Measurement of the longitudinal, transverse and asymmetry fragmentation functions at LEP

D J Miller,A T Watson,P Schenk,F X Gentit,C H Shepherd-Themistocleous,S Asai,G A Snow,H M Fischer,V Gibson,G Yekutieli,R K Carnegie,N I Geddes,P Krieger,P G Estabrooks,G P Siroli,P S Wells,J Kanzaki,Y Rozen,P Utzat,J J Ward,E Barberio,G M Dallavalle,R D Heuer,P Teixeira-Dias,K W Bell,M Sasaki,J Letts,M J Goodrick,I J Bloodworth,O Schaile,S Dado,M Jimack,D E Hutchcroft,M Fanti,F S Merritt,S Braibant,C P Ward,P Gagnon,J Gascon,S Söldner-Rembold,B W Kennedy,E Lefebvre,A K Honma,D E Plane,M Settles,M Morii,G Azuelos,M Kobel,A Beck,K Stephens,R Mir,H Mes,P Capiluppi,K Kawagoe,M W Redmond,J E Pilcher,H Przysiezniak,J G Layter,B Fabbro,C Dallapiccola,M Jones,R E Hughes-Jones,S L Chu,M Tecchio,W Matthews,D Axen,C K Hargrove,M Fierro,J Steuerer,C Beeston,R Akers,G Giacomelli,C Charlesworth,J A Wilson,A S Turcot,M S Dixit,D Hochman,I Cohen,K Runge,B Wilkens,M Hapke,J C Clayton,P Vikas,C Hartmann,P W Jeffreys,D R Rust,O C Cooke,H Lafoux,N K Watson,J C Hill,D S Koetke,J Allison,S Marcellini,P Bock,S Tarem,M Tscheulin,R Lahmann,S Bentvelsen,B Stockhausen,S W Gensler,H Fukui,O Biebel,E A Mckigney,C Markus,N Altekamp,A Montanari,M G Rison,M J Losty,P A Hart,S Anderson,J Bechtluft,T J Smith,J Lauber,R Sobie,M Cuffiani,C Y Chang,B Nellen,T R Wyatt,M Hansroul,G Vasseur,P Berlich,P Taras,D Karlen,T Tsukamoto,T Kawamoto,S Towers,G T Zorn,S Arcelli,M Foucher,A Skuja,K Ametewee,B Schmitt,M Starks,M A Thomson,N Wermes,S Bethke,D L Rees,E Ros,G Beaudoin,S Kluth,S A Robins,N Rodning,D L Wagner,P Poffenberger,T Geralis,D M Gingrich,F Odorici,W G Scott,V Zacek,J D Gillies,J Schwiening,R J Barlow,A Gaidot,R J Hemingway,F K Loebinger,T W Pritchard,F Fiedler,N J Oldershaw,F Fabbri,C Burgard,P Weber,W R Gibson,S Orito,J King,A Wagner,A Skillman,A Stahl,G A Beck,R Kowalewski,G D Long,F G Oakham,J P Pansart,D R Ward,G Duckeck,R W Springer,R M Brown,M Sproston,P Giacomelli,G D Lafferty,T P Kokott,A Posthaus,A A Carter,P M Watkins,D Strom,T Behnke,R Bürgin,S G Clowes,K J Anderson,J Goldberg,R Folman,D C Imrie,M J Pearce,J Ludwig,C Stegmann,P Mättig,F Scharf,F Meijers,B C Shen,R G Kellogg,M Rosvick,S L Lloyd,R J Homer,P Routenburg,A Fürtjes,M Mannelli,C Darling,A Luig,B Lorazo,J W Gary,U C Dunwoody,H M Bosch,J R Carter,W Mohr,W Gorn,D Lellouch,M F Turner-Watson,A H Ball,W P Lai,G Alexander,N Tesch,G Herten,B Nijjhar,A M Rossi,C M Hawkes,A Joly,J E Conboy,T Hilse,U Müller,C Grandi,A Buijs,J Kirk,A M Lee,F Wäckerle,M Boutemeur,J M Roney,C Sbarra,P Bright-Thomas,M Hauschild,T Kress,G W Wilson,A M Smith,A Michelini,S J Hillier,G N Patrick,P Scharff-Hansen,A J Martin,C J Oram,P D Phillips,E Gross,B Poli,B J King,M Schulz,A D Schaile,R Tafirout,D G Charlton,I P Ducrdoth,A Malik,R Bartoldus,T Mori,M Schröder,D Lanske,J E Duboscq,E Duchovni,G Wolf,P Schütz,P Kyberd,G Mikenberg,G Bella,A Jawahery,D G Fong,M Fincke-Keeler,S Komamiya,P Sherwood,J R Batley,P R Hobson,P Fath,S Menke,M J Oreglia,F Palmonari,D Rigby,P Jovanović ,S W O’neale ,P E.l Clarke ,T Shears ,Ö Runólfsson ,Tatsuo Kobayashi ,Roberto Giacomelli ,Ch Geich-Gimbel ,S J De Jong ,M G Vincter ,J Von Krogh ,E Do Couto E Silva ,Thomas J Mcmahon ,W D Zeuner ,J E.g Edwards ,G Hanson ,A Mcnab ,J P Martín ,S A Wotton ,R Keeler ,L J Levinson ,H.‐C Schultz‐Coulon ,Robert Howard ,J A Mckenna ,H Ogren ,T Włodek ,Eckhard Von Torne ,J L Pinfold ,P Szymański ,H Evans ,P Igo‐Kemenes ,R Van Kooten ,H Burckhart ,R J Hawkings ,H Jérémie ,T Mäshimo ,Roger Jones ,Hui Deng ,L A Del Pozo

doi:10.1007/bf01566668

Abstract

The fragmentation function for the process e+e−→h+X, whereh represents a hadron, may be decomposed into transverse, longitudinal and asymmetric contributions by analysis of the distribution of polar production angles. A number of new tests of QCD have been proposed using these fragmentation functions, but so far no data have been published on the separate components. We have performed such a separation using data on charged particles from hadronic Z0 decays atOpal, and have compared the results with the predictions of QCD. By integrating the fragmentation functions, we determine the average charged particle multiplicity to be\(\overline {n_{ch} } = 21.05 \pm 0.20\). The longitudinal to total cross-section ratio is determined to be σL/σtot=0.057±0.005. From the longitudinal fragmentation function we are able to extract the gluon fragmentation function. The connection between the asymmetry fragmentation function and electroweak asymmetrics is discussed.

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