Event Structure and Double Helicity Asymmetry in Jet Production from Polarized p+p Collisions at sqrt(s) = 200 GeV

preprint2010arXivOpen access
A. AdareS. AfanasievC. AidalaN. N. AjitanandY. AkibaH. Al-BatainehJ. AlexanderK. AokiL. AphecetcheR. ArmendarizS. H. AronsonJ. AsaiE. T. AtomssaR. AverbeckT. C. AwesB. AzmounV. BabintsevG. BaksayL. BaksayA. BaldisseriK. N. BarishP. D. BarnesB. BassalleckS. BatheS. BatsouliV. BaublisA. BazilevskyS. BelikovR. BennettY. BerdnikovA. A. BickleyJ. G. BoissevainH. BorelK. BoyleM. L. BrooksH. BueschingV. BumazhnovG. BunceS. ButsykS. CampbellB. S. ChangJ. -L. CharvetS. ChernichenkoJ. ChibaC. Y. ChiM. ChiuI. J. ChoiT. ChujoP. ChungA. ChurynV. CiancioloC. R. ClevenB. A. ColeM. P. CometsP. ConstantinM. CsanádT. CsörgőT. DahmsK. DasG. DavidM. B. DeatonK. DehmeltH. DelagrangeA. DenisovD. d'EnterriaA. DeshpandeE. J. DesmondO. DietzschA. DionM. DonadelliO. DrapierA. DreesA. K. DubeyA. DurumV. DzhordzhadzeY. V. EfremenkoJ. EgdemirF. EllinghausW. S. EmamA. EnokizonoH. En'yoS. EsumiK. O. EyserD. E. FieldsM. Finger JrM. FingerF. FleuretS. L. FokinZ. FraenkelJ. E. FrantzA. FranzA. D. FrawleyK. FujiwaraY. FukaoT. FusayasuS. GadratI. GarishviliA. GlennH. GongM. GoninJ. GossetY. GotoR. Granier de CassagnacN. GrauS. V. GreeneM. Grosse PerdekampT. GunjiH. -Å. GustafssonT. HachiyaA. Hadj HenniC. HaegemannJ. S. HaggertyH. HamagakiR. HanH. HaradaE. P. HartouniK. HarunaE. HaslumR. HayanoM. HeffnerT. K. HemmickT. HesterX. HeH. HiejimaJ. C. HillR. HobbsM. HohlmannW. HolzmannK. HommaB. HongT. HoraguchiD. HornbackT. IchiharaH. IinumaK. ImaiM. InabaY. InoueD. IsenhowerL. IsenhowerM. IshiharaT. IsobeM. IssahA. IsupovB. V. JacakJ. JiaJ. JinO. JinnouchiB. M. JohnsonK. S. JooD. JouanF. KajiharaS. KametaniN. KamiharaJ. KaminM. KanetaJ. H. KangH. KanouD. KawallA. V. KazantsevA. KhanzadeevJ. KikuchiD. H. KimD. J. KimE. KimE. KinneyÁ. KissE. KistenevA. KiyomichiJ. KlayC. Klein-BoesingL. KochendaV. KochetkovB. KomkovM. KonnoD. KotchetkovA. KozlovA. KrálA. KravitzJ. KubartG. J. KundeN. KuriharaK. KuritaM. J. KweonY. KwonG. S. KyleR. LaceyY. S. LaiJ. G. LajoieA. LebedevD. M. LeeM. K. LeeT. LeeM. J. LeitchM. A. L. LeiteB. LenziT. LiškaA. LitvinenkoM. X. LiuX. LiB. LoveD. LynchC. F. MaguireY. I. MakdisiA. MalakhovM. D. MalikV. I. MankoY. MaoL. MašekH. MasuiF. MatathiasM. McCumberP. L. McGaugheyY. MiakeP. MikešK. MikiT. E. MillerA. MilovS. MioduszewskiM. MishraJ. T. MitchellM. MitrovskiA. MorrealeD. P. MorrisonT. V. MoukhanovaD. MukhopadhyayJ. MurataS. NagamiyaY. NagataJ. L. NagleM. NaglisI. NakagawaY. NakamiyaT. NakamuraK. NakanoJ. NewbyM. NguyenB. E. NormanR. NouicerA. S. NyaninE. O'BrienS. X. OdaC. A. OgilvieH. OhnishiK. OkadaM. OkaO. O. OmiwadeA. OskarssonM. OuchidaK. OzawaR. PakD. PalA. P. T. PalounekV. PantuevV. PapavassiliouJ. ParkW. J. ParkS. F. PateH. PeiJ. -C. PengH. PereiraV. PeresedovD. Yu. PeressounkoC. PinkenburgM. L. PurschkeA. K. PurwarH. QuJ. RakA. RakotozafindrabeI. RavinovichK. F. ReadS. RembeczkiM. ReuterK. ReygersV. RiabovY. RiabovG. RocheA. RomanaM. RosatiS. S. E. RosendahlP. RosnetP. RukoyatkinV. L. RykovB. SahlmuellerN. SaitoT. SakaguchiS. SakaiH. SakataV. SamsonovS. SatoS. SawadaJ. SeeleR. SeidlV. SemenovR. SetoD. SharmaI. SheinA. ShevelT. -A. ShibataK. ShigakiM. ShimomuraK. ShojiA. SicklesC. L. SilvaD. SilvermyrC. SilvestreK. S. SimC. P. SinghV. SinghS. SkutnikM. SlunečkaA. SoldatovR. A. SoltzW. E. SondheimS. P. SorensenI. V. SourikovaF. StaleyP. W. StankusE. StenlundM. StepanovA. SterS. P. StollT. SugitateC. SuireJ. SziklaiT. TabaruS. TakagiE. M. TakaguiA. TaketaniY. TanakaK. TanidaM. J. TannenbaumA. TaranenkoP. TarjánT. L. ThomasM. TogawaA. ToiaJ. TojoL. TomášekH. ToriiR. S. TowellV. -N. TramI. TserruyaY. TsuchimotoC. ValeH. ValleH. W. van HeckeJ. VelkovskaR. VértesiA. A. VinogradovM. ViriusV. VrbaE. VznuzdaevM. WagnerD. WalkerX. R. WangY. WatanabeJ. WesselsS. N. WhiteD. WinterC. L. WoodyM. WysockiW. XieY. L. YamaguchiA. YanovichZ. YasinJ. YingS. YokkaichiG. R. YoungI. YounusI. E. YushmanovW. A. ZajcO. ZaudtkeC. ZhangS. ZhouJ. ZimányiL. Zolin

