6533b7d1fe1ef96bd125caf3
RESEARCH PRODUCT
Search for muoproduction of X(3872) at COMPASS and indication of a new state X˜(3872)
L. SilvaL. SilvaS.s. DasguptaS.s. DasguptaA.g. ChumakovA.g. ChumakovJ. NovýJ. NovýJ. NovýY. MiyachiY. MiyachiP.d. EversheimP.d. EversheimP. ZavadaP. ZavadaE. ZemlyanichkinaE. ZemlyanichkinaFrançois HerrmannFrançois HerrmannS. UhlS. UhlY. BedferY. BedferA. AntoshkinA. AntoshkinG. SbrizzaiG. SbrizzaiN.s. RogachevaN.s. RogachevaA. FerreroA. FerreroG.v. KhaustovG.v. KhaustovA. MagnonA. MagnonF. PereiraF. PereiraI. KonorovI. KonorovI. KonorovJ. Ter WolbeekJ. Ter WolbeekMaria Liz CrespoC. RegaliC. RegaliJ. MarzecJ. MarzecA. KvetonA. KvetonG.d. AlexeevG.d. AlexeevK. SchmidtK. SchmidtP. KremserP. KremserO.yu. DenisovF. GautheronF. GautheronF. NerlingF. NerlingYu.a. KhokhlovYu.a. KhokhlovK. KondoK. KondoN. C. R. MakinsN. C. R. MakinsM. FaesslerV.n. KolosovV.n. KolosovA. AmorosoA. AmorosoH. MatsudaH. MatsudaD. NeyretD. NeyretC.d.r. AzevedoC.d.r. AzevedoV. JaryV. JaryV. AnosovV. AnosovM. Grosse PerdekampM. Grosse PerdekampS. SarkarS. SarkarY.-s. LianY.-s. LianR. BeckR. BeckA. SelyuninA. SelyuninB. GrubeB. GrubeM. StolarskiM. StolarskiM. TasevskyM. TasevskyT. SawadaT. SawadaN. HorikawaN. HorikawaM. SulcS. TessaroD. HahneD. HahneV.d. SamoylenkoV.d. SamoylenkoJ. GiarraJ. GiarraN. D'hoseN. D'hoseW. MeyerW. MeyerR. JoostenR. JoostenAndres CicuttinO. SubrtO. SubrtO. SubrtS. WallnerS. WallnerS. PlatchkovS. PlatchkovR. SalacR. SalacJen-chieh PengJen-chieh PengV.a. PolyakovV.a. PolyakovJ. VelosoJ. VelosoN. ZhuravlevN. ZhuravlevG.v. MeshcheryakovG.v. MeshcheryakovA. SandaczM. ViriusM. ViriusF. H. HeinsiusF. H. HeinsiusS. IshimotoS. IshimotoM. AghasyanA.m. KotzinianA.m. KotzinianM. ZavertyaevM. ZavertyaevJan MatousekJan MatousekJan MatousekG. ReicherzG. ReicherzS. Dalla TorreC. QuintansC. QuintansM. PešekM. PešekJ. BarthJ. BarthAlan D. MartinAlan D. MartinM. ChiossoM. ChiossoN.v. AnfimovN.v. AnfimovJan TomsaJan TomsaM. OstrickM. OstrickR.p. KurjataR.p. KurjataM. FingerM. FingerE. KabußE. KabußR.r. DusaevR.r. DusaevA.s. NunesA.s. NunesT. WeisrockT. WeisrockR. BirsaK. AugstenK. AugstenK. AugstenV. FrolovV. FrolovV. FrolovA. MaggioraA. VauthA. VauthA.a. LednevA.a. LednevV.e. LyubovitskijV.e. LyubovitskijC. ChatterjeeC. ChatterjeeP. JörgP. JörgYakov Petrovich KulinichYakov Petrovich KulinichGerhard K. MallotGerhard K. MallotAndrey IvanovAndrey IvanovFrank KleinFrank KleinP. BordaloP. BordaloA. NagaytsevA. NagaytsevJohannes BernhardJohannes BernhardJohannes BernhardCh. DreisbachCh. DreisbachD. PanzieriK. ZarembaK. ZarembaE.r. BielertE.r. BielertMarkus F. KrämerMarkus F. KrämerJ. PochodzallaJ. PochodzallaK. KönigsmannK. KönigsmannM. SluneckaM. SluneckaA. GuskovA. GuskovJ.m. FriedrichJ.m. FriedrichA. SrnkaH. SuzukiH. SuzukiS. DasguptaS. DasguptaB. MarianskiT. GrussenmeyerT. GrussenmeyerA. RybnikovA. RybnikovAndrea BressanAndrea BressanAnatoli Vasilievich EfremovAnatoli Vasilievich EfremovL. DharaL. DharaT. MatsudaT. MatsudaM. MeyerM. MeyerM. MeyerM. DziewieckiM. DziewieckiMarkus BallMarkus BallM. GorzellikM. GorzellikW.-d. NowakW.