Light resonances in K0SK±π∓ and ηπ+π− final states in γγ collisions at LEP

Acciarri, M.; Achard, P.; Adriani, O.; Aguilar-Benı́tez, M.; Alcaraz, J.; Alemanni, G.; Allaby, J.; Aloisio, A.; Alviggi, M. G.; Ambrosi, G.; Anderhub, H.; Andreev, V.; Angelescu, T.; Anselmo, F.; Arefiev, A.; Azemoon, T.; Aziz, T.; Bagnaia, P.; Bajo, A.; Baksay, L.; Balandras, A.; Baldew, S.V.; Banerjee, S.; Barczyk, A.; Barillère, R.; 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, B.L.; Bhattacharya, S.; Biasini, M.; Biland, A.; Blaising, J. J.; Blyth, S.; Bobbink, G. J.; Böhm, A.; Boldizsár, L.; Borgia, B.; Bourilkov, D.; Bourquin, M.; Braccini, S.; Branson, J. G.; Brochu, F. M.; Buffini, A.; Buijs, A.; Bürger, J.; Burger, W. J.; Cai, X. D.; Capell, M.; Romeo, G. Cara; Carlino, G.; Cartacci, A. M.; Casaus, J.; Castellini, G.; Cavallari, F.; Cavallo, N.; Cecchi, C.; Cerrada, M.; Cesaroni, F.; Chamizo, M.; Chang, Y. H.; Chaturvedi, U. K.; Chemarin, M.; Chen, A.; Chen, G.; Chen, G. M.; Chen, H. F.; Chen, H. S.; Chiefari, G.; Cifarelli, L.; Cindolo, F.; Civinini, C.; Clare, I.; Clare, R.; Coignet, G.; Colino, N.; Costantini, S.; Cotorobai, F.; Cruz, B. De La; Csilling, Á.; Cucciarelli, S.; Dai, T.; Dalen, J. A. van; D’Alessandro, R.; Asmundis, R. de; Déglon, P.; Degré, A.; Deiters, K.; Volpe, D. della; Delmeire, E.; Denes, P.; DeNotaristefani, F.; Salvo, A. De; Diemoz, M.; Dierckxsens, M.; Dierendonck, D. van; Dionisi, C.; Dittmar, M.; Dominguez, A.; Doria, A.; Dova, M. T.; Duchesneau, D.; Dufournaud, D.; Duinker, P.; Durán, I.; Mamouni, H. El; Engler, A.; Eppling, F. J.; Erné, F.C.; Extermann, P.; Fabre, Michel; Falagán, M. A.; Falciano, S.; Favara, A.; Fay, J.; Fedin, O. L.; Felcini, M.; Ferguson, T.; Fesefeldt, H.; Fiandrini, E.; Field, J. H.; Filthaut, F.; Fisher, P. H.; Fisk, I.; Forconì, G.; Freudenreich, K.; Furetta, C.; Galaktionov, Yu.; Ganguli, S. N.; Garcı́a-Abia, P.; Gataullin, M.; Gau, S. S.; Gentile, S.; Gheordanescu, N.; Giagu, S.; Gong, Z. F.; Grenier, G.; Grimm, O.; Gruenewald, M. W.; Guida, M.; Gulik, R. van; Gupta, V. K.; Gurtu, A.; Gutay, L.; Haas, D.; Hasan, A.; Hatzifotiadou, D.; Hebbeker, T.; Hervé, A.; Hidas, P.; Hirschfelder, J.; Hofer, H.; Holzner, G.; Hoorani, H. R.; Hou, S.; Hu, Y.; Iashvili, I.; Jin, B. N.; Jones, L. W.; Jong, P. de; Josa-Mutuberrı́a, I.; Khan, R. A.; Kaur, M.; Kienzle‐Focacci, M. N.; Kim, D.; Kim, J. K.; Kirkby, J.; Kiss, D.; Kittel, W.; Klimentov, A.; König, A. C.; Kopál, M.; Kopp, A. K.; Koutsenko, V.; Kräber, M.; Kraemer, R. W.; Krenz, W.; Krüger, A.; Kunin, A.; Guevara, P. Ladrón