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Related papers: Eta-eta' mixing from V->Pgamma and J/psi->VP decay…

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We perform a thorough analysis of the VP\gamma(\gamma*) and P\gamma\gamma(\gamma*) decays in the resonance chiral theory, where V stand for the vector resonances \rho, K*, \omega, \phi, P stand for \pi, K, \eta, \eta' and \gamma*…

High Energy Physics - Phenomenology · Physics 2013-05-30 Yun-Hua Chen , Zhi-Hui Guo , Han-Qing Zheng

We study $B\to J/\Psi \eta^{(\prime)}$ decays and suggest two methods to determine the $\eta-\eta^{\prime}$ mixing angle. We calculate not only the factorizable contribution in QCD facorization scheme but also the nonfactorizable hard…

High Energy Physics - Phenomenology · Physics 2016-09-08 Jing-Wu Li , Dong-Sheng Du

We present further tests and applications of the new eta-eta' mixing scheme recently proposed by us. The particle states are decomposed into orthonormal basis vectors in a light-cone Fock representation. Because of flavor symmetry breaking…

High Energy Physics - Phenomenology · Physics 2009-10-31 T. Feldmann , P. Kroll , B. Stech

We study the radiative decays $h_{c}\rightarrow\gamma\eta^{(\prime)}$ in the framework of perturbative QCD and evaluate analytically the one-loop integrals with the light quark masses kept. Interestingly, the branching ratios…

High Energy Physics - Phenomenology · Physics 2019-08-27 Chao-Jie Fan , Jun-Kang He

With the recent investigations of $g^{\ast}g^{\ast}-\eta^{(\prime)}$ transition form factor and $\eta-\eta^{\prime}$ mixing scheme, we present an updated study of the radiative decays $J/\Psi\to\eta^{(\prime)}\gamma$ in perturbative QCD.…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ya-Dong Yang

An enhanced phenomenological model that includes isospin-symmetry breaking is presented in this letter. The model is then used in a number of statistical fits to the most recent experimental data for the radiative transitions $V\!P\gamma$…

High Energy Physics - Phenomenology · Physics 2020-06-16 Rafel Escribano , Emilio Royo

We introduce a parametrization scheme for $J/\psi(\psi^\prime)\to VP$ where the effects of SU(3) flavor symmetry breaking and doubly OZI-rule violation (DOZI) can be parametrized by certain parameters with explicit physical interpretations.…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gang Li , Qiang Zhao , Chao-Hsi Chang

We include the $\eta_c$ meson into the $\eta$-$\eta'$-$G$ mixing formalism constructed in our previous work, where $G$ represents the pseudoscalar gluball. The mixing angles in this tetramixing matrix are constrained by theoretical and…

High Energy Physics - Phenomenology · Physics 2012-02-07 Yu-Dai Tsai , Hsiang-nan Li , Qiang Zhao

Eta bound states in nuclei are sensitive to the flavour-singlet component in the eta. The bigger the singlet component, the more attraction and the greater the binding. eta-etaprime mixing plays an important role in understanding the value…

High Energy Physics - Phenomenology · Physics 2010-12-17 Steven D. Bass , Anthony W. Thomas

The quark/gluon content of eta(1295) and eta(1440) mesons is discussed, mesons being considered as members of the first radial excitation 2^1S_0 qqbar nonet. Recent results on eta(1295) and eta(1440) two-photon widths from L3 together with…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. V. Anisovich

The mixing of $\eta-\eta'$ or $\eta-\eta'-G$ is of a great theoretical interest, because it concerns many aspects of the underlying dynamics and hadronic structure of pseudoscalar mesons and glueball. Determining the mixing parameters by…

High Energy Physics - Phenomenology · Physics 2011-02-09 Hong-Wei Ke , Xue-Qian Li , Zheng-Tao Wei

The $\eta-\eta^{\prime}$ mixture is discussed in the chiral bag model to calculate the pseudoscalar octet-singlet mixing angle consistent with the experimental data. The color anomaly is taken into account with the modified boundary…

