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Optimized Continuous Application of Hyperpolarized Xenon to Liquids 2018 B. Niederl?nder.pdf

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A:NewToolsandMethodsinExperimentandTheory
OptimizedContinuousApplicationofHyperpolarizedXenontoLiquids
BenjaminNiederländer,PeterBlümler,ThierryBrotin,DagmarVan
Dusschoten,AndreasOffenhäusser,HansJoachimKrause,andWernerHeil
,JustAcceptedManuscript•DOI:.8b09479•PublicationDate(Web):07Nov2018
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:.
Page1of36TheJournalofPhysicalChemistry
Niederlä-Xeviamembranes1/24
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4OptimizedContinuousApplicationof
5
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7HyperpolarizedXenontoLiquids
8
9
101,412
änder,ümler*,,
12
,äusser4,H.-
14
15
,UniversityofMainz,Germany
17
,ENSdeLyon,France
19
ülichGmbH,IBG-2,Germany
ülichGmbH,ICS-8,Germany
22
23
24
25
26
27Abstract:
28Inrecentyears,NMRwithhyperpolarized(HP)xenoninsidefunctionalizedhoststructures
29
30()havebecomeapotentialcandidateforthedirectobservationofmetabolic
31
32processes().Acriticalissueforrealapplicationsisthedissolutionofthe
33HP-,wepresentrecentdevelopmentsfor
34
35animprovedandcontrolleddissolutionofHP-Xeinliquidsusinghollowfibermembranesand
36

38129
-Xecontinuouslyatsmalladjustablepressures
40andinapolarization-
41
42HP-gasinaqueousliquids,
43

45

46
47optimizethesystemparameters,severalphysicalmodelsweredevelopedtodescribethe
48
49transportandthelossesofnuclearpolarization.
50
51Finally,-Xewas
52dissolvedinanaqueouscryptophane-A-(OCHCOOH)solution,andstableXesignalscould
26
53
54bemeasuredover35min,
55
56experimentalconditionsenabledthestudyofchemicalexchangeofxenonbetweencryptophane
57
58andwaterenvironmentsevenforatime-consuming2DNMR-
59stabilityoverthemeasurementtimeallowedanexactdeterminationoftheresidencetimeofthe
60
Xe-atominsidethecryptophane,±.
ACSParagonPlusEnvironment:.
TheJournalofPhysicalChemistryPage2of36
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5
612912
7Xenon-NMRisawell-establishedmethodtocharacterizemicroporoussystems,surfaces

9
10explores,however,itswidechemicalshiftrangeofmorethan300ppminNMR(nuclear
114
12magneticresonance)spectraallowstodistinguishphysicaladductsandadsorbatesselectively
13
,xenondissolvesinmanyliquids,allowingsuchstudiesalsoin
14
,itssolubilityinaqueousenvironmentsisratherlow,oftenlimiting
16
,suchsensitivityproblems
181296
19canbepartiallyalleviatedbytheuseofso-calledlaser-orhyperpolarized(HP)Xe.
20Hyperpolarized129Xeistypicallyproducedbyspin-exchangeopticalpumping6andexhibitsa
21
22spinpolarizationwhichisseveralordersofmagnitudehigherthaninthermalequilibriumat
23
24commonmagneticfieldstrengths(5–25T)androomtemperature.
25
26Inrecentyears,dissolvedxenonbecameapotentialcandidateformolecularimagingduetoits
27affinitytofunctionalizedhost-molecules(,cucurbiturilsandcryptophanes)
28
,cryptophaneswerefunctionalizedbybiotintodetect
30
31certainproteinsviathefrequencyshiftoftheHP-XeNMR-signalwheninsidethecryptophane
,
33

35
36liquidcontentinsuchfoams,thegas/liquidinterfacecancauseseverelossinspectralresolution
37
,thedissolutionprocess
39hastoberapidandwithoutsignificantdepolarizationoftheHP-
40
41overcomebyusinghollow-fibermembranes,asalreadyusedforclinicalblood-oxygenation
429
43().Suchmembranesactlikenanoporoussieveswherethegas/liquid
44
interfaceisprimarilyprovidedbytheinterplayofsurfacetensionandimmiscibilityofpolymer
45