de; Laktineh, I. B.; Landi, G.; Lebeau, M.; Lebedev, A.; Lebrun, P.; Lecomte, P.; Lecoq, P.; Coultre, P. Le; Lee, H. J.; Goff, J. M. Le; Leiste, R.; Levtchenko, P.; Li, C.; Likhoded, S.; Lin, C. H.; Lin, W.; Linde, F.L.; Lista, L.; Liu, Z. A.; Lohmann, W.; Longo, E.; Lu, Y. S.; Lübelsmeyer, K.; Luci, C.; Luckey, D.; Lugnier, L.; Luminari, L.; Lustermann, W.; G., W.; Maity, M.; Malgeri, L.; Малинин, А.; Mañá, C.; Mangeol, D.; Mans, J.; Marian, G.; Martin, J. P.; Marzano, F.; Mazumdar, K.; McNeil, R. R.; Mele, S.; Merola, L.; Meschini, M.; Metzger, W. J.; Mey, M. von der; Mihul, A.; Milcent, H.; Mirabelli, G.; Mnich, J.; Mohanty, G. B.; Moulik, T.; Muanza, G. S.; Muijs, A. J.M.; Musicar, B.; Musy, M.; Napolitano, M.; Nessi‐Tedaldi, F.; Newman, H. B.; Nießen, T.; Nisati, A.; Nowak, H.; Ofierzynski, R. A.; Organtini, G.; Oulianov, A.; Palomares, C.; Pandoulas, D.; Paoletti, S.; Paolucci, P.; Paramatti, R.; Park, H. K.; Park, I. H.; Passaleva, G.; Patricelli, S.; Paul, T.; Pauluzzi, M.; Paus, C.; Pauß, F.; Pedace, M.; Pensotti, S.; Perret-Gallix, D.; Petersen, B. A.; Piccolo, D.; Pierella, F.; Pieri, M.; Piroué, P.; Pistolesi, E.; Plyaskin, V.; Pohl, M.; Pojidaev, V.; Postema, H.; Pothier, J.; Prokofiev, D.; Quartieri, J.; Rahal-Callot, G.; Rahaman, M. A.; Raics, P.; Raja, N.; Ramelli, R.; Rancoita, P.G.; Ranieri, R.; Raspereza, A.; Raven, G.; Razis, P. A.; Ren, D.; Rescigno, M.; Reucroft, S.; Riemann, S.; Riles, K.; Rodin, J.; Roe, B. P.; Romero, L.; Rosca, A.; Rosier‐Lees, S.; Rubio, J. A.; Ruggiero, G.; Rykaczewski, H.; Saremi, S.; Sarkar, S.; Salicio, J.; Sánchez, E.; Sanders, M. P.; Schäfer, C.; Schegelsky, V. A.; Schmidt-Kaerst, S.; Schmitz, D.; Schopper, H.; Schotanus, D. J.; Schwering, G.; Sciacca, C.; Seganti, A.; Servoli, L.; Shevchenko, S.; Shivarov, N.; Shoutko, V.; Shumilov, E.; Shvorob, A.; Siedenburg, T.; Son, D.; Smith, Bryan; Спиллантини, П.; Steuer, M.; Stickland, D.; Stone, A.; Stoyanov, B.; Straessner, A.; Sudhakar, K.; Sultanov, G.; Sun, L. Z.; Sushkov, S.; Suter, H.; Swain, J. D.; Szillási, Z.; Sztaricskai, T.; Tang, X. W.; Tauscher, L.; Taylor, L.; Tellili, B.; Timmermans, C.; Ting, Samuel C.C.; Ting, S. M.; Tonwar, S. C.; Töth, J.; Tully, C.; Tung, K. L.; Uchida, Y.; Ulbricht, J.; Valente, E.; Vesztergombi, G.; Vetlitsky, I.; Vicinanza, D.; Viertel, G.; Villa, S.; Vivargent, M.; Vlachos, S.; Vodopianov, I.; Vogel, H.; Vogt, H.; Vorobiev, I.; Vorobyov, A. A.; Vorvolakos, A.; Wadhwa, M.; Wallraff, W.; Wang, M.; Wang, X. L.; Wang, Z. M.; Weber, A.; Weber, Martin; Wienemann, P.; Wilkens, H. G.; Wu, S. X.; Wynhoff, S.; Xia, L.; Xu, Z. Z.; Yamamoto, J.; Yang, B. Z.; Yang, C. G.; Yang, H. J.; Yang, Min; Ye, J. B.; Yeh, S. C.; Zalite, A.; Zalite, Yu; Zhang, Z. P.; Zhu, G. Y.; Zhu, R. Y.; Zichichi, A.; Zilizi, G.; Zimmermann, B.; Zöller, Margot

doi:10.1016/s0370-2693(01)00102-2

Cited by 50 publications

(41 citation statements)

