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Inorganics2020,8,19;doi:10.3390/inorganics8030019www.mdpi.com/journal/inorganics
Review
Metal–DithioleneBondingContributionsto
PyranopterinMolybdenumEnzymeReactivity
JingYang
1
,JohnH.Enemark
2
andMartinL.Kirk
1,
*
1
DepartmentofChemistryandChemicalBiology,TheUniversityofNewMexico,MSC032060,
Albuquerque,NM87131‐0001,USA;yangjing@unm.edu
2
DepartmentofChemistryBiochemistry,UniversityofArizona,Tucson,AZ85721,USA;
jenemark@email.arizona.edu
*Correspondence:mkirk@unm.edu;Tel.:+1‐505‐277‐5992
Received:2February2020;Accepted:2March2020;Published:5March2020
Abstract:Herewehighlightpastworkonmetal–dithioleneinteractionsandhowtheunique
electronicstructureofthemetal–dithioleneunitcontributestoboththeoxidativeandreductivehalf
reactionsinpyranopterinmolybdenumandtungstenenzymes.Themetallodithioleneelectronic
structuresdetailedherewereinterrogatedusingmultiplegroundandexcitedstatespectroscopic
probesontheenzymesandtheirsmallmoleculeanalogs.Thespectroscopicresultshavebeen
interpretedinthecontextofbondingandspectroscopiccalculations,andthepseudo‐Jahn–Teller
effect.Thedithioleneisauniqueligandwithrespecttoitsredoxactivenature,electronicsynergy
withthepyranopterincomponentofthemolybdenumcofactor,andtheabilitytoundergochelate
ringdistortionsthatcontrolcovalency,reductionpotential,andreactivityinpyranopterin
molybdenumandtungstenenzymes.
Keywords:metal–dithiolene;pyranopterinmolybdenumenzymes;fold‐angle;tungstenenzymes;
electronicstructure;pseudo‐Jahn–Tellereffect;thione;molybdenumcofactor;Moco
1.Introduction
Itisnowwell‐establishedthatallknownmolybdenum‐containingenzymes[1–3],withthesole
exceptionofnitrogenase,containacommonpyranopterindithiolene(PDT)(Figure1)organic
cofactor(originallycalledmolybdopterin(MPT)),whichcoordinatestotheMocenteroftheenzymes
throughthesulfuratomsofthedithiolenefragment.Todate,thePDTcomponent[4]ofthe
molybdenumcofactor(Moco)istheonlyknownoccurrenceofdithioleneligationinbiological
systems.Thiscofactorisalsofoundinanaerobictungstenenzymes,anditmaybeoneofthemost
ancientcofactorsinbiology[5].Thestudyofmetal–dithiolenecompounds(metallodithiolenes)has
undergonearecentrenaissance,withtheirsynthesis,geometricstructure,spectroscopy,bonding,
andelectronicstructurehavingbeenrecentlyhighlighted[4,6–20].Here,webrieflyreviewthe
discoveryofmetallodithiolenecompounds[13,21].Thishistoryisfollowedbyamoreextensive
discussionofkeyinvestigationsintothemyriadrolesofthedithioleneligandsinthestructure,
bondingandreactivityofmetalcompounds,usingmultiplespectroscopictechniques,aswellas
theoreticalcalculations.Throughoutthisreview,thekeyimplicationsoftheseresultsforMoandW
enzymesarediscussed.
Inorganics2020,8,192of14
Figure1.Thereducedtetrahydroformofthepyranopterindithiolene(PDT)coordinatedtoMointhe
molybdenumcofactor(Moco).Intheenzymes,theMoioncanredoxcyclebetweentheMoIV,MoV,
andMoVIoxidationstates.
Intheearly1960s,severalresearchgroupsreportedintenselycoloredsquareplanarmetal
complexeswithchelatingsulfur‐donorligandsthatcouldstabilizemetalcompoundsinarangeof
formaloxidationstatesrelatedbyone‐electronoxidation‐reduction(i.e.,redox)reactions(Figure2)
[22–24].McClevertygavethesenovelligandsthegeneralname“dithiolene”inordertoemphasize
theirdelocalizedelectronicstructures[25].Theseligandsarealsodescribedasbeing“non‐innocent”
duetotheparticipationofthedithioleneligandsinthemultipleone‐electronreactionsoftheirmetal
complexesandtheinabilitytoassignaspecificoxidationstatetothemetalionorthedithiolene
ligands[11].
Figure2.Squareplanermetallodithiolenecomplexes.R=CN,CH3,Ph,CF3.
