We report on the final electroweak measurements performed with data taken at the Z resonance by the experiments operating at the electron-positron colliders SLC and LEP. The data consist of 17 million Z decays accumulated by the ALEPH, DELPHI, L3 and OPAL experiments at LEP, and 600 thousand Z decays by the SLID experiment using a polarised beam at SLC. The measurements include cross-sections, forward-backward asymmetries and polarised asymmetries. The mass and width of the Z boson, m(Z) and Gamma(Z), and its couplings to fermions, for example the p parameter and the effective electroweak mixing angle for leptons, are precisely measured: m(Z) = 91.1875 +/- 0.0021 GeV, Gamma(Z) = 2.4952 +/- 0.0023 GeV, rho(l) = 1.0050 +/- 0.0010, sin(2)theta(eff)(lept) = 0.23153 +/- 0.00016. The number of light neutrino species is determined to be 2.9840 +/- 0.0082, in agreement with the three observed generations of fundamental fermions. The results are compared to the predictions of the Standard Model (SM). At the Z-pole, electroweak radiative corrections beyond the running of the QED and QCD coupling constants are observed with a significance of five standard deviations, and in agreement with the Standard Model. Of the many Z-pole measurements, the forward-backward asymmetry in b-quark production shows the largest difference with respect to its SM expectation, at the level of 2.8 standard deviations. Through radiative corrections evaluated in the framework of the Standard Model, the Z-pole data are also used to predict the mass of the top quark, m(t) = 173(+10)(+13) GeV, and the mass of the W boson, m(W) = 80.363 +/- 0.032 GeV. These indirect constraints are compared to the direct measurements, providing a stringent test of the SM. Using in addition the direct measurements of m(t) and m(W), the mass of the as yet unobserved SM Higgs boson is predicted with a relative uncertainty of about 50% and found to be less than 285 GeV at 95% confidence level. (c) 2006 Elsevier B.V. All rights reserved.
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[10.1016/j.physrep.2005.12.006]
Precision electroweak measurements on the Z resonance