References 31 publications

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“…4 166 ± 22 1.283 ± 0.004 3.13 ± 0.20 ± 0.16 57.7 ± 7.6 ± 5.3 ± 4.9 0.4-0.9 9 1 ± 15 1.287 ± 0.004 3.35 ± 0.29 ± 0.25 29.8 ± 4.7 ± 3.8 ± 2.5 0.9-6.0 8 4 ± 11 1.272 ± 0.004 3.30 ± 0.31 ± 0.38 28.2 ± 3.8 ± 4.3 ± 2.4 Fig. 2.…”

Section: F 1 (1285) Formationmentioning

confidence: 99%

“…The TPC/Two-Gamma and Mark II Collaborations observed the axial vector meson (J PC = 1 ++ ) f 1 (1285) in single-tag events [2,3]. We previously reported an indication of the formation of f 1 (1285) in untagged events at LEP [4]. The f 1 (1285) decay into ηππ is dominated by the two-body decay f 1 (1285) → a 0 (980)π [5].…”

Section: Introductionmentioning

confidence: 99%

“…3 Also supported by the Hungarian OTKA fund under contract number T026178. 4 Supported also by the Comisión Interministerial de Ciencia y Tecnología. 5 Also supported by CONICET and Universidad Nacional de La Plata, CC 67, 1900 La Plata, Argentina.…”

Section: Introductionmentioning

confidence: 99%

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f1(1285) formation in two-photon collisions at LEP

et al. 2002

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Section: F 1 (1285) Formationmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

See 1 more Smart Citation

f1(1285) formation in two-photon collisions at LEP

et al. 2002

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“…But then, η(1295) should also be produced, but it is not ! There is also no evidence for η(1295) from γγ fusion at LEP, nor from a study of γγ → K 0 s K ± π ∓ , but η(1440) is seen [3]. The η(1440) coupling to photons is much stronger than that of η(1295): the assumption that the η(1295) is a (uū + dd) radial excitation must be wrong !…”

Section: Search For the Pseudoscalar Glueballmentioning

confidence: 99%

Hadron Spectroscopy Without Constituent Glue

Klempt

2005

Int. J. Mod. Phys. A

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Glueballs and hybrids are predicted to exist but searches for them have failed to provide conclusive evidence. One-gluon exchange is not an important part of strong interactions in this energy regime. Instead, quarks seem to interact indirectly, via changes of the QCD vacuum. Strong interactions seem to be governed by instanton-induced interactions; the chiral soliton model gives a more suitable interpretation of the Θ + (1540) than models based on the dynamics of four quarks and one antiquark.

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“…The η(1475) could be the first radial excitation of η ′ (958). The L3 measurements of the KKπ and ηπ + π − decays in photon-photon fusion suggest that the η(1405) has a large gluonic content [15]. However, CLEO with a five times larger data sample did not confirm the L3 results, but their upper limits are still consistent with the glueball and the radial excitation hypotheses for the η(1405) and η(1475) [16].…”

Section: Introductionmentioning

confidence: 99%

Study ofψ(3686)→ωKK¯πdecays

Ablikim¹,

Ачасов²,

Albayrak³

et al. 2013

Phys. Rev. D

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Based on 106 million ψ(3686) events collected with the BESIII detector at the BEPCII, the decay ψ(3686) → ωKKπ is studied. Enhancements around 1.44 GeV/c 2 and the f1(1285) are observed in the mass spectrum of KKπ, and the corresponding branching fraction (upper limit) is measured, as well as the branching fractions of ψ(3686) → ωK * + K − + c.c. and ψ(3686) → ωK * 0 K 0 + c.c., all for the first time.

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Light resonances in K0SK±π∓ and ηπ+π− final states in γγ collisions at LEP

Cited by 50 publications

References 31 publications

f1(1285) formation in two-photon collisions at LEP

f1(1285) formation in two-photon collisions at LEP

Hadron Spectroscopy Without Constituent Glue

Study ofψ(3686)→ωKK¯πdecays

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