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Observation of a new narrow axial-vector meson a₁(1420)

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arxiv 1501.05732 v3 pith:YI5PE3MV submitted 2015-01-23 hep-ex

Observation of a new narrow axial-vector meson a₁(1420)

C. Adolph , R. Akhunzyanov , M.G. Alexeev , G.D. Alexeev , A. Amoroso , V. Andrieux , V. Anosov , A. Austregesilo
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C. Azevedo B. Badelek F. Balestra J. Barth R. Beck Y. Bedfer J. Bernhard K. Bicker E. R. Bielert R. Birsa J. Bisplinghoff M. Bodlak M. Boer P. Bordalo F. Bradamante C. Braun A. Bressan M. Buechele E. Burtin W.-C. Chang M. Chiosso I. Choi S.U. Chung A. Cicuttin M.L. Crespo Q. Curiel S. Dalla Torre S.S. Dasgupta S. Dasgupta O.Yu. Denisov L. Dhara S.V. Donskov N. Doshita W Duennweber V. Duic M. Dziewiecki A. Efremov P.D. Eversheim W. Eyrich M. Faessler A. Ferrero M. Finger M. Finger jr. H. Fischer C. Franco N. du Fresne von Hohenesche J.M. Friedrich V. Frolov F. Gautheron O.P. Gavrichtchouk S. Gerassimov I. Gnesi M. Gorzellik S. Grabmueller A. Grasso M. Grosse-Perdekamp B. Grube T. Grussenmeyer A. Guskov F. Haas D. Hahne D. von Harrach R. Hashimoto F.H. Heinsius F. Herrmann F. Hinterberger N. Horikawa N. d'Hose C.-Yu Hsieh S. Huber S. Ishimoto A. Ivanov Yu. Ivanshin T. Iwata R. Jahn V. Jary P. Joerg R. Joosten E. Kabuss B. Ketzer G.V. Khaustov Yu.A. Khokhlov Yu. Kisselev F. Klein K. Klimaszewski J.H. Koivuniemi V.N. Kolosov K. Kondo K. Koenigsmann I. Konorov V.F. Konstantinov A.M. Kotzinian O. Kouznetsov M. Kraemer P. Kremser F. Krinner Z.V. Kroumchtein N. Kuchinski F. Kunne K. Kurek R.P. Kurjata A.A. Lednev A. Lehmann M. Levillain S. Levorato J. Lichtenstadt A. Maggiora A. Magnon N. Makins N. Makke G.K. Mallot C. Marchand A. Martin J. Marzec J. Matousek H. Matsuda T. Matsuda G. Meshcheryakov W. Meyer T. Michigami Yu.V. Mikhailov Y. Miyachi A. Nagaytsev T. Nagel F. Nerling D. Neyret V.I. Nikolaenko J. Novy W.-D. Nowak A.S. Nunes A.G. Olshevsky I. Orlov M. Ostrick D. Panzieri B. Parsamyan S. Paul J.-C. Peng F. Pereira M. Pesek D.V. Peshekhonov S. Platchkov J. Pochodzalla V.A. Polyakov J. Pretz M. Quaresma C. Quintans S. Ramos C. Regali G. Reicherz C. Riedl E. Rocco N.S. Rossiyskaya D.I. Ryabchikov A. Rychter V.D. Samoylenko A. Sandacz C. Santos S. Sarkar I.A. Savin G. Sbrizzai P. Schiavon K. Schmidt H. Schmieden K. Schoenning S. Schopferer T. Schlueter A. Selyunin O.Yu. Shevchenko L. Silva L. Sinha S. Sirtl M. Slunecka F. Sozzi A. Srnka M. Stolarski M. Sulc H. Suzuki A. Szabelski T. Szameitat P. Sznajder S. Takekawa J. ter Wolbeek S. Tessaro F. Tessarotto F. Thibaud V. Tskhay S. Uhl J. Veloso M. Virius S. Wallner T. Weisrock M. Wilfert K. Zaremba M. Zavertyaev E. Zemlyanichkina M. Ziembicki A. Zink
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classification hep-ex
keywords decayinganalysisfinalmassmesonmodelnarrowstates
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The COMPASS collaboration at CERN has measured diffractive dissociation of 190 GeV/$c$ pions into the $\pi^-\pi^-\pi^+$ final state using a stationary hydrogen target. A partial-wave analysis (PWA) was performed in bins of $3\pi$ mass and four-momentum transfer using the isobar model and the so far largest PWA model consisting of 88 waves. A narrow $J^{PC} = 1^{++}$ signal is observed in the $f_0(980)\,\pi$ channel. We present a resonance-model study of a subset of the spin-density matrix selecting $3\pi$ states with $J^{PC} = 2^{++}$ and $4^{++}$ decaying into $\rho(770)\,\pi$ and with $J^{PC} = 1^{++}$ decaying into $f_0(980)\,\pi$. We identify a new $a_1$ meson with mass $(1414^{+15}_{-13})$ MeV/$c^2$ and width $(153^{+8}_{-23})$ MeV/$c^2$. Within the final states investigated in our analysis, we observe the new $a_1(1420)$ decaying only into $f_0(980)\,\pi$, suggesting its exotic nature.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. The $a_1(1420)$ in a Unitary Coupled-Channel Three-Body Approach

    hep-ph 2026-06 conditional novelty 6.5

    Nine-channel unitary three-body fits to COMPASS lineshapes reproduce the a1(1420) enhancement by triangle singularity without requiring a genuine a1(1420) pole.

  2. The $a_1(1420)$ in a Unitary Coupled-Channel Three-Body Approach

    hep-ph 2026-06 unverdicted novelty 5.0

    Unitary coupled-channel three-body model fitted to COMPASS data reproduces the a1(1420) enhancement via triangle singularity, indicating no genuine resonance pole is required.

  3. Effects of Final State Interactions on Landau Singularities

    hep-ph 2024-07 unverdicted novelty 5.0

    Triangle singularities mimicking resonances are analyzed in the presence of final-state rescattering using Landau equations and a scattering formalism enforcing two- and three-body unitarity.