Importantly,thesenon‐innocentdithioleneligandscanmodulatethenatureofthecovalent
bondingwithtransitionmetalionsviathevariousredoxstatesaccessibletothedithiolene(Figure3)
[13].Theene‐1,2‐dithiolateisthereducedformoftheligandandpossessessixπ‐electrons.Thisligand
formisbothaσ‐donorandπ‐donorthatusuallyformsstrongcovalentbondswithanoxidized
transitionmetalion,asisobservedintheactivesitesofmostpyranopterinMoandWenzymes(e.g.,
Mo(V)/Mo(VI)‐dithiolenebonds).Theradicalanionformwithfiveπ‐electronsisusuallyfoundin
moleculeschelatedbymultipledithioleneligands,whereextendeddelocalizationoftheπ‐electrons
andmixed‐valencyassistsinthestabilizationofthemetal–ligandbonds.Thefullyoxidized1,2‐
dithioneformoftheligandpossessesonlyfourπ‐electronsandcanbedescribedbytworesonance
structures(e.g.,the1,2‐dithioneand1,2‐dithiete).Thelow‐lyingemptyπ*orbitalsoftheS=Cbonds
inthedithionecanacceptπ‐electrondensityfromelectron‐richlow‐valenttransitionmetals[16,17],
therebystabilizingsuchcompounds.However,dithione‐containinglow‐valentmetalcomplexesare
encounteredmuchlessfrequentlythanhigh‐valenttransitionmetalionscoordinatedbyreduced
formsofdithioleneligands.
Figure3.Dithioleneredoxstatesandresonancestructuresfortheoxidizeddithione/dithieteforms.
(AdaptedwithpermissionfromInorganicChemistry,2016,55,785–793.Copyright(2016)American
ChemicalSociety).
Inorganics2020,8,193of14
In1982,JohnsonandRajagopalanproposedthatMococonsistedoftheMoioncoordinatedby
thedithiolenefragmentofthePDT(Figure1),fromtheresultsofanelegantseriesofdegradative,
analyticalandspectroscopicstudiesofsulfiteoxidase[26].Thisproposedstructurewassubsequently
confirmedbyX‐raycrystallography[27,28],andnumerousexamplesarenowknown[29].
Molybdenumandtungstenenzymesaretheonlyknownexamplesofdithiolenecoordinationin
biology,andgiventhe“non‐innocent”behaviorofdithioleneligandsinsimplemetalcompounds,
onemayaskwhatroledoesdithiolenecoordinationplayinmolybdenumenzymes?Throughaseries
ofexamplesinvolvingsmallmoleculesandenzymes,wewilladdressthisimportantquestionand
howitrelatestocontrolofmetal–ligandcovalency,reductionpotentials,andreactivityin
pyranopterinMoandWenzymes.
2.Mo–DithioleneBonding
2.1.EarlyDescriptionsofMo–DithioleneBonding
Someinsightintotheroleofdithiolenecoordinationinenzymesisprovidedbythe
organometalliccompoundsofthegeneralformulaCp2M(bdt),whereCpisC5H5−,andMiseitherMo,
VorTi.Thefoldangleofthedithioleneliganddependsontheformald‐electroncountofthemetal,
andthisanglerangesfromnearlyplanar(9°)forMo(d2),to35°forV(d1),and46°forTi(d0)(Figure
4).LauherandHoffman[30]relatedthisincreaseinthefoldanglewithdecreasedd‐electroncount
todonationfromthefilledout‐of‐planeSπ+orbitaltothein‐planemetald‐orbital(Figure5).Forthe
molybdenumenzymes,thesemodelcompoundresultsimplythattheMo–dithiolenefoldanglein
MococouldberelatedtotheformaloxidationstateoftheMoatom,withMo(VI)(d0)sitespossessing
arelativelylargefoldangleandMo(V)(d1)andMo(IV)(d0)sitespossessingsmallerfoldangles.
Accuratefoldanglesaredifficulttodetermineforlargeproteinmolecules,butvaluesrangingfrom
6–33°havebeencalculatedforvariousmolybdenumenzymes[31].Thebindingofsubstrateor
inhibitors,and/ordynamicconformationalchangesintheprotein,areexpectedtomodulatethe
activesitechelatefoldangleandtherebyaffectenzymereactivity[4,32].
Figure4.Foldangledistortionsasafunctionofredoxorbitalelectronoccupancyinaseriesof
Cp2MIV(bdt)complexes.(AdaptedwithpermissionfromJ.Am.Chem.Soc.2018,140,14777–14788.
Copyright(2018)AmericanChemicalSociety).
Figure5.Pictorialdescriptionofhowtheligandfoldanglemodulatesthedegreeofmixingbetween
thedithioleneout‐of‐planeSorbitals(Sπ+)andthein‐planeMo(xy)redoxorbital.Thechelateringfold
Inorganics2020,8,194of14
isalongthedithioleneS–Svector.(AdaptedwithpermissionfromProc.Natl.Acad.Sci.USA.2003,
100,3719–3724.Copyright(2003) NationalAcademyof Sciences.
