11 research outputs found
Observation of a new Xi(b) baryon
The first observation of a new b baryon via its strong decay into Xi(b)^-
pi^+ (plus charge conjugates) is reported. The measurement uses a data sample
of pp collisions at sqrt(s) = 7 TeV collected by the CMS experiment at the LHC,
corresponding to an integrated luminosity of 5.3 inverse femtobarns. The known
Xi(b)^- baryon is reconstructed via the decay chain Xi(b)^- to J/psi Xi^- to
mu^+ mu^- Lambda^0 pi^-, with Lambda^0 to p pi^-. A peak is observed in the
distribution of the difference between the mass of the Xi(b)^- pi^+ system and
the sum of the masses of the Xi(b)^- and pi^+, with a significance exceeding
five standard deviations. The mass difference of the peak is 14.84 +/- 0.74
(stat.) +/- 0.28 (syst.) MeV. The new state most likely corresponds to the
J^P=3/2^+ companion of the Xi(b).Comment: Submitted to Physical Review Letter
Measurements of inclusive W and Z cross sections in pp collisions at root s=7 TeV
This is the pre-print version of the Published Article, which can be accessed from the link below - Copyright @ 2011 Springer VerlagMeasurements of inclusive W and Z boson production cross sections in pp collisions at sqrt(s)=7 TeV are presented, based on 2.9 inverse picobarns of data recorded by the CMS detector at the LHC. The measurements, performed in the electron and muon decay channels, are combined to give sigma(pp to WX) times B(W to muon or electron + neutrino) = 9.95 \pm 0.07(stat.) \pm 0.28(syst.) \pm 1.09(lumi.) nb and sigma(pp to ZX) times B(Z to oppositely charged muon or electron pairs) = 0.931 \pm 0.026(stat.) \pm 0.023(syst.) \pm 0.102(lumi.) nb. Theoretical predictions, calculated at the next-to-next-to-leading order in QCD using recent parton distribution functions, are in agreement with the measured cross sections. Ratios of cross sections, which incur an experimental systematic uncertainty of less than 4%, are also reported
Measurement of dijet angular distributions and search for quark compositeness in pp collisions at âs=7TeV
Dijet angular distributions are measured over a wide range of dijet invariant masses in pp collisions at root s = 7 TeV, at the CERN LHC. The event sample, recorded with the CMS detector, corresponds to an integrated luminosity of 36 pb(-1). The data are found to be in good agreement with the predictions of perturbative QCD, and yield no evidence of quark compositeness. With a modified frequentist approach, a lower limit on the contact interaction scale for left-handed quarks of Lambda(+) = 5.6 TeV (Lambda(-) = 6.7 TeV) for destructive (constructive) interference is obtained at the 95% confidence level
Realising Team-Working in the Field: An Agent-based Approach
Multi-agent systems technology is applied to enable co-operation between mobile workers in the field, minimising user intervention and increasing reachability. A component-based approach is taken to simplify the management of deployed co-operation services. A Personal Assistant running on a mobile device is introduced to show how an intelligent and autonomous agent can increase the utility of users during workforce co-operation processes. Finally, a real world trial of the technology by network installation and maintenance engineers in the UK is described. Some technical issues revealed during the trial are discussed, as is the impact of the technology on the business process
Dependence on pseudorapidity and on centrality of charged hadron production in PbPb collisions at sqrt(sNN)=2.76 TeV
none2175A measurement is presented of the charged hadron multiplicity in hadronic
PbPb collisions, as a function of pseudorapidity and centrality, at a collision energy of
2.76TeV per nucleon pair. The data sample is collected using the CMS detector and
a minimum-bias trigger, with the CMS solenoid o. The number of charged hadrons is
measured both by counting the number of reconstructed particle hits and by forming hit
doublets of pairs of layers in the pixel detector. The two methods give consistent results.