SCHAEL S; BARATE R; BRUNELIERE R; BUSKULIC D; DE BONIS I; DECAMP D; GHEZ P; GOY C; JEZEQUEL S; LEES JP; LUCOTTE A; MARTIN F; MERLE E; MINARD MN; NIEF JY; ODIER P; PIETRZYK B; TROCME B; BRAVO S; CASADO MP; CHMEISSANI M; COMAS P; CRESPO JM; FERNANDEZ E; FERNANDEZ BOSMAN M; GARRIDO L; GRAUGES E; JUSTE A; MARTINEZ M; MERINO G; MIQUEL R; MIR LM; ORTEU S; PACHECO A; PARK IC; PERLAS J; RIU I; RUIZ H; SANCHEZ F; COLALEO A; CREANZA D; DE FILIPPIS N; DE PALMA M; IASELLI G; MAGGI G; MAGGI M; NUZZO S; RANIERI A; RASO G; RUGGIERI F; SELVAGGI G; SILVESTRIS L; TEMPESTA P; TRICOMI A; ZITO G; HUANG X; LIN J; OUYANG Q; WANG T; XIE Y; XU R; XUE S; ZHANG J; ZHANG L; ZHAO W; ABBANEO D; BAZARKO A; BECKER U; BOIX G; BIRD F; BLUCHER E; BONVICINI B; BRIGHT THOMAS P; BARKLOW T; BUCHMULLER O; CATTANEO M; CERUTTI F; CIULLI V; CLERBAUX B; DREVERMANN H; FORTY RW; FRANK M; GREENING TC; HAGELBERG R; HALLEY AW; GIANOTTI F; GIRONE M; HANSEN JB; HARVEY J; JACOBSEN R; HUTCHCROFT DE; JANOT R; JOST B; KNOBLOCH J; KADO, MARUMI ;LEHRAUS I; LAZEYRAS P; MALEY R; MATO P; MAY J; MOUTUSSI A; PEPE ALTARELLI M; RANJARD F; ROLANDI L; SCHLATTER D; SCHMITT B; SCHNEIDER O; TEJESSY W; TEUBERT F; TOMALIN IR; TOURNEFIER E; VEENHOF R; VALASSI A; WIEDENMANN W; WRIGHT AE; AJALTOUNI Z; BADAUD F; CHAZELLE G; DESCHAMPS O; DESSAGNE S; FALVARD A; FERDI C; FAYOLLE D; GAY P; GUICHENEY C; HENRARD P; JOUSSET J; MICHEL B; MONTEIL S; MONTRET JC; PALLIN D; PASCOLO JM; PERRET P; PODLYSKI F; BERTELSEN H; FERNLEY T; HANSEN JD; HANSEN JR; HANSEN PH; KRAAN AC; LINDAHL A; MOLLERUD R; NILSSON BS; RENSCH B; WAANANEN A; DASKALAKIS G; KYRIAKIS A; MARKOU C; SIMOPOULOU E; SIOTIS I; VAYAKI A; ZACHARIADOU K; BLONDEL A; BONNEAUD G; BRIENT JC; MACHEFERT E; ROUGE A; RUMPF M; SWYNGHEDAUW M; TANAKA R; VERDERI M; VIDEAU H; CIULLI V; FOCARDI E; PARRINI G; ZACHARIADOU K; CORDEN M; GEORGIOPOULOS C; ANTONELLI A; ANTONELLI M; BENCIVENNI G; BOLOGNA G; BOSSI F; CAMPANA P; CAPON G; CERUTTI F; CHIARELLA V; FELICI G; LAURELLI P; MANNOCCHI G; MURTAS GP; PASSALACQUA L; PICCHI P; COLRAIN P; TEN HAVE I; HUGHES IS; KENNEDY J; KNOWLES IG; LYNCH JG; MORTON WT; NEGUS P; O'SHEA V; RAINE C; REEVES P; SCARR JM; SMITH K; THOMPSON AS; TURNBULL RM; WASSERBAECH S; BUCHMULLER O; CAVANAUGH R; DHAMOTHARAN S; GEWENIGER C; HANKE P; HANSPER G; HEPP V; KLUGE EE; PUTZER A; SOMMER J; STENZEL H; TITTEL K; WERNER W; WUNSCH M; BEUSELINCK R; BINNIE DM; CAMERON W; DAVIES G; DORNAN PJ; GOODSIR S; MARINELLI N; MARTIN EB; NASH J; NOWELL J; RUTHERFORD SA; SEDGBEER JK; THOMPSON JC; WHITE R; WILLIAMS MD; GHETE VM; GIRTLER P; KNERINGER E; KUHN D; RUDOLPH G; BOUHOVA THACKER E; BOWDERY CK; BUCK PG; CLARKE DP; ELLIS G; FINCH AJ; FOSTER F; HUGHES G; JONES RWL; KEEMER NR; PEARSON MR; ROBERTSON NA; SLOAN T; SMIZANSKA