Abstract

We report on event structure and double helicity asymmetry (ALLA_LL) of jet production in longitudinally polarized p+p collisions at s\sqrt{s}=200 GeV. Photons and charged particles were measured at midrapidity ∣η∣<0.35|η| < 0.35 with the requirement of a high-momentum (>2>2 GeV/cc) photon in each event. Measured event structure is compared with {\sc pythia} and {\sc geant} simulations. The shape of jets and the underlying event were well reproduced at this collision energy. For the measurement of jet ALLA_{LL}, photons and charged particles were clustered with a seed-cone algorithm to obtain the cluster pTp_T sum (pTrecop_T^{\rm reco}). The effect of detector response and the underlying events on pTrecop_T^{\rm reco} was evaluated with the simulation. The production rate of reconstructed jets is satisfactorily reproduced with the NLO pQCD jet production cross section. For 4<pTreco<124 < p_T^{\rm reco} < 12 GeV/cc with an average beam polarization of <P>=49< P > = 49% we measured ALL=−0.0014±0.0037statA_{LL} = -0.0014 \pm 0.0037^{\rm stat} at the lowest pTrecop_T^{\rm reco} bin (4-5 GeV/cc) and −0.0181±0.0282stat-0.0181 \pm 0.0282^{\rm stat} at the highest pTrecop_T^{\rm reco} bin (10-12 GeV/cc) with a beam polarization scale error of 9.4% and a $\pT$ scale error of 10%. Jets in the measured pTrecop_T^{\rm reco} range arise primarily from hard-scattered gluons with momentum fraction 0.02<x<0.30.02 < x < 0.3 according to {\sc pythia}. The measured ALLA_{LL} is compared with predictions that assume various ΔG(x)ΔG(x) distributions based on the GRSV parameterization. The present result imposes the limit −1.1<∫0.020.3dxΔG(x,μ2=1GeV2)<0.4-1.1 < \int_{0.02}^{0.3}dx ΔG(x, μ^2 = 1 {\rm GeV}^2) < 0.4 at 95% confidence level or ∫0.020.3dxΔG(x,μ2=1GeV2)<0.5\int_{0.02}^{0.3}dx ΔG(x, μ^2 = 1 {\rm GeV}^2) < 0.5 at 99% confidence level.

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