The charged hadron multiplicity density, dNch/deta|eta=0, for head-on collisions is found to be
161255, where the uncertainty is dominated by systematic eects. Comparisons of these
results to previous measurements and to various models are also presented.noneS. CHATRCHYAN; V. KHACHATRYAN; A.M. SIRUNYAN; A. TUMASYAN; W. ADAM; T. BERGAUER; M. DRAGICEVIC; J. ER N(O; C. FABJAN; M. FRIEDL; R. FRUHWIRTH; V.M. GHETE; J. HAMMER; S. H N(ANSEL; C. HARTL; M. HOCH; N. H N(ORMANN; J. HRUBEC; M. JEITLER; G. KASIECZKA; W. KIESENHOFER; M. KRAMMER; D. LIKO; I. MIKULEC; M. PERNICKA; H. ROHRINGER; R. SCH N(OFBECK; J. STRAUSS; A. TAUROK; F. TEISCHINGER; W.WALTENBERGER; G.WALZEL; E.WIDL; C.-E.WULZ; V. MOSSOLOV; N. SHUMEIKO; J. SUAREZ GONZALEZ; L. BENUCCI; L. CEARD; E.A. DE WOLF; X. JANSSEN; T. MAES; L. MUCIBELLO; S. OCHESANU; B. ROLAND; R. ROUGNY; M. SELVAGGI; H. VAN HAEVERMAET; P. VAN MECHELEN; N. VAN REMORTEL; V. ADLER; S. BEAUCERON; S. BLYWEERT; J. DâHONDT; O. DEVROEDE; A. KALOGEROPOULOS; J. MAES; M. MAES; S. TAVERNIER; W. VAN DONINCK; P. VAN MULDERS; I. VILLELLA; E.C. CHABERT; O. CHARAF; B. CLERBAUX; G. DE LENTDECKER; V. DERO; A.P.R. GAY; G.H. HAMMAD; T. HREUS; P.E. MARAGE; C. 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CARRILLO MORENO; F. VAZQUEZ VALENCIA; H.A. SALAZAR IBARGUEN; E. CASIMIRO LINARES; A. MORELOS PINEDA; M.A. REYES-SANTOS; P. ALLFREY; D. KROFCHECK; J. TAM; P.H. BUTLER; R. DOESBURG; H. SILVERWOOD; M. AHMAD; I. AHMED; M.I. ASGHAR; H.R. HOORANI; W.A. KHAN; T. KHURSHID; S. QAZI; M. CWIOK; W. DOMINIK; K. DOROBA; A. KALINOWSKI; M. KONECKI; J. KROLIKOWSKI; T. FRUEBOES; R. GOKIELI; M. G N4ORSKI; M. KAZANA; K. NAWROCKI; M. SZLEPER; G. WROCHNA; P. ZALEWSKI; N. ALMEIDA; A. DAVID; P. FACCIOLI; P.G. FERREIRA PARRACHO; M. GALLINARO; P. MARTINS; G. MINI; P. MUSELLA; A. NAYAK; L. RAPOSO; P.Q. RIBEIRO; J. SEIXAS; P. SILVA; D. SOARES; J. VARELA; H.K.W N(OHRI; I. BELOTELOV; P. BUNIN; M. FINGER; M. FINGER JR.; I. GOLUTVIN; A. KAMENEV; V. KARJAVIN; G. KOZLOV; A. LANEV; P. MOISENZ; V. PALICHIK; V. PERELYGIN; S. SHMATOV; V. SMIRNOV; A. VOLODKO; A. ZARUBIN; N. BONDAR; V. GOLOVTSOV; Y. IVANOV; V. KIM; P. LEVCHENKO; V. MURZIN; V. ORESHKIN; I. SMIRNOV; V. SULIMOV; L. UVAROV; S. VAVILOV; A. VOROBYEV; YU. ANDREEV; S. GNINENKO; N. GOLUBEV; M. KIRSANOV; N. KRASNIKOV; V. MATVEEV; A. PASHENKOV; A. TOROPIN; S. TROITSKY; V. EPSHTEYN; V. GAVRILOV; V. KAFTANOV; M. KOSSOV; A. KROKHOTIN; S. KULESHOV; N. LYCHKOVSKAYA; A. OULIANOV; G. SAFRONOV; S. SEMENOV; I. SHREYBER; V. STOLIN; E. VLASOV; A. ZHOKIN; E. BOOS; M. DUBININ; L. DUDKO; A. ERSHOV; A. GRIBUSHIN; O. KODOLOVA; I. LOKHTIN; S. OBRAZTSOV; S. PETRUSHANKO; L. SARYCHEVA; V. SAVRIN; A. SNIGIREV; V. ANDREEV; M. AZARKIN; I. DREMIN; M. KIRAKOSYAN; S.V. RUSAKOV; A. VINOGRADOV; I. AZHGIREY; S. BITIOUKOV; V. GRISHIN1; V. KACHANOV; D. KONSTANTINOV; V. KRYCHKINE; V. PETROV; R. RYUTIN; S. SLABOSPITSKY; A. SOBOL; L. TOURTCHANOVITCH; S. TROSHIN; N. TYURIN; A. UZUNIAN; A. VOLKOV; P. ADZIC; M. DJORDJEVIC; D. KRPIC; D. MALETIC; J. MILOSEVIC; J. PUZOVIC; M. AGUILAR-BENITEZ; J. ALCARAZ MAESTRE; P. ARCE; C. BATTILANA; E. CALVO; M. CEPEDA; M. CERRADA; N. COLINO; B. DE LA CRUZ; C. DIEZ PARDOS; C. FERNANDEZ BEDOYA; J.P. FERN N4ANDEZ RAMOS; A. FERRANDO; J. FLIX; M.C. FOUZ; P. GARCIA-ABIA; O. GONZALEZ LOPEZ; S. GOY LOPEZ; J.M. HERNANDEZ; M.I. JOSA; G. MERINO; J. PUERTA