M; SNOW SW; WILLIAMS MI; VAN DER AA O; DELAERE C; LEIBENGUTH G; LEMAITRE V; BAUERDICK LAT; BLUMENSCHEIN U; VAN GEMMEREN P; GIEHL I; HOLLDORFER F; JAKOBS K; KASEMANN M; KAYSER F; KLEINKNECHT K; MULLER AS; QUAST G; RENK B; ROHNE E; SANDER HG; SCHMELING S; WACHSMUTH H; WANKE R; ZEITNITZ C; ZIEGLER T; AUBERT JJ; BENCHOUK C; BONISSENT A; CARR J; COYLE P; CURTIL C; EALET A; ETIENNE F; FOUCHEZ D; MOTSCH F; PAYRE P; ROUSSEAU D; TILQUIN A; TALBY M; THULASIDES M; ALEPPO M; ANTONELLI M; RAGUSA F; BUSCHER V; DAVID A; DIETL H; GANIS G; HUTTMANN K; LUTJENS G; MANNERT C; MANNER W; MOSER HG; SETTLES R; SEYWERD H; STENZEL H; VILLEGAS M; WIEDENMANN W; WOLF G; AZZURRI P; BOUCROT J; CALLOT O; CHEN S; CORDIER A; DAVIER M; DUFLOT L; GRIVAZ JF; HEUSSE P; JACHOLKOWSKA A; LE DIBERDER F; LEFRANCOIS J; MUTZ AM; SCHUNE MH; SERIN L; VEILLET JJ; VIDEAU I; ZERWAS D; AZZURRI P; BAGLIESI G; BETTARINI S; BOCCALI T; BOZZI C; CALDERINI G; DELL'ORSO R; FANTECHI R; FERRANTE I; FIDECARO F; FOA L; GIAMMANCO A; GIASSI A; GREGORIO A; LIGABUE F; LUSIANI A; MARROCCHESI PS; MESSINEO A; PALLA F; RIZZO G; SANGUINETTI G; SCIABA A; SGUAZZONI G; SPAGNOLO P; STEINBERGER J; TENCHINI R; VENTURI A; VANNINI C; VENTURI A; VERDINI PG; AWUNOR O; BLAIR GA; COWAN G; GARCIA BELLIDO A; GREEN MG; MEDCALF T; MISIEJUK A; STRONG JA; TEIXEIRA DIAS P; BOTTERILL DR; CLIFFT RW; EDGECOCK TR; EDWARDS M; HAYWOOD SJ; NORTON PR; TOMALIN IR; WARD JJ; BLOCH DEVAUX B; BOUMEDIENE D; COLAS P; EMERY S; FABBRO B; KOZANECKI W; LANCON E; LEMAIRE MC; LOCCI E; PEREZ P; RANDER J; RENARDY JF; ROUSSARIE A; SCHULLER JP; SCHWINDLING J; TUCHMING B; VALLAGE B; BLACK SN; DANN JH; KIM HY; KONSTANTINIDIS N; LITKE AM; MCNEIL MA; TAYLOR G; BOOTH CN; CARTWRIGHT S; COMBLEY F; HODGSON PN; LEHTO M; THOMPSON LF; AFFHOLDERBACH K; BARBERIO E; BOHRER A; BRANDT S; BURKHARDT H; FEIGL E; GRUPEN C; HESS J; LUTTERS G; MEINHARD H; MINGUET RODRIGUEZ J; MIRABITO L; MISIEJUK A; NEUGEBAUER E; NGAC A; PRANGE G; RIVERA F; SARAIVA P; SCHAFER U; SIELER U; SMOLIK L; STEPHAN F; TRIER H; APOLLONIO M; BOREAN C; BOSISIO L; DELLA MARINA R; GIANNINI G; GOBBO B; MUSOLINO G; PITIS L; HE H; KIM H; PUTZ J; ROTHBERG J; ARMSTRONG SR; BELLANTONI L; BERKELMAN K; CINABRO D; CONWAY JS; CRANMER K; ELMER P; FENG Z; FERGUSON DPS; GAO Y; GONZALEZ S; GRAHL J; HARTON JL; HAYES OJ; HU H; JIN S; JOHNSON RP; KILE J; MCNAMARA PA; NIELSEN J; OREJUDOS W; PAN Y; SAADI Y; SCOTT IJ; SHARMA V; WALSH AM; WALSH J; WEAR J; VON WIMMERSPERG TOELLER