2.2.SpectroscopicInvestigationsofMo–DithioleneBonding
2.2.1.ElectronParamagneticResonance(EPR)Spectroscopy
Animportantspectroscopicsignatureofmolybdenumenzymes,suchasxanthineoxidaseand
sulfiteoxidase,isauniqueMo(V)electronparamagneticresonance(EPR)spectrum.TheEPRspectra
oftheenzymesdisplayarelativelylargeaverageg‐value(gave=1.97)andrelativelysmall95,97Mo
hyperfineinteractions(hfi)comparedtotheEPRspin‐Hamiltonianparametersfromtypicalinorganic
Mo(V)complexesthatpossesshardN,O,andCldonorligands.TheuniqueEPRparametersfor
molybdenumenzymeshavebeenascribedtocovalentdelocalizationofelectrondensitybetweenthe
Mo(V)centerandthesulfuratomsofthecoordinatedpyranopterindithioleneunit[33].Theoxo‐
Mo(V)modelcompoundTp*MoO(bdt)(Figure6,whereTp*ishydrotris‐(3,5‐dimethyl‐1‐
pyrazolyl)borateandbdtis1,2‐benzenedithiolate))displaysMo(V)EPRspin‐Hamiltonian
parametersthatareverysimilartothoseobservedintheenzymes.Thissupportstheproposalof
dithiolenecoordinationinMoenzymes[34],whichhasbeenconfirmedbyX‐raycrystalstructures
[2].RecentmultidimensionalvariablefrequencypulsedEPRstudiesofsulfiteoxidase,wherethe
sulfuratomsofMocohavebeenisotopicallylabeledwith33S(I=3/2),haveprovideddirect
experimentalevidencefordelocalizationofMo(V)spindensityontotheSatomsofthedithiolene
fragmentofMoco[35,36].Densityfunctionaltheory(DFT)computationsshowspinpolarization
effectsandstrongcovalentintermixingbetweenthein‐planemetaldxyorbitalandout‐of‐planepz
orbitalsofthePDTdithioleneSatoms,whichprovideamechanismfortheobservationofasignificant
33Shyperfineinteraction[12,36].
Figure6.TheTp*MoVO(bdt)model.Notethattheapicaloxoligandcanbechangedtoaterminal
sulfidoornitrosyltoprobetheelectronicstructureoftheMo–dithioleneunit.Thebdtligandcanalso
beconvenientlyinterchangedwithalargevarietyofotherdithiolenes.
2.2.2.ElectronicAbsorptionandResonanceRamanSpectroscopies
ExperimentalinvestigationoftheelectronicstructuresoftheMocentersofenzymesisdifficult
becauseoftheintenseabsorptionsfromotherchromophores(e.g.,theb‐typehemeinsulfiteoxidase
andironsulfurcentersandFADinxanthineoxidase)[37–41].However,theeffectsofdithiolene
coordinationonelectronicstructurehavebeeninvestigatedformodeloxo‐Mo(V)compounds(Figure
6)byelectronicabsorption,XAS,magneticcirculardichroism(MCD),and resonanceRaman(rR)
spectroscopies[12,14–17,32,33,42–51].ForTp*MoO(bdt),theelectronicabsorptionsat19,400cm−1
(Band4)and22,100cm−1(Band5)areassignedtoS➝Mochargetransferbands(Figure7A)[12].
TheseassignmentshavebeenconfirmedbyrRspectroscopy(Figure7A,B),whichshowsthree
resonantlyenhancedvibrationsat362.0,393.0,and931.0cm−1.Thelowerfrequencyvibrations(ν1and
ν6)canbeassignedtosymmetricS–Mo–Sstretchingandbendingvibrations,andthe931.0cm−1
frequency(ν3)isprimarilytheMo≡Ostretch.Figure7Cshowsamolecularorbitaldiagramthatis
consistentwiththespectroscopicdataofFigures7A,B.Band5ofFigure7Aisassignedas𝜓opa”➝
𝜓xza”,𝜓yza’(bluearrow,Figure7C),atransitionwhichformallyresultsinthepromotionofanelectron
fromanout‐of‐planedithiolenemolecularorbitaltothenearlydegenerateModxz,yz‐basedorbitals,
whicharestronglyantibondingwithrespecttotheapicalMo≡Obond.Thisbandassignmentis
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supportedbytherRenhancementofν
3
(squares)withexcitationintoBand5(Figures7A,B).The
preferentialenhancementofvibrationsν
1
(diamonds)andν
6
(circles)uponexcitationat514.5nm
(Figures7A,B)supportsassignmentofBand4astheelectronictransitionψ
ipa”
➝ψ
xya’
(redarrow,
Figure7C),
whichpromotesanelectronfromtheantisymmetricin‐planedithioleneorbital(ψ
ipa”
)to
thehalf‐filledin‐planeMod
xy
(ψ
xya’
)orbital.Theintensityofthiselectronictransitionillustratesthe
covalencyofin‐planemetal–dithiolenebondingandsuggeststhatsuchapseudo‐σ‐mediatedprocess
couldplayaroleinone‐electrontransferstepsofenzymecatalysis.