PELAYO; I. REDONDO; L. ROMERO; J. SANTAOLALLA; C. WILLMOTT; C. ALBAJAR; G. CODISPOTI; J.F. DE TROC N4ONIZ; J. CUEVAS; J. FERNANDEZ MENENDEZ; S. FOLGUERAS; I. GONZALEZ CABALLERO; L. LLORET IGLESIAS; J.M. VIZAN GARCIA; I.J. CABRILLO; A. CALDERON; M. CHAMIZO LLATAS; S.H. CHUANG; I. DIAZ MERINO; C. DIEZ GONZALEZ; J. DUARTE CAMPDERROS; M. FELCINI; M. FERNANDEZ; G. GOMEZ; J. GONZALEZ SANCHEZ; R. GONZALEZ; SUAREZ; C. JORDA; P. LOBELLE PARDO; A. LOPEZ VIRTO; J. MARCO; R. MARCO; C. MARTINEZ RIVERO; F. MATORRAS; J. PIEDRA GOMEZ; T. RODRIGO; A. RUIZ JIMENO; L. SCODELLARO; M. SOBRON SANUDO; I. VILA; R. VILAR CORTABITARTE; D. ABBANEO; E. AUFFRAY; P. BAILLON; A.H. BALL; D. BARNEY; F. BEAUDETTE; A.J. BELL; D. BENEDETTI; C. BERNET; A.K. BHATTACHARYYA; W. BIALAS; P. BLOCH; A. BOCCI; S. BOLOGNESI; H. BREUKER; G. BRONA; K. BUNKOWSKI; T. CAMPORESI; E. CANO; A. CATTAI; G. CERMINARA; T. 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AGOSTINO; J. ALEXANDER; F. BLEKMAN; A. CHATTERJEE; S. DAS; N. EGGERT; L.J. FIELDS; L.K. GIBBONS; B. HELTSLEY; K. HENRIKSSON; W. HOPKINS; A. KHUKHUNAISHVILI; B. KREIS; V. KUZNETSOV; Y. LIU; G. NICOLAS KAUFMAN; J.R. PATTERSON; D. PUIGH; D. RILEY; A. RYD; M. SAELIM; X. SHI; W. SUN; W.D. TEO; J. THOM; J. THOMPSON; J. VAUGHAN; Y.WENG; P.WITTICH; A. BISELLI; G. CIRINO; D. WINN; S. ABDULLIN; M. ALBROW; J. ANDERSON; G. APOLLINARI; M. ATAC; J.A. BAKKEN; S. BANERJEE; L.A.T. BAUERDICK; A. BERETVAS; J. BERRYHILL; P.C. BHAT; I. BLOCH; F. BORCHERDING; K. BURKETT; J.N. BUTLER; V. CHETLURU; H.W.K. CHEUNG; F. CHLEBANA; S. CIHANGIR; M. DEMARTEAU; D.P. EARTLY; V.D. ELVIRA; I. FISK; J. FREEMAN; Y. GAO; E. GOTTSCHALK; D. GREEN; K. GUNTHOTI; O. GUTSCHE; A. HAHN; J. HANLON; R.M. HARRIS; J. HIRSCHAUER; E. JAMES; H. JENSEN; M. JOHNSON; U. JOSHI; R. KHATIWADA; B. KILMINSTER; B. KLIMA; K. KOUSOURIS; S. KUNORI; S. KWAN; P. LIMON; R. LIPTON; J. LYKKEN; K. MAESHIMA; J.M. MARRAFFINO; D. MASON; P. MCBRIDE; T. MCCAULEY; T. MIAO; K. MISHRA; S. MRENNA; Y. MUSIENKO; C. NEWMAN-HOLMES; V. OâDELL; S. POPESCU; R. PORDES; O. PROKOFYEV; N. SAOULIDOU; E. SEXTON-KENNEDY; S. SHARMA; A. SOHA; W.J. SPALDING; L. SPIEGEL; P. TAN; L. TAYLOR; S. TKACZYK; L. UPLEGGER; E.W. VAANDERING; R. VIDAL; J. WHITMORE; W. WU; F. Y
The epidemiology of the metabolic syndrome and its association with diabetes, cardiovascular disease and other conditions
See paper for full list of authorsMeasurements of inclusive W and Z boson production cross sections in pp collisions at sqrt(s)=7 TeV are presented, based on 2.9 inverse picobarns of data recorded by the CMS detector at the LHC. The measurements, performed in the electron and muon decay channels, are combined to give sigma(pp to WX) times B(W to muon or electron + neutrino) = 9.95 \pm 0.07(stat.) \pm 0.28(syst.) \pm 1.09(lumi.) nb and sigma(pp to ZX) times B(Z to oppositely charged muon or electron pairs) = 0.931 \pm 0.026(stat.) \pm 0.023(syst.) \pm 0.102(lumi.) nb. Theoretical predictions, calculated at the next-to-next-to-leading order in QCD using recent parton distribution functions, are in agreement with the measured cross sections. Ratios of cross sections, which incur an experimental systematic uncertainty of less than 4%, are also reported
Charged particle multiplicities in interactions at , 2.36, and 7 TeV
