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External ionization source improvements for fourier transform ion cyclotron resonance mass spectrometry PDF

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Preview External ionization source improvements for fourier transform ion cyclotron resonance mass spectrometry

EXTERNALIONIZATIONSOURCEIMPROVEMENTSFORFOURIER TRANSFORMIONCYCLOTRONRESONANCEMASSSPECTROMETRY By KEITHDAVIDZIENTEK ADISSERTATIONPRESENTEDTOTHEGRADUATESCHOOL OFTHEUNIVERSITYOFFLORIDAINPARTIALFULFILLMENT OFTHEREQUIREMENTSFORTHEDEGREEOF DOCTOROFPHILOSOPHY UNIVERSITYOFFLORIDA 2004 Thisdissertationisdedicatedtomygrandfather,RodneyLawton. ACKNOWLEDGMENTS Firstly,IwouldliketothankSifuDaleHerring. Ihadbeenaspringboarddiver fromthe5*gradeallthewaythroughcollege. AfterIcametotheUniversityofFlorida,1 foundthelackofasportsteamledmetogrowcomplacent. IdonotthinkIwasever properlyfocuseduntilIbegantotrainwithSiftiDaleHerring. Martialartshasservedto keepmehealthy,bothphysicallyandmentally,overthelastfouryears. Ithankhimfor trainingmeandgivingmesomedisciplinethatIthoughtIalwayshad. Teachingmehow touseswordswasanunexpectedbutappreciatedbonus. Secondly,Iwouldliketothanksomeofthepeoplewhohavehelpedmeoutinmy researchovertheyearswithadviceandassistance. SteveMilesandLarryHartleyofthe chemistryelectronicsshophaveprovidedexcellentadviceonelectronicsandJoe ShaloskyandToddProxofthechemistrymachineshophavebeenafountofknowledge ondesignandconstruction. Theirassistancehasbeenimmeasurableandessentialtothe completionofthisresearch. Thirdly,IwouldliketothankthepastandpresentmembersoftheEylerresearch groupaswellasDr.JohnEyler. GroupmemberssuchasStanleyStevens,Jr.andSusan Abbatiellohaveprovidedmuchassistanceandwereinvaluabletothecompletionofthis research. Dr.JohnEylerhasbeenasourceofenthusiasmandknowledgetomeandIam forevergratefultohaveworkedforhim. Iknewthatanyproblemcouldbesolvedwith hismentoringandthediscussionswehadprovedtobeessentialtomyunderstandingof iii anytopicthatIhappenedtohavequestionsaboutonthatparticularday. This dissertationwouldnothavebeenpossiblewithouthisguidance. 1wouldliketothankmyfamily,especiallymyfather,whohasprovidedboth encouragementandcriticismatalltherighttimes. Hisenthusiasmforscienceand learningwasalmostinspirationalattimesandwasthemajorcontributiontothegenesis ofmysciencecareer. MyparentswerethefoundationofmyentireacademiccareerandI oweeverythingtothem. IwouldalsoliketothankEllenSternforallofherlove, devotion,andfaithinme. Withouthernoneofthiswouldhavebeenpossible. Her supportandguidancehavebeencrucialtomysuccess. Finally,1wouldthankmylategrandfather,RodneyLawton. Itwashisoptimism andenthusiasmthatservedasmotivationformeduringtoughtimes. Evenwhen1had doubts,healwaysbelievedthatIwouldearnmydoctorate. Forhisunwaveringsupport,I dedicatethisdissertationtomygrandfatherinhopesofhonoringhismemory. IV 657 TABLEOFCONTENTS page ACKNOWLEDGEMENTS ii LISTOFTABLES vi LISTOFFIGURES vii ABSTRACT xi CHAPTER 1 FTICRMASSSPECTROMETRY 1 Introduction 1 IonMotioninaMagneticField 3 IonTrapping 6 Excitation(SingleFrequency) 8 Detection(SingleFrequency) H FourierTransform 1 Excitation(Broadband) 1 