Figure7.(A)SolidstateresonanceRamanprofilesand5Kmullelectronicabsorptionspectrumfor
Tp*Mo
V
O(bdt).(B)ResonanceRamanspectrumforTp*Mo
V
O(bdt)(293K)using514.5nmexcitation
(75mW).(C)GeneralmolecularorbitaldiagramforTp*Mo
V
O(dithiolene)complexes.Thez‐axisis
orientedalongtheMo≡Obondandtheenergiesofthemolecularorbitalsarenotdrawntoscale.
Transitionsaredescribedinthetext.(AdaptedwithpermissionfromInorganicChemistry,1999,38,
1401.Copyright(1999)AmericanChemicalSociety).
3.SynergisticInteractionsbetweentheDithioleneandPterinComponentsofthePDT
ElectroniccouplingbetweenthedithioleneandthepterincomponentsofthePDTismost
prevalentinthedihydropyranopterinformofthePDT[4,15,20,29,52].Thiscouplingisdramatically
reducedinatetrahydropyranopterinduetothelossofextendedπ‐conjugationinthesesystems.
Two‐electronoxidationofthetetrahydropyranopterincomponentofthePDTcanresultinan
unusualasymmetricdithioleneknownasthe“thiol–thione”formthatleadstobondandelectronic
asymmetryinthemetal–dithiolenecore[4,15,52].AsdepictedinFigure8,thetwo‐electronoxidized
10,10a‐dihydropyranopterincanundergoaninducedinternalredoxreactionuponprotonationatthe
N‐5positionthatinvolvesasubsequentchargetransferbetweenthedithiolenechelateandthe
piperazineringofthepterin.Thisprotonationresultsinadominantmonoanionicthiol–thionechelate
formoftheligandwhenboundtoMoorW.Thisthiol–thionecharactercanalsooccurintheabsence
ofprotonationbytheconceptofresonance,whichmayalsobedescribedasconfigurationalmixing
betweenthethiol–thioneanddithiolstates.Thistypeofthiol–thionechelatehasbeenobservedand
studiedinasmallmoleculeMo(IV)systems[4,15,20,52].Inthesesystems,excitedstatethiol–thione
characterwasshowntobeadmixedintothegroundstateconfigurationusingavarietyof
spectroscopicandcomputationalprobesoftheelectronicstructure.Theanalysisofthedataindicates
Inorganics2020,8,196of14
thatatwo‐electronoxidizedpterinisinherentlyelectronwithdrawing,allowingforalow‐lying
dithiolene→ pterinintraligandchargetransfer(ILCT)statetomixwiththegroundstatetoprovide
avariabledegreeofthiol–thionecharacterintheelectronicgroundstate.
(a)(b)
Figure8.OxidizedPDTligands:dihydropyranopterin(a)andprotonateddihydropyranopterin(b)
yieldingthethiol/thione.
Definitivespectroscopicsignaturesareassociatedwiththepresenceofadihydropterinformof
thePDTligand.Itisobservedthatthedithiolene→ pterinintraligandchargetransfer(ILCT)bandis
intense(E=20,000–27,500cm−1;ε~10,000–16,000M−1cm−1)[52],andthereisconsiderableresonance
enhancementofnumerousRamanvibrationsthatcanbeassignedasoriginatingfrompterinand
dithioleneC=CandC=Nvibrations.Keyresonanceenhancedvibrationalmodesthatcanbeused
tocharacterizethepresenceofdihydropterinthiol–thionecharacterintheenzymesincludethe1508
cm−1and1549cm−1pyranopterin–dithiolenestretchingfrequenciesthatwereobservedinthisMo(IV)
cyclizedpyranopterindithiolenemodelcompound.ThisoxidizedpyranringclosedformofthePDT
hasyettobedefinitivelyobservedinanypyranopterinMoenzyme,butitspresencewouldhave
profoundimplicationsontheelectronicstructureoftheMosite.Namely,thechangeinligandcharge
from−2to−1leadstoanasymmetricreductioninthechargedonatedbythemonoanionicligand
comparedtothedianionicdithiolene.Chargeeffectsonoxygenatomtransfercatalysishaverecently
beenexploredinmodelcompoundsshowingdramaticrateenhancementsintheoxidativehalf
reactionthatleadstosubstratereduction[53].Thisreactivitycorrelateswithalargeshiftinthe
Mo(VI/V)reductionpotentialbetweencationic[Tpm*MoO2Cl]+(−660mVvs.Fc+/Fc)andcharge
neutralTp*MoO2Cl(−1010mVvs.Fc+/Fc)[53].Thesameeffectonredoxpotentialandreactivity
wouldbeexpectedinenzymesthatcouldadoptanoxidizedPDTwithathiol–thioneconfiguration.
