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Multipole Analysis of Recent Pion Electroproduction Data

We have performed a series of global and single-Q2 fits to the growing database for pion electroproduction. We compare to some other recent fits which have used different formalisms, more selective datasets, and truncated multipole expansions. We present r

February8,200823:10WSPC/TrimSize:9inx6inforProceedingsnstar02

3

002 anJ 42 3v8601030/th-lcu:nviXraMULTIPOLEANALYSISOFRECENTPION

ELECTROPRODUCTIONDATA

R.ARNDT,W.BRISCOE,I.STRAKOVSKY,ANDR.WORKMAN

CenterforNuclearStudies,DepartmentofPhysics

TheGeorgeWashingtonUniversity,Washington,D.C.20052

Wehaveperformedaseriesofglobalandsingle-Q2 tstothegrowingdatabaseforpionelectroproduction.Wecomparetosomeotherrecent tswhichhaveuseddi erentformalisms,moreselectivedatasets,andtruncatedmultipoleexpansions.WepresentresultsfortheE2/M1andS2/M1ratios,asafunctionofQ2.

1.FitProcedure

In ttingthepionelectroproductiondatabase1,wehave xedtheQ2=0pointbasedonour tstopionphotoproduction2.Thephotoproductionmultipoleshavebeenparametrizedusingtheform

M=(Born+αB)(1+iTπN)+αRTπN+(ImTπN TπN2

)(αHr+iαHi),(1)

containingtheBornterms,withphenomenologicalpieces(α)maintainingthecorrectthresholdbehaviorandWatson’stheorem.TheπNT-matrix(TπN)connectseachmultipoletostructurefoundintheelasticπNscat-teringanalysis.AdditionalstructureisparametrizedthroughtheBornterms(whichcontainvector-mesoncontributions),andthephenomenolog-icalstructurefunctions(αB,αR,αHr,andαH

i).

Atnon-zeroQ2,theBorntermshavebuilt-inQ2dependence,othertermshavebeenmodi edbyafactor

f(Q2)=

k ΛQ

2(1+Q2/0.71)2

e 1+αQ2+β W

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