Nuclear Theory · Physics 2016-09-08 Soon-Tae Hong , Dong-Pil Min

Mixing of the pseudoscalar mesons is discussed in the quark-flavor basis. The divergences of the axial vector currents which embody the axial vector anomaly, combined with the assumption that the decay constants follow the pattern of…

High Energy Physics - Phenomenology · Physics 2025-01-22 P. Kroll

I review to which extent the properties of pseudoscalar mesons can be understood in terms of the underlying quark (and eventually gluon) structure. Special emphasis is put on the progress in our understanding of eta-eta' mixing.…

High Energy Physics - Phenomenology · Physics 2014-11-17 Thorsten Feldmann

It has been realized for a long time that knowing the eta and eta^prime wave functions in terms of quark and gluon components probes our understanding of non-perturbative QCD dynamics. Great effort has been given to this challenge -- yet no…

High Energy Physics - Phenomenology · Physics 2012-02-03 Camilla Di Donato , Giulia Ricciardi , Ikaros Bigi

We compute the masses and decay widths of gluonia using QCD spectral sum rules and low-energy theorems. In the scalar sector, one finds a gluonium having a mass $M_G=(1.5\pm 0.2)$ GeV, which decays mainly into the $U(1)_A$ channels…

High Energy Physics - Phenomenology · Physics 2008-11-26 Stephan Narison

Instead of the glueball-$\eta'$ mixing ansatz, the latest measured ratios of the branching fractions of $B_{(s)}^0\to J/\psi \eta^{(\prime)}$ decays by LHCb can be understood by including the contribution from the light quark annihilation…

High Energy Physics - Phenomenology · Physics 2025-07-30 Ying Chen , Geng Li

Mixing of the pseudoscalar mesons is discussed in the quark-flavor basis with the hypothesis that the basis decay constants follow the pattern of particle state mixing. The divergences of the axial vector currents which embody the axial…

High Energy Physics - Phenomenology · Physics 2025-01-22 P. Kroll

A study of $B^0$~and $B^0_s$ meson decays into $J/\psi\eta$~and $J/\psi\eta^{\prime}$ final states is performed using a data set of proton-proton collisions at centre-of-mass energies of 7 and 8TeV, collected by the LHCb experiment and…