Thepresenceofathiol–thioneformofthePDTinanenzymewouldalsohaveaconsiderableimpact
ontheactivesiteelectronicstructure,andenablethepyranopterintoplayamoresignificantrolein
catalysisbyfine‐tuningtheMoredoxpotentialandprovidingaπ‐pathwayforelectrontransfer
regenerationoftheactivesite[52].Additionally,theasymmetryinthedithiolene(thiol/thione)charge
donationwouldbeexpectedtoresultinasignificanttranseffectortransinfluenceonoxoorsulfido
ligandsthatarecoordinatedtotheMoorWionandorientedtranstothethionesulfur.
4.TheElectronicBufferEffectandFoldAngleDistortions
4.1.PhotoelectronSpectroscopy(PES)Studies
AcommonstructuralfeatureofthelargegroupofpyranopterinMoenzymesthatcatalyzea
widerangeofoxidation/reductionreactionsincarbon,sulfur,andnitrogenmetabolismis
coordinationbythesulfuratomsofone(ortwo)uniquedithiolenegroupsderivedfromtheside
chainofanovelsubstitutedpterin(PDT,Figure1).Giventheelectroniclabilityofthedithiolene,a
possibleroleofdithiolenecoordinationinmolybdoenzymesistobuffertheinfluenceofotherligands
andchangesintheformaloxidationstateofthemetal.Gas‐phasephotoelectronspectroscopy(PES)
isapowerfultoolforprobingmetal–ligandcovalencyinisolatedmolecules.Gas‐phaseultraviolet
PESofthemolybdenummodelcomplexeswiththegeneralformulaTp*MoE(tdt)(Figure6,whereE
=O,S,orNO,andtdt=3,4‐toluenedithiolate),exhibitnearlyidenticalfirstionizationenergies(6.88–
6.95eV)eventhoughthereisadramaticdifferenceintheelectronicstructurepropertiesoftheaxial
ligand.Collectively,theseresultshaveprovideddirectexperimentalevidenceforthe“electronic
buffer”effectofdithioleneligands[54].
Additionalevidencefortheelectronicbuffereffectofdithioleneligandshasbeenprovidedby
gas‐phasecoreandvalenceelectronionizationenergymeasurementsoftheseriesofmolecules
Inorganics2020,8,197of14
Cp2M(bdt)(Figure4,Cp=η
5‐cyclopentadienyl,M=Ti,V,Mo,andbdt=benzene‐1,2‐dithiolate).
Comparisonofthegas‐phasecoreandvalenceionizationenergyshiftsprovidesaunique
quantitativeenergymeasureofvalenceorbitaloverlapinteractionsbetweenthemetalandthesulfur
orbitalsthatisseparatedfromtheeffectsofchargeredistribution.Theresultsexplainthelarge
amountofsulfurcharacterintheredox‐activeorbitalsandtheelectronicbufferingofoxidationstate
changesinmetal–dithiolenesystems.Theexperimentallydeterminedorbitalinteractionenergiesalso
revealapreviouslyunidentifiedoverlapinteractionofthepredominantlysulfurHOMOofthebdt
ligandwiththefilledπorbitalsoftheCpligands,suggestingthatdirectdithioleneinteractionswith
otherligandsboundtothemetalcouldbesignificantforothermetallodithiolenesystemsinchemistry
andbiology[55].
4.2.ALargeFoldAngleDistortioninaMo(IV)–DithioneComplex
Mo(IV)–dithionecomplexesaremuchrarerthanMo(V)/Mo(VI)‐dithiolenecomplexes.Recently,
adetailedspectroscopicandcomputationalstudywasperformedonanovelMo(IV)–dithione
complex,MoO(SPh)2(iPr2Dt0)(whereiPr2Dt0=N,N′‐isopropylpiperazine‐2,3‐dithione)[17].The
structureofthisunusualmoleculewasdeterminedbyx‐raycrystallographyanddisplaysa
remarkablylargedithiolenefoldangle(η=70°).Thislargefoldanglewascomparedtothatobserved
inmorethan75othermetallodithiolenecomplexesfoundintheCambridgecrystallographic
