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1. MeasurementofMuonNeutrinoQuasi- ‐Elas9cScaLeringonaHydrocarbonTargetatEν 3.5GeVMINERvACollabora9on.May9,2013e- ‐Print:arXiv:1305.22432. MeasurementofMuonAn9neutrinoQuasi- ‐Elas9cScaLeringonaHydrocarbonTargetatEν Emodeldashedredline- ‐- ‐- ‐- ‐- ‐- ‐- ‐- ‐A.Bodek35

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.A.BodekandJ.RitchiePhys.Rev.D23(1981)Bodek107048

ConclusionsonTE/MECinQEscaLering ewdatareasonablywell.Updatedparameteriza9onA 5.19andB 2. eVtowardshigherν.TheshivsareindependentofQ2. actormodelareexpected WearecurrentlyextendingtheanalysislowerQ2( 0.3GeV2)tooverlapwithouranalysisofthelowQ2L- ‐TseparatedresultsfromCarlsonetal. )canbetested.A.Bodek49

- resultsina2ndnucleoninthefinalstatewithKE VthespectatornucleonhasKE45- thKE 48- ‐90MeV- ‐à 50

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energyis25MeVß 1p1h(FermiGas)0.8GeV/cß 2p2h(SRC)0.8GeV/ca 2.76GeV- ‐1forC12a 2.44GeV- ‐1forFe56Spectator:k2 0.3- ‐0.4GeVKE k22/2M 45- ‐80MeV0.8GeV/c]TheBodekRitchieModelIsanapproxima ontotheSpectralFunc emovalenergysincethasaspectatornucleon.57

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Relative Cross sectionRMSwidthoftheνdistribu QEscaLeringwithFermimo9onk.W2 M2W2 M2 2Mν- ‐2k*q–Q2- ‐- ‐à ν Q2/2M k*q/M ν RMS k*q3/M q3 k3 /MRMSwidthTEWithq3 {Q2(1 haslopeof k 3 /M ν RMS - ‐momentumtransfertothenucleon.{ k3 (krms)/ 3}22W (GeV )A.Bodek60

Relative Cross sectionRelative Cross edata.Weshowafewexamples:- ‐Q2 0.3GeV2ε 0.98Residual TEcontribu9on)Q2 0.3GeV2ε 0.88Residual istribu9onW (GeVQ2 0.3GeV2fortwodifferentvirtualp)hotonpolariza on–getsamesameTEA.Bodekσ σL εσT2222W (GeV )61

Q2 0.68GeV2ε 0.98Relative Cross sectionRelative Cross sectionRelative Cross sectionσ σL εσTQ2 0.65GeV2ε 0.96Residual TEcontribu9on)Q2 0.62GeV2ε 0.71Residual TEcontribu9on)Q2 0.62- ‐0.68GeV2:threedifferentvirtualphotonpolariza on–getsimilarTEA.BodekW (GeV )W (GeV ) σ σL εσT22226222W (GeV )

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Neutrino!Cross!sec9ons! ng(the(energy(dependence(of(neutrino