The COMPASS Collaboration experiment recently discovered a new isovector resonancelike signal with axial-vector quantum numbers, the a(1)(1420), decaying to f(0)(980)(pi). With a mass too close to and a width smaller than the axial-vector ground state a(1)(1260), it was immediately interpreted as a new light exotic meson, similar to the X, Y, Z states in the hidden-charm sector. We show that a resonancelike signal fully matching the experimental data is produced by the decay of the a(1) (1260) resonance into K* (-> K pi) (K) over bar and subsequent rescattering through a triangle singularity into the coupled f(0)(980)p channel. The amplitude for this process is calculated using a new approach based on dispersion relations. The triangle-singularity model is fitted to the partial-wave data of the COMPASS experiment. Despite having fewer parameters, this fit shows a slightly better quality than the one using a resonance hypothesis and thus eliminates the need for an additional resonance in order to describe the data. We thereby demonstrate for the first time in the lightmeson sector that a resonancelike structure in the experimental data can be described by rescattering through a triangle singularity, providing evidence for a genuine three-body effect.

Triangle Singularity as the Origin of the a_{1}(1420)

Alexeev, M G;Amoroso, A;Balestra, F;Chiosso, M;Frolov, V;Grasso, A;Ivanov, A;Kotzinian, A M;Panzieri, D;Parsamyan, B;
2021-01-01

Abstract

The COMPASS Collaboration experiment recently discovered a new isovector resonancelike signal with axial-vector quantum numbers, the a(1)(1420), decaying to f(0)(980)(pi). With a mass too close to and a width smaller than the axial-vector ground state a(1)(1260), it was immediately interpreted as a new light exotic meson, similar to the X, Y, Z states in the hidden-charm sector. We show that a resonancelike signal fully matching the experimental data is produced by the decay of the a(1) (1260) resonance into K* (-> K pi) (K) over bar and subsequent rescattering through a triangle singularity into the coupled f(0)(980)p channel. The amplitude for this process is calculated using a new approach based on dispersion relations. The triangle-singularity model is fitted to the partial-wave data of the COMPASS experiment. Despite having fewer parameters, this fit shows a slightly better quality than the one using a resonance hypothesis and thus eliminates the need for an additional resonance in order to describe the data. We thereby demonstrate for the first time in the lightmeson sector that a resonancelike structure in the experimental data can be described by rescattering through a triangle singularity, providing evidence for a genuine three-body effect.
2021
127
8
1
7
https://journals.aps.org/prl/pdf/10.1103/PhysRevLett.127.082501
Alexeev, G D; Alexeev, M G; Amoroso, A; Andrieux, V; Anosov, V; Antoshkin, A; Augsten, K; Augustyniak, W; Azevedo, C D R; Badełek, B; Balestra, F; Ball, M; Barth, J; Beck, R; Bedfer, Y; Berenguer Antequera, J; Bernhard, J; Bodlak, M; Bradamante, F; Bressan, A; Burtsev, V E; Chang, W-C; Chatterjee, C; Chiosso, M; Chumakov, A G; Chung, S-U; Cicuttin, A; Correia, P M M; Crespo, M L; D'Ago, D; Dalla Torre, S; Dasgupta, S S; Dasgupta, S; Denisenko, I; Denisov, O Yu; Donskov, S V; Doshita, N; Dreisbach, Ch; Dünnweber, W; Dusaev, R R; Efremov, A; Eversheim, P D; Faccioli, P; Faessler, M; Finger, M; Finger, M; Fischer, H; Franco, C; Friedrich, J M; Frolov, V; Gautheron, F; Gavrichtchouk, O P; Gerassimov, S; Giarra, J; Gnesi, I; Gorzellik, M; Grasso, A; Gridin, A; Grosse Perdekamp, M; Grube, B; Guskov, A; von Harrach, D; Heitz, R; Herrmann, F; Horikawa, N; d'Hose, N; Hsieh, C-Y; Huber, S; Ishimoto, S; Ivanov, A; Iwata, T; Jandek, M; Jary, V; Joosten, R; Jörg, P; Kabuß, E; Kaspar, F; Kerbizi, A; Ketzer, B; Khaustov, G V; Khokhlov, Yu A; Kisselev, Yu; Klein, F; Koivuniemi, J H; Kolosov, V N; Kondo Horikawa, K; Konorov, I; Konstantinov, V F; Kotzinian, A M; Kouznetsov, O M; Koval, A; Kral, Z; Krinner, F; Kulinich, Y; Kunne, F; Kurek, K; Kurjata, R P; Kveton, A; Lavickova, K; Levorato, S; Lian, Y-S; Lichtenstadt, J; Lin, P-J; Longo, R; Lyubovitskij, V E; Maggiora, A; Magnon, A; Makins, N; Makke, N; Mallot, G K; Maltsev, A; Mamon, S A; Marianski, B; Martin, A; Marzec, J; Matoušek, J; Matsuda, T; Mattson, G; Meshcheryakov, G V; Meyer, M; Meyer, W; Mikhailov, Yu V; Mikhasenko, M; Mitrofanov, E; Mitrofanov, N; Miyachi, Y; Moretti, A; Nagaytsev, A; Naim, C; Neyret, D; Nový, J; Nowak, W-D; Nukazuka, G; Nunes, A S; Olshevsky, A G; Ostrick, M; Panzieri, D; Parsamyan, B; Paul, S; Pekeler, H; Peng, J-C; Pešek, M; Peshekhonov, D V; Pešková, M; Pierre, N; Platchkov, S; Pochodzalla, J; Polyakov, V A; Pretz, J; Quaresma, M; Quintans, C; Reicherz, G; Riedl, C; Rudnicki, T; Ryabchikov, D I; Rybnikov, A; Rychter, A; Samoylenko, V D; Sandacz, A; Sarkar, S; Savin, I A; Sbrizzai, G; Schmieden, H; Selyunin, A; Sinha, L; Slunecka, M; Smolik, J; Srnka, A; Steffen, D; Stolarski, M; Subrt, O; Sulc, M; Suzuki, H; Sznajder, P; Tessaro, S; Tessarotto, F; Thiel, A; Tomsa, J; Tosello, F; Townsend, A; Tskhay, V; Uhl, S; Vasilishin, B I; Vauth, A; Veit, B M; Veloso, J; Ventura, B; Vidon, A; Virius, M; Wagner, M; Wallner, S; Zaremba, K; Zavada, P; Zavertyaev, M; Zemko, M; Zemlyanichkina, E; Zhao, Y; Ziembicki, M
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/1893494
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