JH; WIEDENMANN W; WU J; WU SL; WU X; YAMARTINO JM; ZOBERNIG G; DISSERTORI G; ABDALLAH J; ABREU P; ADAM W; ADYE T; ADZIC P; AJINENKO I; ALBRECHT T; ALDERWEIRELD T; ALEKSEEV GD; ALEMANY FERNANDEZ R; ALLMENDINGER T; ALLPORT PP; ALMEHED S; AMALDI U; AMAPANE N; AMATO S; ANASHKIN E; ANASSONTZIS EG; ANDERSSON P; ANDREAZZA A; ANDRINGA S; ANJOS N; ANTILOUS P; APEL WD; ARNOUD Y; ASK S; ASMAN B; AUGUSTIN JE; AUGUSTINUS A; BAILLON P; BALLESTRERO A; BAMBADE P; BARAO F; BARBIELLINI G; BARBIER R; BARDIN D; BARKER G; BARONCELLI A; BATTAGLIA M; BAUBILLIER M; BECKS KH; BEGALLI M; BEHRMANN A; BEILLIERE P; BELOKOPYTOV Y; BELOUS K; BEN HAIM E; BENEKOS N; BENVENUTI A; BERAT C; BERGGREN M; BERNTZON L; BERTINI D; BERTRAND D; BESANCON M; BESSON N; BIANCHI F; BIGI M; BILENKY MS; BIZOUARD MA; BLOCH D; BLOM M; BLUJ M; BONESINI M; BONIVENTO W; BOONEKAMP M; BOOTH PSL; BORGLAND AW; BORISOV G; BOSIO C; BOTNER O; BOUDINOV E; BOUQUET B; BOURDARIOS C; BOWCOCK TJV; BOYKO I; BOZOVIC I; BOZZO M; BRACKO M; BRANCHINI P; BRENKE T; BRENNER R; BRODET E; BRUCKMAN P; BRUNET JM; BUGGE L; BURAN T; BURGSMUELLER T; BUSCHBECK B; BUSCHMANN P; CABRERA S; CACCIA M; CALVI M; ROZAS AJC; CAMPORESI T; CANALE V; CANEPA M; CARENA F; CARROLL L; CASO C; GIMENEZ MVC; CASTRO N; CATTAI A; CAVALLO F; CERRUTI C; CHABAUD V; CHAPKIN M; CHARPENTIER P; CHAUSSARD L; CHECCHIA P; CHELKOV GA; CHEN M; CHIERICI R; CHLIAPNIKOV R; CHOCHULA P; CHOROWICZ V; CHUDOBA J; CHUNG SU; CIESLIK K; COLLINS P; COLOMER M; CONTRI R; CORTINA E; COSME G; COSSUTI F; COSTA MJ; COWELL JH; CRAWLEY HB; CRENNELL D; CREPE S; CROSETTI G; CUEVAS J; CZELLAR S; D'HONDT J; DALMAGNE B; DALMAU J; DAMGAARD G; DAVENPORT M; DA SILVA T; DA SILVA W; DEGHORAIN A; DELLA RICCA G; DELPIERRE P; DEMARIA N; DE ANGELIS A; DE BOER W; DE BRABANDERE S; DE CLERCQ C; DE LOTTO B; DE MARIA N; DE MIN A; DE PAULA L; DIJKSTRA H; DI CIACCIO L; DI DIODATO A; DI SIMONE A; DJANNATI A; DOLBEAU J; DOROBA K; DRACOS M; DREES J; DREES KA; DRIS M; DUPERRIN A; DURAND JD; EHRET R; EIGEN G; EKELOF T; EKSPONG G; ELLERT M; ELSING M; ENGEL JP; ERZEN B; SANTO MCE; FALK E; FANOURAKIS G; FASSOULIOTIS D; FAYOT J; FEINDT M; FENYUK A; FERNANDEZ J; FERRARI P; FERRER A; FERRER RIBAS E; FERRO F; FICHET S; FIRESTONE A; FISCHER PA; FLAGMEYER U; FOETH H; FOKITIS E; FONTANELLI F; FRANEK B; FRODESEN AG; FRUHWIRTH R; FULDA QUENZER F; FUSTER J; GALLONI A; GAMBA D; GAMBLIN S; GANDELMAN M; GARCIA C; GARCIA J; GASPAR C; GASPAR M; GASPARINI U; GAVILLET P; GAZIS