database,wherefoldangleswerefoundtorangefrom0.3°to37.3°withanaveragevalueforηof
12.5°[17].ThelargefoldangledistortioninthemetallodithioleneringofMoO(SPh)2(iPr2Dt0)is
reflectedinitsunusualelectronabsorptionspectrum.ThecombinationofanelectronrichMo(IV)
centerandelectrondonatingthiolate(SPh)ligandsresultsinthepresenceoflow‐energyMo(IV)d(x2‐
y2)➝dithioneMLCTandthiolate➝dithioneLL’CTtransitionsasaresultofthestrongπ‐acceptor
characterofthedithioneligand.ThesespectralassignmentsaresupportedbyresonanceRaman
profilesconstructedforthe378cm−1S–Mo–Ssymmetricstretchandthe945cm−1MoOstretchin
additiontotheresultsofTDDFTcomputations.Thedonor–acceptornatureofthecomplexwas
revealedinamolecularorbitalfragmentsanalysisusingadonorfragment,[(PhS)2Mo(IV)]2+(F1)and
anacceptorfragment,[iPr2Dt0](F2).Theanalysisshowedthat21%oftheF1HOMOwasmixedinto
theF2fragmentLUMOata70ofoldangle.Incontrast,only5%oftheF1HOMOwasmixedintoF2
fragmentLUMOinaplanerconfiguration(η=0°),correlatingtheeffectiveπ‐acceptorabilityofthe
dithionewiththeligandfoldangle.TheeffectsofthisHOMO‐LUMOmixingalsoaffectstheHOMO‐
LUMOgap,withtheHOMO‐LUMOgapincreasingatlargerfoldangles(Figure9).Theincreased
covalencythatresultsfromthefoldangledistortionrepresentsanexampleofastrongpseudo‐Jahn–
Tellereffect,videinfra,involvingvibroniccouplingbetweenthegroundstateandalow‐energy
excitedstateinthenon‐distorted(η=0°)geometryofthismolecule.Ascanofthepotentialenergy
surfaceasafunctionofthisfoldangledistortioncoordinateresultsinanasymmetricdoublewell
potential(Figure10),withtheglobalminimumrepresentingagroundstategeometrywiththe
dithioneligandfolddistortedtowardtheapicaloxoligand.Thus,anoxidizeddithioneformofthe
PDTpresentinanenzymeactivesitewouldbeexpectedtopossessaverylargeligandfoldangle,
unlessthepolypeptideenforcesamoreplanerfoldanglegeometry.
Inorganics2020,8,198of14
Figure9.FrontierorbitalenergiesasafunctionoffoldangleinMoIVO(SPh)2(iPr2Dt0),whichpossesses
adithioneπ‐acceptorligand.(AdaptedwithpermissionfromInorganicChemistry,2016,55,785–793.
Copyright(2016)AmericanChemicalSociety).
Figure10.AdoublewellinthegroundstatepotentialenergysurfaceofMoIVO(SPh)2(iPr2Dt0)asa
functionoftheligandfoldangle.(AdaptedwithpermissionfromInorganicChemistry,2016,55,785–
793.Copyright(2016)AmericanChemicalSociety).
4.3.Low‐FrequencyPyranopterinDithioleneVibrationalModesinXanthineOxidase/Dehydrogenase
Low‐frequencydithiolenedistortionsthatarecoupledtolargeelectrondensitychangesatthe
Moionrepresentanexampleoftheelectronicbuffereffect[54],andhavebeenprobedinbovine
xanthineoxidase(XO)andR.capsulatusxanthinedehydrogenase(XDH)usingresonanceRaman
spectroscopy[40].Computationshaveshownthatexcitingintoalow‐energyMo(IV)→product
metal‐to‐ligandchargetransfer(MLCT)bandresultsinalargedegreeofchangetransferfromthe
Mo(IV)HOMOtotheproductLUMO,resultinginanexcitedstatewithsignificantMo(V)hole
character(e.g.,Mo(IV)–P0→Mo(V)–P∙).Thus,theopticalchargetransferprocessmimicsthe
instantaneousone‐electronoxidationoftheMoion,whichisencounteredintheelectrontransfer
reactionsoftheenzymes.