FTICRComparedtootherMassAnalyzers 1 AdvantagestoIncreasedMagneticFieldStrength 18 BroadbandExcitationSchemes 19 FTICRPulseSequence 20 ComponentsofanFTICRMassSpectrometer 20 Conclusions 23 2 MASSSEEECTIONINMULTIPOEEIONGUIDES 25 Introduction 25 EquationsofMotioninaQuadrupole 30 StabilityDiagramsforMultipoles 35 3 GLOWDISCHARGEFTICRMASSSPECTROMETRY 40 V 1 Introduction 40 TheGlowDischargeProcess 41 GlowDisehargeMassSpectrometry 45 Interferences 45 MassAnalyzers 47 GD-FTICRMassSpeetrometry 48 Experimental 52 Results 54 Conclusions 63 4 ELECTROSPRAYIONIZATIONFTICRMASSSPECTROMETRY 64 Introduction 64 Experimental 66 Results 69 Conclusions 76 5 ATMOSPHERICPRESSUREIONIZATION 77 Introduction 77 AtmosphericPressureChemiealIonization 77 AtmospheriePressurePhotoionization 79 Instrumentation 8 EstrogensandEstrogenDerivatives 83 Experimental 85 Results 87 Conclusions 90 6 CONCLUSIONSANDFUTURESTUDIES 91 REFERENCELIST 95 BIOGRAPHICALSKETCH 100 VI LISTOFTABLES Table Page 2.1 Maximaandminimaforavarietyofmultipoleswithordern 38 3.1 Ionizationeventsinglowdischargeplasma 43 3.2 Massresolvingpowersrequiredtoseparateseveralatomicions andpotentialinterferences 46 3.3 Advantagesanddisadvantagesofseveraltypesofmassanalyzersfor elementalanalysis 49 3.4 ThecertifiedcompositionofNISTSUM1104,free-cuttingbrasspinsample 62 4.1 MajorIonsfoundinPNG2422A 75 5.1 Summaryofsomepossiblereactionsinacoronadischarge 79 5.2 ReactionsfoundintheAPPIionizationsource 80 5.3 Gasphaseionizationenergiesofsomecommongasesandsolvents 81 5.4 ReactionsinvolvingdopantintheAPPIionizationsource 82 vii 5 LISTOFFIGURES Figure page I.I TheLorentzforceactsuponchargedparticlesinthepresenceofan externalmagneticfield,Bo 4 1.2 Ionmotionwhichisradiallyconfinedinthexandydirectionsbyan externalmagneticfield,B,actingalongthezaxis 6 1.3 Apositivevoltageappliedtothetrappingplateswillconfineions axiallyintheICRanalyzercell 7 1.4 Ionsareinitiallyconfinednearthecenterofthecellinapartially incoherentpacket. UpontheapplicationofanRFpulsetothe excitationelectrodes,theionsareacceleratedtoacoherentpacket inalargerorbit 10 1.5 Themovementoftheexcitedionadjacenttothedetectplatesinduces asinusoidalcurrentintheplates. Thefrequencyofthecurrentis equivalenttothecyclotronfrequenciesoftheions 12 1.6 Astheradiusoftheionsdecreasesduetocollisionsbetween backgroundneutralsandothermolecules,theinducedsignal alsodecreases 13 1.7 ThemathematicalFouriertransformconvertsatimedomainsignal intoafrequencydomainspectrum. Masscalibrationgivesthem/q massspectrum 1 1.8 AtypicalFTICRmassspectrometeroutfittedwithanElectron Ionization(El)source 22 2.1 Behaviorofapositiveioncenteredbetweentwoelectrodes. A sinusoidalwaveformisappliedtoElectrodes1and2. Thewaveform appliedtoElectrode2is180degreesoutofphasefromthewaveform appliedtoElectrode1 26 viii 2.2 Cross-sectionalviewofaquadrupolararrangementofelectrodes 28 2.3 Equipotentialfieldlinesinaquadrupolararrangementofelectrodes 29 2.4 Stableandunstableiontrajectoriesinaquadrupoleionguide 33 2.5 Theoreticalstabilitydiagramforaquadrupoleionguide 34 2.6 Calculatedstabilitydiagramforaquadrupoleionguide 35 2.7 Theoreticalstabilitydiagramforahexapoleionguide. Uindicates