High Energy Physics - Experiment · Physics 2015-01-28 LHCb collaboration , R. Aaij , B. Adeva , M. Adinolfi , A. Affolder , Z. Ajaltouni , S. Akar , J. Albrecht , F. Alessio , M. Alexander , S. Ali , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , S. Amerio , Y. Amhis , L. An , L. Anderlini , J. Anderson , R. Andreassen , M. Andreotti , J. E. Andrews , R. B. Appleby , O. Aquines Gutierrez , F. Archilli , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , M. Baalouch , S. Bachmann , J. J. Back , A. Badalov , C. Baesso , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , V. Batozskaya , V. Battista , A. Bay , L. Beaucourt , J. Beddow , F. Bedeschi , I. Bediaga , S. Belogurov , K. Belous , I. Belyaev , E. Ben-Haim , G. Bencivenni , S. Benson , J. Benton , A. Berezhnoy , R. Bernet , AB Bertolin , M. -O. Bettler , M. van Beuzekom , A. Bien , S. Bifani , T. Bird , A. Bizzeti , P. M. Bjørnstad , T. Blake , F. Blanc , J. Blouw , S. Blusk , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , A. Borgia , M. Borsato , T. J. V. Bowcock , E. Bowen , C. Bozzi , D. Brett , M. Britsch , T. Britton , J. Brodzicka , N. H. Brook , H. Brown , A. Bursche , J. Buytaert , S. Cadeddu , R. Calabrese , M. Calvi , M. Calvo Gomez , P. Campana , D. Campora Perez , L. Capriotti , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , L. Carson , K. Carvalho Akiba , RCM Casanova Mohr , G. Casse , L. Cassina , L. Castillo Garcia , M. Cattaneo , Ch. Cauet , R. Cenci , M. Charles , Ph. Charpentier , M. Chefdeville , S. Chen , S. -F. Cheung , N. Chiapolini , M. Chrzaszcz , X. Cid Vidal , G. Ciezarek , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , V. Coco , J. Cogan , E. Cogneras , V. Cogoni , L. Cojocariu , G. Collazuol , P. Collins , A. Comerma-Montells , A. Contu , A. Cook , M. Coombes , S. Coquereau , G. Corti , M. Corvo , I. Counts , B. Couturier , G. A. Cowan , D. C. Craik , A. C. Crocombe , M. Cruz Torres , S. Cunliffe , R. Currie , C. D'Ambrosio , J. Dalseno , P. David , P. N. Y. David , A. Davis , K. De Bruyn , S. De Capua , M. De Cian , J. M. De Miranda , L. De Paula , W. De Silva , P. De Simone , C. -T. Dean , D. Decamp , M. Deckenhoff , L. Del Buono , N. Déléage , D. Derkach , O. Deschamps , F. Dettori , A. Di Canto , H. Dijkstra , S. Donleavy , F. Dordei , M. Dorigo , A. Dosil Suárez , D. Dossett , A. Dovbnya , K. Dreimanis , G. Dujany , F. Dupertuis , P. Durante , R. Dzhelyadin , A. Dziurda , A. Dzyuba , S. Easo , U. Egede , V. Egorychev , S. Eidelman , S. Eisenhardt , U. Eitschberger , R. Ekelhof , L. Eklund , I. El Rifai , Ch. Elsasser , S. Ely , S. Esen , H. -M. Evans , T. Evans , A. Falabella , C. Färber , C. Farinelli , N. Farley , S. Farry , R. Fay , D. Ferguson , V. Fernandez Albor , F. Ferreira Rodrigues , M. Ferro-Luzzi , S. Filippov , M. Fiore , M. Fiorini , M. Firlej , C. Fitzpatrick , T. Fiutowski , P. Fol , M. Fontana , F. Fontanelli , R. Forty , O. Francisco , M. Frank , C. Frei , M. Frosini , J. Fu , E. Furfaro , A. Gallas Torreira , D. Galli , S. Gallorini , S. Gambetta , M. Gandelman , P. Gandini , Y. Gao , J. García Pardiñas , J. Garofoli , J. Garra Tico , L. Garrido , D. Gascon , C. Gaspar , U. Gastaldi , R. Gauld , L. Gavardi , G. Gazzoni , A. Geraci , E. Gersabeck , M. Gersabeck , T. Gershon , Ph. Ghez , A. Gianelle , S. Gianì , V. Gibson , L. Giubega , V. V. Gligorov , C. Göbel , D. Golubkov , A. Golutvin , A. Gomes , C. Gotti , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , E. Graverini , G. Graziani , A. Grecu , E. Greening , S. Gregson , P. Griffith , L. Grillo , O. Grünberg , B. Gui , E. Gushchin , Yu. Guz , T. Gys , C. Hadjivasiliou , G. Haefeli , C. Haen , S. C. Haines , S. Hall , B. Hamilton , T. Hampson , X. Han , S. Hansmann-Menzemer , N. Harnew , S. T. Harnew , J. Harrison , J. He , T. Head , V. Heijne , K. Hennessy , P. Henrard , L. Henry , J. A. Hernando Morata , E. van Herwijnen , M. Heß , A. Hicheur , D. Hill , M. Hoballah , C. Hombach , W. Hulsbergen , N. Hussain , D. Hutchcroft , D. Hynds , M. Idzik , P. Ilten , R. Jacobsson , A. Jaeger , J. Jalocha , E. Jans , P. Jaton , A. Jawahery , F. Jing , M. John , D. Johnson , C. R. Jones , C. Joram , B. Jost , N. Jurik , S. Kandybei , W. Kanso , M. Karacson , T. M. Karbach , S. Karodia , M. Kelsey , I. R. Kenyon , T. Ketel , B. Khanji , C. Khurewathanakul , S. Klaver , K. Klimaszewski , O. Kochebina , M. Kolpin , I. Komarov , R. F. Koopman , P. Koppenburg , M. Korolev , L. Kravchuk , K. Kreplin , M. Kreps , G. Krocker , P. Krokovny , F. Kruse , W. Kucewicz , M. Kucharczyk , V. Kudryavtsev , K. Kurek , T. Kvaratskheliya , V. N. La Thi , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , R. W. Lambert , G. Lanfranchi , C. Langenbruch , B. Langhans , T. Latham , C. Lazzeroni , R. Le Gac , J. van Leerdam , J. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , S. Leo , O. Leroy , T. Lesiak , B. Leverington , Y. Li , T. Likhomanenko , M. Liles , R. Lindner , C. Linn , F. Lionetto , B. Liu , S. Lohn , I. Longstaff , J. H. Lopes , P. Lowdon , D. Lucchesi , H. Luo , A. Lupato , E. Luppi , O. Lupton , F. Machefert , I. V. Machikhiliyan , F. Maciuc , O. Maev , S. Malde , A. Malinin , G. Manca , G. Mancinelli , A. Mapelli , J. Maratas , J. F. Marchand , U. Marconi , C. Marin Benito , P. Marino , R. Märki , J. Marks , G. Martellotti , A. Martín Sánchez , M. Martinelli , D. Martinez Santos , F. Martinez Vidal , D. Martins Tostes , A. Massafferri , R. Matev , Z. Mathe , C. Matteuzzi , A. Mazurov , M. McCann , J. McCarthy , A. McNab , R. McNulty , B. McSkelly , B. Meadows , F. Meier , M. Meissner , M. Merk , D. A. Milanes , M. -N. Minard , N. Moggi , J. Molina Rodriguez , S. Monteil , M. Morandin , P. Morawski , A. Mordà , M. J. Morello , J. Moron , A. -B. Morris , R. Mountain , F. Muheim , K. Müller , M. Mussini , B. Muster , P. Naik , T. Nakada , R. Nandakumar , I. Nasteva , M. Needham , N. Neri , S. Neubert , N. Neufeld , M. Neuner , A. D. Nguyen , T. D. Nguyen , C. Nguyen-Mau , M. Nicol , V. Niess , R. Niet , N. Nikitin , T. Nikodem , A. Novoselov , D. P. O'Hanlon , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , S. Ogilvy , O. Okhrimenko , R. Oldeman , C. J. G. Onderwater , M. Orlandea , J. M. Otalora Goicochea , A. Otto , P. Owen , A. Oyanguren , B. K. Pal , A. Palano , F. Palombo , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , L. L. Pappalardo , C. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , C. Patrignani , A. Pearce , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , P. Perret , M. Perrin-Terrin , L. Pescatore , E. Pesen , K. Petridis , A. Petrolini , E. Picatoste Olloqui , B. Pietrzyk , T. Pilař , D. Pinci , A. Pistone , S. Playfer , M. Plo Casasus , F. Polci , S. Polikarpov , A. Poluektov , I. Polyakov , E. Polycarpo , A. Popov , D. Popov , B. Popovici , C. Potterat , E. Price , J. D. Price , J. Prisciandaro , A. Pritchard , C. Prouve , V. Pugatch , A. Puig Navarro , G. Punzi , W. Qian , B. Rachwal , J. H. Rademacker , B. Rakotomiaramanana , M. Rama , M. S. Rangel , I. Raniuk , N. Rauschmayr , G. Raven , F. Redi , S. Reichert , M. M. Reid , A. C. dos Reis , S. Ricciardi , S. Richards , M. Rihl , K. Rinnert , V. Rives Molina , P. Robbe , A. B. Rodrigues , E. Rodrigues , P. Rodriguez Perez , S. Roiser , V. Romanovsky , A. Romero Vidal , M. Rotondo , J. Rouvinet , T. Ruf , H. Ruiz , P. Ruiz Valls , J. J. Saborido Silva , N. Sagidova , P. Sail , B. Saitta , V. Salustino Guimaraes , C. Sanchez Mayordomo , B. Sanmartin Sedes , R. Santacesaria , C. Santamarina Rios , E. Santovetti , A. Sarti , C. Satriano , A. Satta , D. M. Saunders , D. Savrina , M. Schiller , H. Schindler , M. Schlupp , M. Schmelling , B. Schmidt , O. Schneider , A. Schopper , M. -H. Schune , R. Schwemmer , B. Sciascia , A. Sciubba , A. Semennikov , I. Sepp , N. Serra , J. Serrano , L. Sestini , P. Seyfert , M. Shapkin , I. Shapoval , Y. Shcheglov , T. Shears , L. Shekhtman , V. Shevchenko , A. Shires , R. Silva Coutinho , G. Simi , M. Sirendi , N. Skidmore , I. Skillicorn , T. Skwarnicki , N. A. Smith , E. Smith , E. Smith , J. Smith , M. Smith , H. Snoek , M. D. Sokoloff , F. J. P. Soler , F. Soomro , D. Souza , B. Souza De Paula , B. Spaan , P. Spradlin , S. Sridharan , F. Stagni , M. Stahl , S. Stahl , O. Steinkamp , O. Stenyakin , S. Stevenson , S. Stoica , S. Stone , B. Storaci , S. Stracka , M. Straticiuc , U. Straumann , R. Stroili , L. Sun , W. Sutcliffe , K. Swientek , S. Swientek , V. Syropoulos , M. Szczekowski , P. Szczypka , T. Szumlak , S. T'Jampens , M. Teklishyn , G. Tellarini , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , J. Todd , S. Tolk , L. Tomassetti , D. Tonelli , S. Topp-Joergensen , N. Torr , E. Tournefier , S. Tourneur , M. T. Tran , M. Tresch , A. Trisovic , A. Tsaregorodtsev , P. Tsopelas , N. Tuning , M. Ubeda Garcia , A. Ukleja , A. Ustyuzhanin , U. Uwer , C. Vacca , V. Vagnoni , G. Valenti , A. Vallier , R. Vazquez Gomez , P. Vazquez Regueiro , C. Vázquez Sierra , S. Vecchi , J. J. Velthuis , M. Veltri , G. Veneziano , M. Vesterinen , B. Viaud , D. Vieira , M. Vieites Diaz , X. Vilasis-Cardona , A. Vollhardt , D. Volyanskyy , D. Voong , A. Vorobyev , V. Vorobyev , C. Voß , J. A. de Vries , R. Waldi , C. Wallace , R. Wallace , J. Walsh , S. Wandernoth , J. Wang , D. R. Ward , N. K. Watson , D. Websdale , M. Whitehead , D. Wiedner , G. Wilkinson , M. Wilkinson , M. P. Williams , M. Williams , H. W. Wilschut , F. F. Wilson , J. Wimberley , J. Wishahi , W. Wislicki , M. Witek , G. Wormser , S. A. Wotton , S. Wright , K. Wyllie , Y. Xie , Z. Xing , Z. Xu , Z. Yang , X. Yuan , O. Yushchenko , M. Zangoli , M. Zavertyaev , L. Zhang , W. C. Zhang , Y. Zhang , A. Zhelezov , A. Zhokhov , L. Zhong

The pseudo-scalar flavor-singlet meson mixes with two gluons. A dimensional argument by Kogut and Susskind shows that this can screen the Goldstone pole of the chiral limit in this channel, if the gluon correlations are infrared enhanced.…

High Energy Physics - Phenomenology · Physics 2009-10-30 Lorenz von Smekal , Almut Mecke , Reinhard Alkofer