E; GELE D; GERBER JP; GERDYUKOV L; GHODBANE N; GIL I; GLEGE F; GOKIELI R; GOLOB B; GOMEZ CEBALLOS G; GONCALVES P; CABALLERO IG; GOPAL G; GORN L; GORSKI M; GOUZ Y; GRACCO V; GRAHL J; GRAZIANI E; GREEN C; GREFRATH A; GRIMM HJ; GRIS P; GROSDIDIER G; GRZELAK K; GUNTHER M; GUY J; HAAG C; HAHN F; HAHN S; HALLGREN A; HAMACHER K; HAMILTON K; HANSEN J; HARRIS FJ; HAUG S; HAULER F; HEDBERG V; HEISING S; HENNECKE M; HENRIQUES R; HERNANDEZ JJ; HERQUET P; HERR H; HESSING TL; HEUSER JM; HIGON E; HOFFMAN J; HOLMGREN SO; HOLT PJ; HOLTHUIZEN D; HOORELBEKE S; HOULDEN MA; HRUBEC J; HUBER M; HUET K; HUGHES GJ; HULTQVIST K; JACKSON JN; JACOBSSON R; JALOCHA P; JANIK R; JARLSKOG C; JARLSKOG G; JARRY P; JEAN MARIE B; JEANS D; JOHANSSON EK; JOHANSSON PD; JONSSON P; JORAM C; JUILLOT P; JUNGERMANN L; KAPUSTA F; KARAFASOULIS K; KATSANEVAS S; KATSOUFIS E; KERANEN R; KERNEL G; KERSEVAN BP; KERZEL U; KHOMENKO BA; KHOVANSKI NN; KIISKINEN A; KING BT; KINVIG A; KJAER NJ; KLAPP O; KLEIN H; KLUIT P; KNOBLAUCH D; KOKKINIAS P; KONOPLIANNIKOV A; KORATZINOS M; KOSTIOUKHINE V; KOURKOUMELIS C; KOUZNETSOV O; KRAMMER M; KREUTER C; KRIZNIC E; KRSTIC J; KRUMSTEIN Z; KUBINEC P; KUCEWICZ W; KUCHARCZYK M; KUROWSKA J; KURVINEN K; LAMSA J; LANCERI L; LANE DW; LANGEFELD P; LAPIN V; LAUGIER JP; LAUHAKANGAS R; LEDER G; LEDROIT F; LEFEBURE V; LEINONEN L; LEISOS A; LEITNER R; LEMONNE J; LENZEN G; LEPELTIER V; LESIAK T; LETHUILLIER M; LIBBY J; LIEBIG W; LIKO D; LIPNIACKA A; LIPPI I; LOERSTAD B; LOKAJICEK M; LOKEN JG; LOPES JH; LOPEZ JM; LOPEZ FEMANDEZ R; LOUKAS D; LUTZ P; LYONS L; MACNAUGHTON J; MAHON JR; MAIO A; MALEK A; MALMGREN TGM; MALTEZOS S; MALYCHEV V; MANDL F; MARCO J; MARCO R; MARECHAL B; MARGONI M; MARIN JC; MARIOTTI C; MARKOU A; MARTINEZ RIVERO C; MARTINEZ VIDAL F; GARCIA SMI; MASIK J; MASTROYIANNOPOULOS N; MATORRAS F; MATTEUZZI C; MATTHIAE G; MAZIK J; MAZZUCATO F; MAZZUCATO M; MCCUBBIN M; MCKAY R; MCNULTY R; MERONI C; MEYER WT; MIAGKOV A; MIGLIORE E; MIRABITO L; MITAROFF W; MJOERNMARK U; MOA T; MOCH M; MOELLER R; MOENIG K; MONGE R; MONTENEGRO J; MORAES D; MOREAU X; MORENO S; MORETTINI P; MORTON G; MUELLER U; MUENICH K; MULDERS M; MULET MARQUIS C; MUNDIM L; MURESAN R; MURRAY W; MURYN B; MYATT G; MYKLEBUST T; NARAGHI F; NASSIAKOU M; NAVARRIA F; NAVAS S; NAWROCKI K; NEGRI P; NEUFELD N; NEUMANN W; NEUMEISTER N; NICOLAIDOU R; NIELSEN BS; NIEUWENHUIZEN M; NIEZURAWSKI P; NIKOLAENKO V; NIKOLENKO M; NOMOKONOV V; NORMAND A; NYGREN A; OBLAKOWSKA MUCHA