unstableregions,PSindicatespartiallystable,andSindicatesregions ofstability 36 2.8 Theoreticalstabilitydiagramforaoctopoleionguide. Uindicates unstableregions, PSindicatespartiallystable,andSindicatesregionsof stability 37 3.1 FTCRmassspectrometerusedforGDexperiments 52 3.2 SchematicofthecoaxialcathodetypeGDsourceusedintheexperiments 53 3.3 Electricalcircuitusedtoprovidepowertotheoctopolerods 56 3.4 GDFTICRmassspectraobtainedfrompinsamplesofTa,In,andFe 57 3.5 GlowdischargeFTICRmassspectraofacoppersampleshowingthe effectsofpreselectiononlowabundanceions. Therffrequencyapplied totheoctopolerodsofthetopspectrumwas1.75MHz,forthebottom spectrumitwas850kHz 58 3.6 Spectraofabrasssample(NIST1104)showingtheeffectsofpreselection onlowabundanceions. Therffrequencyappliedtotheoctopolerodsfor thetopspectrumwas1.9MHz,whiletherffrequencyofthebottomspectrum was660kHz. Anincreaseinsignalintensityforlead(2.77%abundant) relativetocopper(61.33%abundant)andtin(35.31%abundant)isseen 59 3.7 SpectraoftheNIST1104brasssampleseeninfigure3.5.Tin(0.43% abundant)canbeseenabovethenoiseinthebottomspectrum. Themass rangewasexpandedoverthe100-220m/zrangetoshowdetail. Note thatthetinwasnotobservableinthetopspectrum 60 4.1 InstrumentalschematicofthemodifiedBrukerApex47ewithamodified Analyticaelectrospraysource 67 IX 4.2 IonopticsinthemodifiedAnalyticaESIsource. Theionoptics ateitherendofthehexapoleionguideareusedforionaccumulation 68 4.3 ESIFTICRmassspectraofacontaminated6pMAngiotensinIIsolution. Eachmassrangeshowsthetwomostprominentclustersofpeaksin theentiremassspectrum. Thesamplewasrunataflowrateof 17.5pL/hr. Thehexapoleoperationalfrequencywas3.4MHzfor thetopspectrumand1.9MHzforthebottomspectrum 70 4.4 HighmassrangefromthespectrainFigures4.3and4.2. The hexapoleoperationalfrequencyis3.4MHzinthetopspectrumand 1.9MHzinthebottomspectrum. Nootheroperationalparameters werechangedbetweentheacquisitionofeachspectrum. Each spectrumisasumof64scans 72 4.5 ESIFTICRmassspectraofacontaminated6pMAngiotensinII solution. Eachcolumnconsistsofseveralzoomedinslicesofa singlespectrum. ThefrequencyoftheappliedRFforeachspectrum islistedtotheleftofeachrow. TheY-axisscaleisconsistentacross eachrow,butnotdownthecolumns 72 4.6 S/NcomparisonsintheAngiotensinspectraforavarietyof hexapoleoperationalfrequencies. Eachspectrumisasumof64 scans 73 4.7 ESIFTICRmassspectraofa10folddilutionofAgilentTunemix. Eachcolumnconsistsofseveralzoomedinslicesofasinglespectrum. ThefrequencyoftheappliedRFforeachspectrumislistedtotheleft ofeachrow. TheY-axisscaleisconsistentacrosseachrow,butnot downthecolumns 75 5.1 ComparisonofImportantFactorsforAPPI,APCI,andESI 79 5.2 TwopotentialphotoionizationlampgeometriesusedinAPCI 83 5.3 CutawayschematicoftheAPPIionizationsource. Aisthemass spectrometerinlet. Bisthephotoionizationlamp. Cistheheated tube,thestripedbarsindicatetheresistiveheatingelement.Dis theauxiliarygasinlet. Eisthecapillaryinletforsampleintroduction. Fisthesheathgasinlet. Gisthealuminummountingplatform. ThegrayareasrepresentMacorpiecesusedforelectricalinsulation 86 5.4 APPImassspectrumofElquinolin100%MeOH 88 X

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