-d. NowakYu. KisselevYu. KisselevP. SchiavonP. SchiavonC. SantosE. MitrofanovE. MitrofanovBakur ParsamyanBakur ParsamyanW. DünnweberMartin BodlakMartin BodlakYu. IvanshinYu. IvanshinM.g. AlexeevM.g. AlexeevIlya KuznetsovIlya KuznetsovW. C. ChangW. C. ChangS.v. DonskovS.v. DonskovD. SteffenD. SteffenD. SteffenM. WilfertM. WilfertJ. SmolikJ. SmolikK. BickerK. BickerK. BickerS. RamosS. RamosL. SinhaL. SinhaJ. PretzJ. PretzE. FucheyE. FucheyS. LevoratoA. AustregesiloA. AustregesiloA. GridinA. GridinI. J. ChoiI. J. ChoiN. MitrofanovN. MitrofanovC. FrancoC. FrancoStephan M. PaulStephan M. PaulM. LevillainM. LevillainA. ThielA. ThielC. RiedlC. RiedlV. AndrieuxV. AndrieuxV. AndrieuxMikhail MikhasenkoMikhail MikhasenkoF. KrinnerF. KrinnerI.a. SavinI.a. SavinO.p. GavrichtchoukO.p. GavrichtchoukN. MakkeI. OrlovI. OrlovA. SzabelskiA. SzabelskiF. GiordanoF. GiordanoE.a. LevchenkoE.a. LevchenkoN. Du Fresne Von HohenescheN. Du Fresne Von HohenescheN. Du Fresne Von HohenescheS. GerassimovS. GerassimovS. GerassimovN. PierreN. PierreN. PierreR. LongoR. LongoM. QuaresmaM. QuaresmaN. DoshitaN. DoshitaB. KetzerB. KetzerA. VidonA. VidonYu.v. MikhailovYu.v. MikhailovI. GnesiI. GnesiG. HamarV.f. KonstantinovV.f. KonstantinovP. SznajderZ. KralZ. KralT. IwataT. IwataB.i. VasilishinB.i. VasilishinA. GrassoA. GrassoV. TskhayV. TskhayH. FischerH. FischerM. ZiembickiM. ZiembickiM. BücheleM. BücheleA. RychterA. RychterS. SirtlS. SirtlZ.v. KroumchteinZ.v. KroumchteinF. BalestraF. BalestraS.-u. ChungS.-u. ChungF. ToselloT. SzameitatT. SzameitatD. Von HarrachD. Von HarrachK. SchönningK. SchönningF. TessarottoJ.h. KoivuniemiJ.h. KoivuniemiJ.h. KoivuniemiFranco BradamanteFranco BradamanteA. KerbiziA. KerbiziJ. LichtenstadtJ. LichtenstadtF. KunneF. KunneM. PeškováM. PeškováE. SederE. SederK. KurekG. NukazukaG. NukazukaD.v. PeshekhonovD.v. PeshekhonovR. HeitzR. HeitzO.m. KouznetsovO.m. KouznetsovV.e. BurtsevV.e. BurtsevR. AkhunzyanovR. AkhunzyanovS.a. MamonS.a. MamonH. SchmiedenH. SchmiedenC.-y. HsiehC.-y. HsiehB. BadełekB. BadełekW. AugustyniakD.i. RyabchikovD.i. RyabchikovD.i. RyabchikovA.g. OlshevskyA.g. OlshevskyS. HuberS. Hubersubject
PhysicsNuclear and High Energy PhysicsMuonMass distribution010308 nuclear & particles physicsBranching fractionHadronState (functional analysis)01 natural sciencesMomentum0103 physical sciencesTetraquarkAtomic physics010306 general physicsX(3872)description
Abstract We have searched for exclusive production of exotic charmonia in the reaction μ + N → μ + ( J / ψ π + π − ) π ± N ′ using COMPASS data collected with incoming muons of 160 GeV/c and 200 GeV/c momentum. In the J / ψ π + π − mass distribution we observe a signal with a statistical significance of 4.1 σ. Its mass and width are consistent with those of the X ( 3872 ) . The shape of the π + π − mass distribution from the observed decay into J / ψ π + π − shows disagreement with previous observations for X ( 3872 ) . The observed signal may be interpreted as a possible evidence of a new charmonium state. It could be associated with a neutral partner of X ( 3872 ) with C = − 1 predicted by a tetraquark model. The product of cross section and branching fraction of the decay of the observed state into J / ψ π + π − is determined to be 71±28(stat)±39(syst) pb.
year | journal | country | edition | language |
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2018-08-01 | Physics Letters B |