Measurements of primary charged hadron multiplicity distributions are presented for non-single-diffractive events in proton-proton collisions at centre-of-mass energies of s â =0.9 s=0.9, 2.36, and 7 TeV, in five pseudorapidity ranges from |Ρ| < 0.5 to |Ρ| < 2.4. The data were collected with the minimum-bias trigger of the CMS experiment during the LHC commissioning runs in 2009 and the 7 TeV run in 2010. The multiplicity distribution at s â =0.9TeV s=0.9TeV is in agreement with previous measurements. At higher energies the increase of the mean multiplicity with s â s is underestimated by most event generators. The average transverse momentum as a function of the multiplicity is also presented. The measurement of higher-order moments of the multiplicity distribution confirms the violation of Koba-Nielsen-Olesen scaling that has been observed at lower energies
Upsilon production cross section in pp collisions at sqrt(s)=7 TeV
See paper for full list of authorsThe Upsilon production cross section in proton-proton collisions at sqrt(s) = 7 TeV is measured using a data sample collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 3.1 +/- 0.3 inverse picobarns. Integrated over the rapidity range |y|<2, we find the product of the Upsilon(1S) production cross section and branching fraction to dimuons to be sigma(pp to Upsilon(1S) X) B(Upsilon(1S) to mu+ mu-) = 7.37 +/- 0.13^{+0.61}_{-0.42}\pm 0.81 nb, where the first uncertainty is statistical, the second is systematic, and the third is associated with the estimation of the integrated luminosity of the data sample. This cross section is obtained assuming unpolarized Upsilon(1S) production. If the Upsilon(1S) production polarization is fully transverse or fully longitudinal the cross section changes by about 20%. We also report the measurement of the Upsilon(1S), Upsilon(2S), and Upsilon(3S) differential cross sections as a function of transverse momentum and rapidity
Study of Z boson production in PbPb collisions at âs NN=2.76TeV
ArtĂculo escrito por un elevado nĂşmero de autores, solo se referencian el que aparece en primer lugar, el nombre del grupo de colaboraciĂłn, si le hubiere, y los autores pertenecientes a la UAMA search for Z bosons in the Îź+Îź- decay channel has been performed in PbPb collisions at âsNN=2.76TeV with the CMS detector at the LHC, in a 7.2 Îźb-1 data sample. The number of opposite-sign muon pairs observed in the 60-120GeV/c2 invariant mass range is 39, corresponding to a yield per unit of rapidity (y) and per minimum bias event of [33.8Âą5.5(stat)Âą4.4(syst)]Ă10-8, in the |y|<2.0 range. Rapidity, transverse momentum, and centrality dependencies are also measured. The results agree with next-to-leading order QCD calculations, scaled by the number of incoherent nucleon-nucleon collisionsWe thank the technical and administrative staff at CERN and other CMS institutes, and acknowledge support from FMSR (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); Academy of Sciences and NICPB (Estonia); Academy of Finland, ME, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); PAEC (Pakistan); SCSR (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MST and MAE (Russia); MSTD (Serbia); MICINN and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); TUBITAK and TAEK (Turkey); STFC (United Kingdom); DOE and NSF (USA