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A Triangle Singularity as the Origin of the $a_1(1420)$
The COMPASS experiment recently discovered a new isovector resonance-like 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 e...
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Lenguaje: | eng |
Publicado: |
2020
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevLett.127.082501 http://cds.cern.ch/record/2719624 |
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author | 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. 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. |
author_facet | 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. 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. |
author_sort | Alexeev, G.D. |
collection | CERN |
description | The COMPASS experiment recently discovered a new isovector resonance-like 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 resonance-like signal fully matching the experimental data is produced by the decay of the $a_1(1260)$ ground state into $K^\ast(K\pi)\bar{K}$ and subsequent rescattering through a triangle singularity into the coupled $f_0(980)\pi$ channel. The amplitude for this process is calculated using a novel method based on partial-wave projections. For the first time, the triangle singularity model is fitted to the partial-wave data of the COMPASS experiment. Despite having less 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 that a resonance-like structure in the experimental data can be described by rescattering through a triangle singularity, providing evidence for a genuine three-body effect. |
id | cern-2719624 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2020 |
record_format | invenio |
spelling | cern-27196242023-10-26T06:57:51Zdoi:10.1103/PhysRevLett.127.082501doi:10.1103/PhysRevLett.127.082501http://cds.cern.ch/record/2719624engAlexeev, 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.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.A Triangle Singularity as the Origin of the $a_1(1420)$Particle Physics - ExperimentThe COMPASS experiment recently discovered a new isovector resonance-like 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 resonance-like signal fully matching the experimental data is produced by the decay of the $a_1(1260)$ ground state into $K^\ast(K\pi)\bar{K}$ and subsequent rescattering through a triangle singularity into the coupled $f_0(980)\pi$ channel. The amplitude for this process is calculated using a novel method based on partial-wave projections. For the first time, the triangle singularity model is fitted to the partial-wave data of the COMPASS experiment. Despite having less 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 that a resonance-like structure in the experimental data can be described by rescattering through a triangle singularity, providing evidence for a genuine three-body effect.The COMPASS Collaboration experiment recently discovered a new isovector resonancelike signal with axial-vector quantum numbers, the <math display="inline"><mrow><msub><mrow><mi>a</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy="false">(</mo><mn>1420</mn><mo stretchy="false">)</mo></mrow></math>, decaying to <math display="inline"><mrow><msub><mrow><mi>f</mi></mrow><mrow><mn>0</mn></mrow></msub><mo stretchy="false">(</mo><mn>980</mn><mo stretchy="false">)</mo><mi>π</mi></mrow></math>. With a mass too close to and a width smaller than the axial-vector ground state <math display="inline"><mrow><msub><mrow><mi>a</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy="false">(</mo><mn>1260</mn><mo stretchy="false">)</mo></mrow></math>, it was immediately interpreted as a new light exotic meson, similar to the <math display="inline"><mi>X</mi></math>, <math display="inline"><mi>Y</mi></math>, <math display="inline"><mi>Z</mi></math> states in the hidden-charm sector. We show that a resonancelike signal fully matching the experimental data is produced by the decay of the <math display="inline"><mrow><msub><mrow><mi>a</mi></mrow><mrow><mn>1</mn></mrow></msub><mo stretchy="false">(</mo><mn>1260</mn><mo stretchy="false">)</mo></mrow></math> resonance into <math display="inline"><mrow><msup><mrow><mi>K</mi></mrow><mrow><mo>*</mo></mrow></msup><mo stretchy="false">(</mo><mo stretchy="false">→</mo><mi>K</mi><mi>π</mi><mo stretchy="false">)</mo><mover accent="true"><mrow><mi>K</mi></mrow><mrow><mo stretchy="false">¯</mo></mrow></mover></mrow></math> and subsequent rescattering through a triangle singularity into the coupled <math display="inline"><msub><mi>f</mi><mn>0</mn></msub><mo stretchy="false">(</mo><mn>980</mn><mo stretchy="false">)</mo><mi>π</mi></math> 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 light-meson 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.The COMPASS experiment recently discovered a new isovector resonance-like 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 resonance-like signal fully matching the experimental data is produced by the decay of the $a_1(1260)$ resonance into $K^\ast(\to K\pi)\bar{K}$ and subsequent rescattering through a triangle singularity into the coupled $f_0(980)\pi$ 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 less 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 light-meson sector that a resonance-like structure in the experimental data can be described by rescattering through a triangle singularity, providing evidence for a genuine three-body effect.arXiv:2006.05342CERN-EP-2020-104oai:cds.cern.ch:27196242020-06-09 |
spellingShingle | Particle Physics - Experiment 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. 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. A Triangle Singularity as the Origin of the $a_1(1420)$ |
title | A Triangle Singularity as the Origin of the $a_1(1420)$ |
title_full | A Triangle Singularity as the Origin of the $a_1(1420)$ |
title_fullStr | A Triangle Singularity as the Origin of the $a_1(1420)$ |
title_full_unstemmed | A Triangle Singularity as the Origin of the $a_1(1420)$ |
title_short | A Triangle Singularity as the Origin of the $a_1(1420)$ |
title_sort | triangle singularity as the origin of the $a_1(1420)$ |
topic | Particle Physics - Experiment |
url | https://dx.doi.org/10.1103/PhysRevLett.127.082501 https://dx.doi.org/10.1103/PhysRevLett.127.082501 http://cds.cern.ch/record/2719624 |
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