A; OBRAZTSOV V; OLSHEVSKI A; ONOFRE A; ORAVA R; ORAZI G; OSTERBERG K; OURAOU A; OYANGUREN A; PAGANINI P; PAGANONI M; PAIANO S; PAIN R; PAIVA R; PALACIOS JP; PALKA H; PAPADOPOULOU TD; PAPAGEORGIOU K; PAPE L; PARKES C; PARODI F; PARZEFALL U; PASSERI A; PASSON O; PAVEL T; PEGORARO M; PERALTA L; PEREPELITSA V; PERNICKA M; PERROTTA A; PETRIDOU C; PETROLINI A; PHILIPS HT; PIANA G; PIEDRA J; PIERI L; PIERRE F; PIMENTA M; PIOTTO E; PODOBNIK T; POIREAU V; POL ME; POLOK G; POLYCARPO E; POROPAT P; POZDNIAKOV V; PRIVITERA R; PUKHAEVA N; PULLIA A; RADOJICIC D; RAGAZZI S; RAHMANI H; RAKOCZY D; RAMES J; RAMLER L; RATOFF PN; READ A; REBECCHI P; REDAELLI NG; REGLER M; REHN J; REID D; REINHARDT R; RENTON P; RESVANIS LK; RICHARD F; RIDKY J; RINAUDO G; RIPP BAUDOT I; RIVERO M; RODRIGUEZ D; ROHNE O; ROMERO A; RONCHESE P; ROSENBERG EI; ROSINSKY P; ROUDEAU R; ROVELLI T; ROYON C; RUHLMANN KLEIDER V; RUIZ A; RYABTCHIKOV D; SAARIKKO H; SACQUIN Y; SADOVSKY A; SAJOT G; SALMI L; SALT J; SAMPSONIDIS D; SANNINO M; SAVOY NAVARRO A; SCHEIDLE T; SCHNEIDER H; SCHWEMLING P; SCHWERING B; SCHWICKERATH U; SCHYNS MAE; SCURI F; SEAGER P; SEDYKH Y; SEGAR A; SEIBERT N; SEKULIN R; SHELLARD RC; SHERIDAN A; SIEBEL M; SILVESTRE R; SIMARD L; SIMONETTO F; SISAKIAN A; SKAALI TB; SMADJA G; SMIRNOV N; SMIRNOVA O; SMITH GR; SOKOLOV A; SOPCZAK A; SOSNOWSKI R; SPASSOV T; SPIRITI E; SPONHOLZ P; SQUARCIA S; STAMPFER D; STANESCU C; STANIC S; STANITZKI M; STAPNES S; STEVENSON K; STOCCHI A; STRAUSS J; STRUB R; STUGU B; SZCZEKOWSKI M; SZEPTYCKA M; SZUMLAK T; TABARELLI T; TAFFARD AC; TEGENFELDT F; TERRANOVA F; THOMAS J; TILQUIN A; TIMMERMANS J; TINTI N; TKATCHEV L; TOBIN M; TODOROV T; TODOROVOVA S; TOET DZ; TOMARADZE A; TOME B; TONAZZO A; TORTORA L; TORTOSA P; TRANSTROMER G; TRAVNICEK P; TREILLE D; TRISTRAM G; TROCHIMCZUK M; TROMBINI A; TRONCON C; TSIROU A; TURLUER ML; TYAPKIN IA; TYAPKIN P; TZAMARIAS S; ULLALAND O; UVAROV V; VALENTI G; VALLAZZA E; VANDER VELDE C; VAN APELDOORN GW; VAN DAM P; VAN DEN BOECK W; VAN DONINCK WK; VAN ELDIK J; VAN LYSEBETTEN A; VAN REMORTEL N; VAN VULPEN I; VASSILOPOULOS N; VEGNI G; VELOS F; VENTURA L; VENUS W; VERBEURE F; VERDIER P; VERLATO M; VERTOGRADOV LS; VERZI V; VILANOVA D; VITALE L; VLASOV E; VODOPYANOV AS; VOLLMER C; VOULGARIS G; VRBA V; WAHLEN H; WALCK C; WASHBROOK AJ; WEISER C; WETHERELL AM; WICKE D; WICKENS J; WILKINSON G; WINTER M; WITEK M; WLODEK T; WOLF G; YI J; YUSHCHENKO O; ZAITSEV A; ZALEWSKA A; ZALEWSKI P; ZAVRTANIK