TheMo(IV)→2,4‐TVandMo(IV)→4‐TV(2,4‐TV=2,4‐thioviolapterin;4‐TV=4‐thioviolapterin)
MLCTbandsarered‐shiftedrelativetotheMo(IV)→violapterinMLCTband[39,40,56–59].Thered‐
shiftoftheMoIV–2,4‐TVandMoIV–4‐TVMLCTbandseliminatesspectraloverlapwiththeabsorption
envelopeofthe2Fe–2SspinachferredoxinclustersandFAD.TheeliminationoftheFADfluorescence
backgroundandspurioussignalsderivingfrom2Fe–2SvibrationscontributingtotheRaman
spectrumallowfortheacquisitionofveryhigh‐qualityresonanceRamandata.Multiplelow‐
frequency(200–400cm−1)Ramanvibrationsareobservedtobeenhancedwhenusinglaserexcitation
onresonancewiththeMo(IV)→productMLCTband[40],andthesehavebeenassignedasa
vibrationalmodeinvolvingdithiolenefolding,Mo≡Orocking,andpyranopterinmotions(BandA:
MoIV–4‐TV=234cm−1;MoIV–2,4‐TV=236cm−1),aringdistortionvibrationthatpossessesbothMo–
SHandpyranopterinmotions(BandB:MoIV–4‐TV=290cm−1;MoIV–2,4‐TV=286cm−1),thesymmetric
S–Mo–Sdithiolenecorestretchingvibration(BandC:MoIV–4‐TV=326cm−1;MoIV–2,4‐TV=326cm−1),
andthecorrespondingasymmetricS–Mo–Sdithiolenestretch(BandD:MoIV–4‐TV=351cm−1;MoIV–
2,4‐TV=351cm−1)(Figure11).Thus,theinstantaneousgenerationofaholeontheMocenter(Mo(IV)–
P0→Mo(V)–P∙)byphotoexcitationisfeltbythedithiolenechelateandextendsallthewaytothe
aminoterminusofthePDT.ThemostresonantlyenhancedmodeinthisspectralregionisBandC,
thesymmetricS–Mo–Sdithiolenecorestretching,andthefrequencyofthismodeandBandDare
similartothoseobservedinTp*MoO(bdt)[12,32],whichwereassignedasthechelateringsymmetric
S–Mo–Sstretchingandbendingvibrations,respectively.BandAissignificant,sinceitpossesses
dithioleneringfoldingcharacterindicatingthatelectrondensitychangesatMoarebufferedbya
distortionalongthislow‐frequencycoordinate,ashasbeenobservedinthevariousmodelsystems
describedinthisreview.TheseobservationsstronglysupportanelectrontransferroleforthePDTin
catalysis,withthedithiolenecontributingtotheMo–Scovalencynecessaryforincreasingthe
Inorganics2020,8,199of14
electroniccouplingmatrixelementforelectrontransfer(H
DA
)andtoaffecttheMoreductionpotential
viathecovalencyintheMo–S
dithiolene
bonds.
(a)(b)
Figure11.Low‐frequencyrRspectraforwt,Q102G,andQ197AXDH,Mo
IV
−4‐TV(a)andMo
IV
−2,4‐
TV(b).RamanspectrawerecollectedonresonancewiththeMo(IV)→ PMLCTbandusing780nm
laserexcitation(AdaptedwithpermissionfromInorganicChemistry,2017,56,6830–6837.Copyright
(2017)AmericanChemicalSociety).
5.VibrationalControlofCovalency
AcombinationofMCD,electronicabsorption,electronparamagneticresonance,resonance
Raman,andphotoelectronspectroscopieshasbeenusedinconjunctionwiththeorytoreveal
vibrationalcontrolofmetal–ligandcovalencyinaseriesofCp
2
M(bdt)complexes(M=Ti,V,Mo;Cp
=η
5
‐C
5
H
5
)[60](Figure4).Theworkisimportantbecauseithasallowedforadetailedunderstanding
ofhowredoxorbitalelectronoccupancy(Ti(IV)=d
0
,V(IV)=d
1
,Mo(IV)=d
2
,)affectsthenatureofthe
M–dithiolenebondingschemeatparityoftheligandsetandatparityofcharge.Inthisseriesof
complexes,largechangesinthemetallodithiolenefoldangleandelectronicstructureareobservedas
electronsaresuccessivelyremovedfromtheredoxorbital(Figure4).Theseelectronoccupancyeffects
onthefoldangledistortionarenowunderstoodintermsofthepseudo‐Jahn–Tellereffect(PJT).PJT‐
derivedmoleculardistortionsoriginatefromthemixingoftheelectronicgroundstate(Ψ
0
)with
specificexcitedstates(Ψ
i
)[61,62].Thegroundstate–excitedstateenergygap(2Δ),thematrixelements
(F
0i
)ofthevibroniccontributiontotheforceconstant(F),andtheprimarynon‐vibronicforceconstant
(K
0
)allgovernthedegreeoftheligandfolddistortionaccordingto:
𝐹
𝛹
𝜕𝐻 𝜕𝑄
𝛹
(1)
𝐹
∆∙𝐾
(2)
AtthecriticalthresholddefinedbyEquation(2),themetallodithiolenecentersofCp
2
M(bdt)can
distortalongthedithiolenefoldanglecoordinatetoyieldadoublewellpotentialenergysurface
(Figure12),andthemagnitudeofthePJTdistortionismaximizedbyalargeF,asmallΔ,andasmall
K
0
.Thus,thePJTdistortionintheseCp
2
M(bdt)complexeseffectivelycouplessoftfoldanglebending
modesintheM‐dithiolenechelateringtotheinherentelectronicstructureofthesystemviathed‐
electroncount.Importantly,themixingoflow‐energychargetransferstatesintothegroundstateby
thePJTeffectcontrolsthecovalencyoftheM–Sbonds.
