Test of QCD analytic predictions for the multiplicity ratio between gluon and quark jets

G Alexander ,S Anderson ,H M Bosch ,P Poffenberger ,D Chrisman ,C K Hargrove ,M Sasaki ,J Von Krogh ,T Tsukamoto ,P Vikas ,M J Oreglia ,T Shears ,M J Goodrick ,Antônio Rossi ,F Wäckerle ,M Kolrep ,H Jérémie ,T Kress ,S Schmitt ,R M Brown ,W P Lai ,R J Hawkings ,J Bechtluft ,M G Vincter ,C M Hawkes ,V Blobel ,G Azuelos ,David Charlton ,C Beeston ,K Stephens ,S A Wotton ,J S White ,G M Dallavalle ,J R Pater ,K J Anderson ,N K Watson ,K Sachs ,P Giacomelli ,A Stahl ,P Capiluppi ,G A Snow ,J J Ward ,M Morii ,C Hartmann ,P Bock ,E Tsur ,Robert Howard ,E A Mckigney ,H Mes ,S Komamiya ,P E.l Clarke ,A N Bell ,D Karlen ,P G Estabrooks ,L A Del Pozo ,R W Springer ,T Mäshimo ,F G Oakham ,S Kluth ,H Evans ,M Bobinski ,T Kawamoto ,R J Barlow ,D Lellouch ,T J Smith ,P Szymański ,F Odorici ,W Matthews ,R Keeler ,J E.g Edwards ,D G Fong ,A Posthaus ,O Schaile ,T P Kokott ,M Boutemeur ,R Tafirout ,P W Jeffreys ,Eckhard Von Torne ,P Sherwood ,E Ros ,A M Lee ,F K Loebinger ,D S Koetke ,S R Lautenschlager ,A J Martin ,Shun‐Ichi Tanaka ,C H Shepherd-Themistocleous ,N I Geddes ,J G Layter ,D E Plane ,B Stockhausen ,D J Miller ,M Hansroul ,I Cohen ,T Geralis ,S Bentvelsen ,G Vasseur ,M Doucet ,A K Honma ,P Igo‐Kemenes ,P Schütz ,T Mori ,S J De Jong ,R E Hughes-Jones ,Shinji Yamashita ,G Herten ,D Horváth ,H A Neal ,S L Lloyd ,T Behnke ,J Letts ,A Malik ,F Fiedler ,G N Patrick ,B Wilkens ,P Taras ,J Ludwig ,C Sbarra ,M J Losty ,R Nisius ,F Meijers ,K Nagai ,D L Rees ,M Gruwé ,A Wagner ,S M Gascon-Shotkin ,H Burckhart ,B Nellen ,W R Gibson ,P A Hart ,B W Kennedy ,B C Shen ,M Hapke ,E Barberio ,D R Rust ,M J Pearce ,R Bürgin ,Roger Jones ,J Meyer ,J M Roney ,F Strumia ,S D Talbot ,G D Lafferty ,J Allison ,Y Rozen ,M Schumacher ,R Folman ,A Sittler ,M Cuffiani ,H Lafoux ,M Sproston ,P Pfeifenschneider ,E H Vokurka ,P Routenburg ,J Goldberg ,M F Turner-Watson ,Ch Geich-Gimbel ,J E Conboy ,C R Jones ,R Ryłko ,M Verzocchi ,K Ametewee ,H.‐C Schultz‐Coulon ,B J King ,G Yekutieli ,M Hauschild ,S Marcellini ,G Mikenberg ,C Grandi ,K Ishii ,E Lefebvre ,E Do Couto E Silva ,C Lewis ,W Mohr ,A Skuja ,A Gaidot ,E Duchovni ,C Y Chang ,P Krieger ,I J Bloodworth ,P Mättig ,Ö Runólfsson ,T R Junk ,P Jovanović ,S Asai ,C Dallapiccola ,T R Wyatt ,D E Hutchcroft ,D Glenzinskí ,O C Cooke ,R G Kellogg ,E K.g Sarkisyan ,T Hilse ,C D Burgard ,G Bella ,J R Carter ,H Przysiezniak ,M Schröder ,D R Ward ,A D Schaile ,B Schmitt ,R Lahmann ,P S Wells ,S Orito ,M Kobel ,M Jimack ,J P Martín ,S J Hillier ,A M Smith ,J E Bloomer ,B Nijjhar ,S Söldner-Rembold ,S Braibant ,F S Merritt ,R Bartoldus ,F X Gentit ,M Foucher ,Meirin Oan Evans ,J Lauber ,S Arcelli ,K Desch ,P Gagnon ,U Müller ,A T Watson ,A Jawahery ,V Gibson ,G D Long ,G Martı́nez ,M Mannelli ,R J Homer ,I P Duerdoth ,S A Robins ,K W Bell ,M Thiergen ,A Mcnab ,K Runge ,Roberto Giacomelli ,T Omori ,R K Carnegie ,C Markus ,A Michelini ,M S Dixit ,E Gross ,D M Gingrich ,J Pálinkás ,Uwe Rüppel ,A S Turcot ,G W Wilson ,J L Pinfold ,M Starks ,P Schenk ,G Giacomelli ,H M Fischer ,R Van Kooten ,A Rooke ,N Wermes ,F Fabbri ,M Schulz ,J Kirk ,M A Thomson ,N Altekamp ,M Steiert ,M Rosvick ,A H Ball ,D Lanske ,A Fürtjes ,D Strom ,S Bethke ,J R Batley ,C P Ward ,M Jones ,G Wolf ,M Tecchio ,G P Siroli ,R J Hemingway ,S Tarem ,A Montanari ,C Charlesworth ,S Menke ,H O Ogren ,R Mir ,S Dado ,A A Carter ,K Kawagoe ,W G Scott ,G Pásżtor ,J A Mckenna ,S Petzold ,D C Imrie ,Martin Ingram ,J W Gary ,Thomas J Mcmahon ,R Sobie ,J Patt ,D Axen ,F Scharf ,P Fath ,J C Hill ,W J Mcdonald ,R D Heuer ,J A Wilson ,P M Watkins ,A Joly ,N Rodning ,B Poli ,O Biebel ,I Nakamura ,U Jost ,S L Chu ,J Steuerer ,J Gascon ,S Towers ,P Berlich ,D Lazic ,C Hajdú ,J E Pilcher ,R A Mcpherson ,L J Levinson ,G Jones ,S W O’neale ,Tatsuo Kobayashi ,M Hildreth ,G Hanson ,A Skillman ,P Scharff-Hansen ,G Duckeck ,M Fierro ,P Weber ,W Gorn ,D Rigby ,B Bouwens ,P Kyberd ,P R Hobson ,R Kowalewski ,P Utzat ,V Zacek

doi:10.1016/s0370-2693(96)01319-6

Abstract

Gluon jets with about 39 GeV energy are identified in hadronic Z 0 decays by tagging two jets in the same hemisphere of an event as quark jets. Identifying the gluon jet to be all the particles observed in the hemisphere opposite to that containing the two tagged jets yields an inclusive gluon jet definition corresponding to that used in analytic calculations, allowing the first direct test of those calculations. In particular, this jet definition yields results which are only weakly dependent on a jet finding algorithm. We find r ch. =1.552±0.0041 ( stat) ±0.061 ( syst.) for the ratio of the mean charged particle multiplicity in gluon jets to that in light quark uds jets, where the uds jets are identified using an inclusive jet definition similar to that used for the gluon jets. Our result is in general agreement with the prediction of a recent analytic calculation which incorporates energy conservation into the parton shower branching processes, but is considerably smaller than analytic predictions which do not incorporate energy conservation.

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