K0SK0S final state in two-photon collisions and implications for glueballs

Acciarri, M.; Achard, P.; Адриани, О.; 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.; Burger, J. D.; Burger, W. J.; Cai, X.; 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, Yiming; 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, Christian; 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, B. C.; 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.; 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.; 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)00116-2

Cited by 50 publications

(36 citation statements)

References 33 publications

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“…2 we list the variation of the total and partial decay widths of a 2 (1700) in terms of the R value. When R = 4.35 GeV −1 [33], the central value of the experimental total width of a 2 (1700) from L3 [56] can be reproduced by our calculation. The main decay modes of a 2 (1700) include πρ, ρω, πη, and πb 1 (1235).…”

Section: Phenomenological Analysis Of Two-body Decayssupporting

confidence: 52%

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Phenomenological study of the isovector tensor meson family

Pang

Liu

et al. 2014

Phys. Rev. D

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In this work, we study all the observed a 2 states and group them into the a 2 meson family, where their total and two-body Okubo-Zweig-Iizuka allowed strong decay partial widths are calculated via the quark pair creation model. Taking into account the present experimental data, we further give the corresponding phenomenological analysis, which is valuable to test whether each a 2 state can be assigned into the a 2 meson family. What is more important is that the prediction of their decay behaviors will be helpful for future experimental study of the a 2 states.

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Section: Phenomenological Analysis Of Two-body Decayssupporting

confidence: 52%

“…Here, the dashed line with the yellow band denotes the experimental total width given in Ref. [56]. All results are in units of MeV.…”

Section: R Gevmentioning

confidence: 99%

Phenomenological study of the isovector tensor meson family

Pang

Liu

et al. 2014

Phys. Rev. D

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“…The f 0 (1500) has not been measured either in γγ → K S K S by L3 Collaboration [26] or in γγ → π + π − by ALEPH Collaboration [27], implying that this state, if quarkonium, should be dominantly ss. However, the branching ratios for the decay into two pseudoscalar mesons are only compatible with an almost pure nn structure.…”

Section: B Including Four-quark Statesmentioning

confidence: 99%

The nature of the light scalar mesons

Vijande¹,

Valcarce²,

Fernández³

2005

AIP Conference Proceedings

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Despite the apparent simplicity of meson spectroscopy, light scalar mesons cannot be accommodated in the usual qq structure. We study the description of the scalar mesons below 2 GeV in terms of the mixing of a chiral nonet of tetraquarks with conventional qq states. A strong diquark-antidiquark component is found for several states. The consideration of a glueball as dictated by quenched lattice QCD drives a coherent picture of the isoscalar mesons.Pacs: 12.39.-x,12.38.-t 1

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“…Structures in the K 0 S K 0 S mass spectrum have also been observed in two-photon [22] and electronproton collisions [23].…”

mentioning

confidence: 99%