OneoftheuniqueaspectsofMo–SandW–Sbondingisthesmallenergygapbetweenfilled
dithiolene‐basedorbitalsandthelowestenergymetal‐basedorbital,whichnaturallyleadstolow‐
energychargetransferstatesthatcanmixwiththegroundstate.Modesofteningalongthedithiolene
foldcoordinateisimportantinpyranopterinMoandWenzymessincethisleadstoapotentialenergy
surfacewherealargerangeofdithiolenefoldanglesmaybesampledwithoutpayingaprohibitive
energypenalty.ThiseffectismaximizedwhenF
2
≅Δ∙K
0
.Thus,alow‐energypathwayisoperative
thatcanminimizeenergeticallyunfavorablereorganizationalenergycontributionsalongthereaction
coordinate,whichaccompanyredoxchangesatthemetalion.Asmentionedpreviously,thesefold
Inorganics2020,8,1910of14
angledistortionshavebeenshowntobekinematicallycoupledtolowfrequencypyranopterinmodes
inXOandcontributetolow‐energybarriersforelectrontransferregenerationoftheactivesite.
However,intheenzymestheremaybeeitheracompetingoradditiverelationshipbetweenactive
sitedistortionsthataredrivenviathed‐electroncountofthemetalionanddistortionsthatare
imposedbytheprotein.Vibroniccouplingeffectsthatderivefromdifferentoccupancynumbersfor
theredox‐activeorbitalwillfunctiontomodulatetheenzymereductionpotentialintheoxidative
andreductivehalfreactionsofpyranopterinMoandWenzymes,andthisoccursbymodulatingthe
degreeofmetal–ligandcovalencyvialow‐frequencydistortionsattheactivesite.
Figure12.Theexcitedstate(black)andgroundstate(red)potentialenergysurfacesassociatedwith
varyingvaluesofF2(Dotted:F2=0,solid:F2=Δ∙K0,dashed:F2=2Δ∙K0)WhentheconditionF2>Δ∙K0
ismetoneobservesthatthesingle‐wellgroundstatepotentialenergysurfacedistortsintoadouble‐
wellpotential.TheF2>Δ∙K0criteriadescribeastrongPJTeffect.(AdaptedwithpermissionfromJ.Am.
Chem.Soc.2018,140,14777–14788.Copyright(2018)AmericanChemicalSociety).
6.Conclusions
Thisreviewfocusesontheelectronicstructures,molecularstructures,andspectroscopic
propertiesofwell‐characterizedmetallodithiolenecompoundsinordertoprovidedeepinsightinto
therole(s)ofmetal–dithiolenebondinginpyranopterindithiolenecontainingenzymes(Figure1).
Thediscovery,intheearly1960s,thattransitionmetaldithiolenecompoundsundergoaseriesofone‐
electronoxidation‐reductionreactions(Figure2),providedthefirstevidenceforthe“non‐innocence”
ofdithioleneligandsandthehighlycovalentnatureofmetal–dithiolenebonding.Additionallinks
betweenmetal–dithiolenecovalencyandelectronicandmolecularstructurewerepositedfrom
theoreticalstudiesofbentmetallocene−dithiolenecompounds(Figure4)byLauherandHoffmanin
1976[30],whorelatedmetal−dithiolenechelatering“folding”withthemetaliond‐electron
configuration.InvestigationsofModithiolenecompoundsbyelectronicabsorption,resonance
Raman,andEPRspectroscopiesshowedthatS➝Mochargetransferbandsdominatethevisible
spectrumandthatthereissubstantialdelocalizationofspindensityontotheSatomsofthedithiolene.
Recentcomprehensivestudiesofbentmetallocene−dithiolenecompoundshaveshownthatlow‐
energyligandfolddistortionsarisefromapseudo‐Jahn−Teller(PJT)effect,whichinvolvesvibronic
couplingoftheelectronicgroundstatewithelectronicexcitedstatestocontrolmetal−ligand
covalency[60](Section5).Thisvibroniccouplingprocessmayplaycriticalrolesinthecatalyticcycles
ofpyranopterinMoandWenzymesbydynamicand/orstaticmodulationofredoxpotentialsand
providingasuperexchangepathwayforelectrontransferthroughthePDTframework.However,
greaterunderstandingofhowgeometricandelectronicstructurecontrolreactivity,anddefine
functioninMoandWenzymes,willrequirelinkingtheconceptsthathavebeendevelopedfor
metallodithiolenestotheemergingresultsfromstudiesofwell‐characterizedcompoundsthatmimic
thepterincomponentofPDT(Section3).Exploringthesynergisticinteractionsbetweenthe
dithioleneandpterincomponentsofthePDTandthemetalionwillbechallenging,butsuchresearch
promisestoprovideimportantinsightsintothesecriticallyimportantenzymes.
AuthorContributions:J.H.E.,J.Y.,andM.L.K.collectivelyconceivedanddraftedthisarticle.Allauthorshave
readandagreedtothepublishedversionofthemanuscript.
Inorganics2020,8,1911of14
Funding:M.L.K.’sresearchcontributionstothisarticlewerefundedbytheNationalInstitutesofHealth(R01‐
GM‐057378).
ConflictsofInterest:Theauthorsdeclarenoconflictofinterest.
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