D; ZEVGOLATAKOS E; ZHURAVLOV V; ZIMIN NI; ZINTCHENKO A; ZOLLER P; ZUCCHELLI GC; ZUMERLE G; ZUPAN M; ACCIARRI M; ACHARD P; ADRIANI O; AGUILAR BENITEZ M; ALCARAZ J; ALEMANNI G; ALLABY J; ALOISIO A; ALVIGGI MG; AMBROSI G; ANDERHUB H; ANDREEV VP; ANGELESCU T; ANSELMO F; AREFIEV A; AZEMOON T; AZIZ T; BAGNAIA, Paolo ;BAJO A; BAKSAY G; BAKSAY L; BALANDRAS A; BALDEW SV; BALL RC; BANERJEE S; BANERJEE S; BARCZYK A; BARILLERE R; BARONE, Luciano Maria ;BARTALINI P; BASILE M; BATALOVA N; BATTISTON R; BAY A; BECATTINI F; BECKER U; BEHNER F; BELLUCCI L; BERBECO R; BERDUGO J; BERGES P; BERTUCCI B; BETEV BL; BHATTACHARYA S; BIASINI M; BIGLIETTI M; BILAND A; BLAISING JJ; BLYTH SC; BOBBINK BJ; BOHM A; BOLDIZSAR L; BORGIA, BRUNO ;BOTTAI S; BOURILKOV D; BOURQUIN M; BRACCINI S; BRANSON JG; BRIGLJEVIC V; BROCHU F; BROCK IC; BUFFINI A; BUIJS A; BURGER JD; BURGER WJ; BUTTON A; CAI XD; CAMPANELLI M; CAPELL M; ROMEO GC; CARLINO G; CARTACCI A; CASAUS J; CASTELLINI G; CAVALLARI E; CAVALLO N; CECCHI C; CERRADA M; CESARONI F; CHAMIZO M; CHANG YH; CHATURVEDI UK; CHEMARIN M; CHEN A; CHEN G; CHEN GM; CHEN HF; CHEN HS; CHIEFARI G; CIFARELLI L; CINDOLO F; CIVININI C; CLARE I; CLARE R; COIGNET G; COLIJN AP; COLINO N; COSTANTINI S; COTOROBAI F; COZZONI B; DE LA CRUZ B; CSILLING A; CUCCIARELLI S; DAI TS; VAN DALEN JA; D'ALESSANDRO R; DE ASMUNDIS R; DEBRECZENI J; DEGLON P; DEGRE P; DEHMELT K; DEITERS K; DELLA VOLPE D; DELMEIRE E; DENES P; DENOTARISTEFANI F; DE SALVO A; DIEMOZ M; DIERCKXSENS M; VAN DIERENDONCK D; DI LODOVICO F; DIONISI, Carlo ;DITTMAR M; DOMINGUEZ A; DORIA A; DOVA MT; DUCHESNEAU D; DUFOURNAUD D; DUDA M; DUINKER P; DURAN I; DUTTA S; ECHENARD B; ELINE A; EL HAGE A; EL MAMOUNI H; ENGLER A; EPPLING FJ; ERNE FC; EXTERMANN P; FABRE M; FACCINI, Riccardo ;FALAGAN MA; FALCIANO S; FAVARA A; FAY J; FEDIN O; FELCINI M; FERGUSON T; FERRONI, Fernando ;FESEFELDT H; FIANDRINI E; FIELD JH; FILTHAUT F; FISHER PH; FISHER W; FISK I; FORCONI G; FREDJ L; FREUDENREICH K; FURETTA C; GALAKTIONOV Y; GANGULI SN; GARCIA ABIA P; GATAULLIN M; GAU SS; GENTILE, Simonetta ;GHEORDANESCU N; GIAGU, Stefano ;GONG ZF; GRENIER G; GRIMM O; GRUENEWALD MW; GUIDA M; VAN GULIK R; VAN GUPTA VK; GURTU A; GUTAY LJ; HAAS D; HASAN A; HATZIFOTIADOU D; HEBBEKER T; HERVE A; HIDAS P; HIRSCHFELDER J; HOFER H; HOHLMANN M; HOLZNER G; HOORANI H; HOU SR; LASHVILI I; INNOCENTE V; JIN BN; JINDAL P; JONES LW; DEJONG P; JOSA MUTUBERRIA I; KHAN RA; KAUR M; KIENZLE FOCACCI MN; KIM D; KIM JK; KIRKBY J; KISS D; KITTEL W; KLIMENTOV A; KONIG AC; KOFFEMAN E; KOPAL M; KOPP A; KOUTSENKO V; KRABER M; KRAEMER RW; KRENZ W; KRUGER A; KUIJTEN H; KUNIN A; 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2006