47
48maintaintheseconditions,however,thepressuregradientatthisgas/liquidinterfacemustbe
49
50keptlowtoavoideitherliquidingressintothemembranematerialorbubbling.
ö
52
53toenrichbloodinmicewithHP-
54
55theimplementationofthisconceptisthedissolutionoftheHP-gasinbio-liquids.
56
57Inthiswork,wepresentadeviceforfast,efficient,polarization-sustainingandcontinuous
58dissolutionofhyperpolarized129-Xenoninliquidsviahollow-
59
60focuswasgiventothepossibilitytoaddbuffergasestotheHP-Xeandtocontinuousapplication
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4
,wheretheperformance
6

82D-NMRexperimentsonHP-
9
10duetothefieldgradientsviatheHP-gastransferbetweendifferentmagneticfieldsisdiscussed
11
12inAppendixA.
13
14
15

17
18

20
21
22Beforetheessentialnewfeaturesofthesetuparedescribedindetail,aschematicoverviewof
23129

25inahome-builtpolarizerbyspin-exchangeopticalpumping(,adetaileddescriptionis
26
27foundin11).TypicalvaluesforHP-
28129
29withpolarizationlevelsofabout20%using92%isotopicallyenrichedXe-gas(NUKEM
30
31IsotopesGmbH,Alzenau,Germany).Asystemofglass-valves(,KontesHI-VAC,DWK
32LifeSciencesLLC,Rockwood,USA)thenallowsadmixingofbuffergases(
33
34expansionorrelaxationsuppression11)andalsoconnectsaturbopumpforevacuation.
35
36Operatingthecompressorunit()insuctionmodethenallowssubsequentfillingthe
374
compressor’svolumewithseveralgases(hereHP-XeandHe).Thisgasmixtureisthen
38
39continuouslypressedintothemembraneunit(,membranes:CelgardX30-240,3M
40
41DeutschlandGmbH,Wuppertal,Germany)withawell-controlledoverpressureintheorderof
42
.
44Thedissolutionanddetectionpartoftheexperimentwasdesignedinaverycompactwayand
45
46includedtheNMR-excitation/detectioncircuittoreducethedistancebetweengasdissolution
47
,thelatterpartwasplacedinsidethehomogeneouspartofanNMR
49
-
50
51spectrometer(,KEA2100MHz,MAGRITEK,Aachen,Germany).
52
,a
54
55home-builtpermanentmagnet-system(B0=)
56homogeneityandfieldstrengthofthismagnetwasinsufficientforspectroscopyexperiments,
57
58whichwerethereforedoneataspecialsplit-coilsuperconductingmagnetatthe
59
60ForschungszentrumJülich(B0=).
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3AllglassandmetalpartsthatareincontactwiththeHP-gaswerecarefullycleanedbya
4
5universaldetergentsolution(MucasolfromMERZHYGIENEGmbH,Frankfurt,Germany),
6
7rinsedseveraltimeswithwaterandbakedoutinavacuumovenat150°
8treatedidenticallybutbakedoutattemperaturesofabout100°C.
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:Schematicdrawingofthesetupseparatedintosixfunctionalunits:a)pressureunittocontrol
35thecompressorb)compressor(twotypesareusedofwhichonlytheTedlarbagcompressor
36
37isshown)c)polarizertogenerateHP-Xe11whichismanuallytransportedtod)(dashed
38
39arrow).d)Evacuationandgasmixingstage,e)NMRspectrometer,f)membraneunitto

41
42textfordetails.
43
44

46
47
Whiledialysismembranes12areswollenpolymerswhicharesemipermeabletoseparate
48
49
50moleculesfromaliquidcarrier,oxygenationmembranessimplyincreasetheinterfacebetween
-sizescaffoldto
52
53reducetheindividualinterfacesperpore().Theporesizesshouldbeaslarge
54
55aspossibletoachievefastgasexchangebutsmallenoughtomechanicallystabilizethe
56
,theessentialparametertoavoidliquid-leakageintothegas-part
57
58
59
60
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Niederlä-Xeviamembranes5/24
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4
5range20-40barsandhencefourordersofmagnitudehigherthantheoppositeleakageofgas
6
7(bubbles)
8clotting(causingembolism),thepressuredifferenceonsuchmembranesshouldnotexceed15
9
-pressureonthegassideisrealizedbyaspecial
11
12compressor,whichisdescribedinthefollowingsection.
13
14About40ofsuchhollow-fibermembranes(outerdiameter244µm,wallthick

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