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Contents - Max-Planck-Institut für Physik komplexer Systeme

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1.10 AdvancedStudyGroups<br />

AdvancedStudyGroup2010:UnconventionalMagnetisminHighFields<br />

(Convenor:Dr.MikeZhitomirsky)<br />

TheAdvancedStudyGroup(ASG)“UnconventionalMagnetisminHighFields”wasinstalledforafivemonthperiodfromApriltoSeptember,2010withtheaimtoinvestigatenovelfield-inducedphenomena<br />

ingeometricallyfrustratedandquantummagnets. TheASGactivitywascoordinatedwiththeDivision<br />

ofCondensedMatterandtheresearchgroup“NewStatesofQuantumMatter.”Asecondgoalwasto<br />

promotescientificcollaborationwithexperimentalgroupsfromtheDresdenHighMagneticFieldLaboratory(HMD),the<strong>Max</strong>Plank<strong>Institut</strong>eforChemicalPhysicsofSolids(MPI-CPfS),andthe<strong>Institut</strong>e<br />

forSolidStateandMaterialResearch(IFW).ThegroupmemberswereAndreyChubukov(University<br />

Wisconsin-Madison),PeterHoldsworth(ENS,Lyon),FredericMila(EPFL,Lausanne),andMikeZhitomirsky(C.E.A.,Grenoble).<br />

InadditiontheASGhosted30long-andshort-termvisitors. Aspecial<br />

seminarserieswasorganizedatthe mpipkswithmorethan25presentationsgivenbyourmembersand<br />

visitors,aswellasbyinvitedspeakersfromtheneighboringinstitutes.A.Chubukovwasalsooneofthe<br />

scientificcoordinatorsoftheworkshopon“EmergentQuantumStatesinComplexCorrelatedMatter”<br />

thattookplaceatthe mpipksonAugust23–27,2010.Principaldirectionsofresearchwereasfollows:<br />

Quantumspin-nematicstate. Enhancedquantumfluctuationsmaydestroyconventionallong-range<br />

magneticorderandstabilizeaspinanalogofliquidcrystals—astatewithpartiallybrokenrotational<br />

symmetrycharacterizedbytensororderparameter.Suchanewillusivestateofmatterhasattracteda<br />

lotoftheoreticalinterestinthepast,buthasneverbeendiscoveredsofarinrealmaterials.Motivated<br />

byanumberofrecentlystudiedfrustratedmagneticmaterialsweexploreanewroottothespin-nematic<br />

phasebasedontheformationofboundmagnonpairsinquantumantiferromagnetswithcompeting<br />

antiferro-andferromagneticinteractions[1],seealsotheresearchpart2.Theboundmagnonstatesare<br />

formedinthefullypolarizedphaseinhighmagneticfieldsandundergoaBosecondensationtransition<br />

withdecreasingfieldpriortotheconventionalsingle-magnoncondensation.Theresultingcondensateof<br />

magnonpairshasdirectsimilaritieswiththeCooperpaircondensateinsuperconductors.Inaddition,the<br />

paircondensateremainsinvariantunder π-rotationaboutthefielddirectionreflectingthequadrupolar<br />

natureofitsorderparameter.Thedevelopedtheorypredictspresenceofthespin-nematicphaseinthe<br />

frustratedchainmaterial LiCuVO4. Veryrecenthigh-fieldexperimentshaveindeedfoundanewphase<br />

inthiscompoundabove40T.Wehavefurtherexaminedthestabilityofboundmagnonpairsinavariety<br />

offrustratedmodelsincludingplanarmagneticsystems,whicharenowextensivelystudiedatMPI-CPfS.<br />

Monopoledynamicsinspinice. Thefractionalizationofmagneticdipolesintofreeanddeconfined<br />

magneticcharge(monopoles)isadirectconsequenceoftheextensivegroundstatedegeneracy,which<br />

constitutesavacuumforthequasi-particleexcitations.Wehavemodeledtheacsusceptibilitymeasurementsonthespinicematerial<br />

Dy2Ti2O7bythediffusivedynamicsofthisCoulombgasofquasiparticle<br />

interactions[2]. Inparallelwiththesedevelopmentsnovelexperimentshavebeendevisedtomeasure<br />

themagneticchargeofthequasi-particlesusingtheWieneffect.Weprovidedtheoreticalsupportfora<br />

Wieneffectexperiment[3]inwhichthemagneticresponseofacrystalof Dy2Ti2O7toasmallmagnetic<br />

field(1to10Gaussonly)wasmeasuredinaSQUIDmagnetometerspeciallydesignedtodealwithvery<br />

lowfields.Theresultswereinterpretedinanalogywiththedielectricresponseofaleakycapacitor,with<br />

magneticrelaxationduetobothboundandfreemagneticcharges.Throughthisquantitativeanalysiswe<br />

wereabletoconfirmthepredictedvalueofthemagneticchargeassociatedwithaMonopoleexcitation<br />

andillustratethevalidityoftheWieneffectforthismagneticCoulombgassystem.Finally,wecontinued<br />

projectsdedicatedtothetopologicalpropertiesofthevacuumofspinicestate. Wehavepreviously<br />

shownthat,applyingabonddistortion,reducingthesymmetryofthemanifoldofvacuumstatesto Z2<br />

leadstoamulticriticalmeanfieldphasetransition.Webeganinvestigatingthefinitesizescalingbehavior<br />

ofthistransition,withparticularinterestintheidentificationofGaussianfluctuationterms[4]. This<br />

systemmapsontothesix-vertexmodel,whichintwodimensionsisintegrable. Thetransitionhasnot<br />

previouslybeeninterpretedintermsofmeanfieldandGaussianfluctuations.<br />

Unconventionalphasesofcoldatomicgasesinopticallattices. Latticespinsystemsinamagnetic<br />

fieldcanbedirectlymappedontothehard-corebosonmodelsduetotheequivalencebetween SO(2)<br />

and U(1)symmetrygroups.Generalizationoftheeffectivespininteractionfromtheconventional SU(2)<br />

tothe SU(3)symmetricpotentialwasundertakenin[5]. Itfurtherallowstheuseofspinlanguageto<br />

1.10. AdvancedStudyGroups 35

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