Abstract
We report on the final electroweak measurements performed with data taken at the Z resonance by the experiments operating at the electron-positron colliders SLC and LEP. The data consist of 17 million Z decays accumulated by the ALEPH, DELPHI, L3 and OPAL experiments at LEP, and 600 thousand Z decays by the SLID experiment using a polarised beam at SLC. The measurements include cross-sections, forward-backward asymmetries and polarised asymmetries. The mass and width of the Z boson, m(Z) and Gamma(Z), and its couplings to fermions, for example the p parameter and the effective electroweak mixing angle for leptons, are precisely measured: m(Z) = 91.1875 +/- 0.0021 GeV, Gamma(Z) = 2.4952 +/- 0.0023 GeV, rho(l) = 1.0050 +/- 0.0010, sin(2)theta(eff)(lept) = 0.23153 +/- 0.00016. The number of light neutrino species is determined to be 2.9840 +/- 0.0082, in agreement with the three observed generations of fundamental fermions. The results are compared to the predictions of the Standard Model (SM). At the Z-pole, electroweak radiative corrections beyond the running of the QED and QCD coupling constants are observed with a significance of five standard deviations, and in agreement with the Standard Model. Of the many Z-pole measurements, the forward-backward asymmetry in b-quark production shows the largest difference with respect to its SM expectation, at the level of 2.8 standard deviations. Through radiative corrections evaluated in the framework of the Standard Model, the Z-pole data are also used to predict the mass of the top quark, m(t) = 173(+10)(+13) GeV, and the mass of the W boson, m(W) = 80.363 +/- 0.032 GeV. These indirect constraints are compared to the direct measurements, providing a stringent test of the SM. Using in addition the direct measurements of m(t) and m(W), the mass of the as yet unobserved SM Higgs boson is predicted with a relative uncertainty of about 50% and found to be less than 285 GeV at 95% confidence level. (c) 2006 Elsevier B.V. All rights reserved.
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[10.1016/j.physrep.2005.12.006]
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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione.
