) showedrefractorinessofTiTaVonrespondingtothisfamilyof com-pounds,whiletinoxideandzincoxide-basedsensors(inparticular, ZnO850andSTNfor1-iodo-nonaneandST20650,STNandST25 650for decanal)arepreferablefor thedetectionofthiskindof markers.Infacttheirrelativeresponsesareupto20timeshigher (Figs.13and14)thanthoseofTiTaV.
According to these results, we proved that, even for really lowconcentrations(2–5ppmforbenzene,anddosesontheorder of 10−4mol of 1-iodo-nonane and decanal), and withdifferent temperatureandhumidityconditions,chemoresistivesensorscan showhugeresponsesoncesetattheirproperworking tempera-tures(Table2).Thisconfirmstheapplicabilityofchemoresistive gas sensors as tumor marker detectors, leading to interesting
possibilitiestoenhancethehealthsystemandimprovingchances forpreventivescreeningoftumors.
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GiuliaZontaShereceivedtheBachelor’sDegreeinPhysicsandAstrophysicsin December2010(110/110cumlaude)andtheMaster’sDegreeinPhysicsinOctober
2013(110/110),attheUniversityofFerrara.InJanuary2014shestartedherPh.D.in MatterPhysics,workingwiththeSensorsTeam,coordinatedbyDr.CesareMalagù. IntheAprilofthesameyearsheobtainedtherecognition“FerraraSchoolofPhysics”, thatrewardstheinternationalityofherMaster’sthesiswork.Currentlyherresearch focusesonthestudyofthephysic-chemicalbehaviorofchemoresistive nanostruc-turedgassensors,putincontactwithvolatileorganiccompounds(VOCs)ofmedical interest.WithherteamshewonUnifeCup2013,abusinessplancompetitionthat rewardsinnovativestart-upsandStartCupEmiliaRomagna2014,withtheobjective tocreateastart-upfortherealizationofdevicesformedicalscreenings.Nowsheis theco-supervisoroftwostudentswhoareworkingfortheBachelor’sandMaster’s DegreeinPhysics,respectively.
GabrieleAnaniawasbornin1962,Italy.In2013heresultedadequatefortherole ofAssociatedprofessorincompetitiveexamofScientificNationalAbilitation,in sector06/C1–GeneralSurgery(Bando2012DDn.222/2012).In2001heresulted winnerofthetitleofacademicresearcherreservedto“UniversitàdegliStudidi Ferrara”personnelwithalltherequirementsaskedbythelaw4/1999declared withL.D.n.159on26/09/2000.1stlevelmedicalsupervisoratsurgerydepartment of“AziendaOspedale-UniversitàS.AnnadiFerrara”.In1999hewasassignedat Surgeryclinicsectionofsurgery,radiologyandanestheticsciencesdepartmentof “FacoltàdiMedicinaeChirurgiadell’UniversitàdegliStudidiFerrara”directedby Prof.IppolitoDonini.NowhehastheroleofAssociatedProfessorattheUniversityof Ferrara.
BarbaraFabbriSheobtainedherMasterDegreeinPhysicsatUniversityofFerrara in2011.CurrentlysheisaPhDstudentinvolvedinthefieldofgassensorsand micromachining.
AndreaGaiardoHeobtainedhisDegreeinChemistryattheUniversityofFerrarain 2011andtheMaster’sDegreeinChemicalSciencesattheUniversityofFerrarain 2013.Now,hisworkisfocusedinthefieldofinnovativeinorganicsemiconductors forapplicationsingassensing.HestartedhisPhDinPhysicsattheUniversityof FerrarainNovember2014.
SandroGherardiBachelorinPhysicsTechnologiesattheUniversityofFerrarain 2002.ResearchactivitycarriedoutattheSensorsandSemiconductorslaboratoryof theUniversityofFerraraaboutgassensingandindustrialapplicationsofmonitoring devicesbynanostructuredsemiconductorbasedsensors.
AlessioGibertiBachelorinTheoreticalPhysicsattheUniversityofFerrarain2000, heobtainedPhDinPhysicsofMatterin2004atthePhysicsDepartmentofthe UniversityofFerrara.HisresearchsincePhDisfocusedonthefieldofsemiconductor gassensorsbasedonnanostructuredmetaloxides,withparticularinteresttoward theelectricalandselectivityproperties.
VincenzoGuidiBachelorinPhysicsattheUniversityofFerrarain1990,fellowat “BudkerInstituteforNuclearPhysics”ofNovosibirsk(Russia)in1991.Thesisof doc-torateinexperimentalphysicsatLegnaroNationalLaboratoriesin1994.Researcher inexperimentalphysicsatUniversityofFerrara.Researchactivity,carriedoutatthe SensorsandSemiconductorslaboratoryoftheUniversityofFerrara,hasconsisted ofinvestigationsonbasicphenomenainsemiconductorsandtopractical imple-mentationsofsensingdevices.Authorofmorethan140articlesinpeer-reviewed journalsandofmorethan100contributionstotheproceedingsofinternational conferences,reviewerand/oreditorsofnumerousjournalsofPhysicsand Electron-ics,organizerofseveralnationalandinternationalconferencesandeditorofthe proceedings.
NicolòLandiniBachelorinPhysicsandAstrophisicsattheUniversityofFerrarain 2011.HeisagraduatingstudentinPhysics(Master’sDegree)underthesupervision ofDr.CesareMalagù,workingwithchemoresistivegassensorswithbiomedical applications.
CesareMalagùCesareMalagùwasbornin1974inFerrara,Italy.Hereceivedadegree inPhysicsattheUniversityofFerrarain1997(SummaCumLaude)andthePh.D. degreeinexperimentalphysicsin2001.HehasbeenteachingGeneralPhysicssince 2001andworksasaLecturerandAggregatedProfessorsince2007.Hisresearch activityismainlybasedonmodelingoftransportphenomenainnanostructured semiconductors.Hisexpertiseisinthickfilmtechnologyappliedtoenvironmental andenergeticsustainability.Hehasmorethan60papersinpeerreviewedjournals (Hirschindex23)andnumerousproceedingsandinvitedlectures,moreoverheis intheeditorialboardofseveraljournals.Hecoordinatesthesensorsgroupatthe UniversityofFerraraandteachesGeneralPhysicsIIandacourseofSensorsatthe DepartmentofPhysicsandEarthScience.