Exotic meson π1(1600) with JPC=1−+ and its decay into ρ(770)π; Physical Review D; Vol. 105, iss. 1

Bibliografiske detaljer
Parent link:Physical Review D: particles, fields, gravitation, and cosmology
Vol. 105, iss. 1.— 2022.— [012005, 30 p.]
Corporate Authors: Национальный исследовательский Томский политехнический университет Исследовательская школа физики высокоэнергетических процессов, Национальный исследовательский Томский политехнический университет Школа базовой инженерной подготовки Отделение математики и информатики
Andre forfattere: Alekseev G. D. Gennady Dmitrievich, Alekseev M. G. Maksim Gennadjevich, Amoroso A., Burtsev V. E. Vitaly Evgenjevich, Chumakov A. G. Aleksandr Grigorjevich, Dusaev R. R. Renat Ramilyevich, Lyubovitskiy (Lyubovitskij) V. E. Valery Efimovich, Mamon S. A. Sergey Aleksandrovich, Sharko K. A. Konstantin Andreevich
Summary:Title screen
We study the spin-exotic JPC=1−+ amplitude in single-diffractive dissociation of 190  GeV/c pions into π−π−π+ using a hydrogen target and confirm the π1(1600)→ρ(770)π amplitude, which interferes with a nonresonant 1−+ amplitude. We demonstrate that conflicting conclusions from previous studies on these amplitudes can be attributed to different analysis models and different treatment of the dependence of the amplitudes on the squared four-momentum transfer and we thus reconcile these experimental findings. We study the nonresonant contributions to the π−π−π+ final state using pseudodata generated on the basis of a Deck model. Subjecting pseudodata and real data to the same partial-wave analysis, we find good agreement concerning the spectral shape and its dependence on the squared four-momentum transfer for the JPC=1−+ amplitude and also for amplitudes with other JPC quantum numbers. We investigate for the first time the amplitude of the π−π+ subsystem with JPC=1−− in the 3π amplitude with JPC=1−+ employing the novel freed-isobar analysis scheme. We reveal this π−π+ amplitude to be dominated by the ρ(770) for both the π1(1600) and the nonresonant contribution. These findings largely confirm the underlying assumptions for the isobar model used in all previous partial-wave analyses addressing the JPC=1−+ amplitude.
Sprog:engelsk
Udgivet: 2022
Fag:
Online adgang:https://doi.org/10.1103/PhysRevD.105.012005
Format: Electronisk Book Chapter
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=669454

MARC

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200 1 |a Exotic meson π1(1600) with JPC=1−+ and its decay into ρ(770)π  |f G. D. Alekseev, M. G. Alekseev, A. Amoroso [et al.] 
203 |a Text  |c electronic 
300 |a Title screen 
320 |a [References.: 75 tit.] 
330 |a We study the spin-exotic JPC=1−+ amplitude in single-diffractive dissociation of 190  GeV/c pions into π−π−π+ using a hydrogen target and confirm the π1(1600)→ρ(770)π amplitude, which interferes with a nonresonant 1−+ amplitude. We demonstrate that conflicting conclusions from previous studies on these amplitudes can be attributed to different analysis models and different treatment of the dependence of the amplitudes on the squared four-momentum transfer and we thus reconcile these experimental findings. We study the nonresonant contributions to the π−π−π+ final state using pseudodata generated on the basis of a Deck model. Subjecting pseudodata and real data to the same partial-wave analysis, we find good agreement concerning the spectral shape and its dependence on the squared four-momentum transfer for the JPC=1−+ amplitude and also for amplitudes with other JPC quantum numbers. We investigate for the first time the amplitude of the π−π+ subsystem with JPC=1−− in the 3π amplitude with JPC=1−+ employing the novel freed-isobar analysis scheme. We reveal this π−π+ amplitude to be dominated by the ρ(770) for both the π1(1600) and the nonresonant contribution. These findings largely confirm the underlying assumptions for the isobar model used in all previous partial-wave analyses addressing the JPC=1−+ amplitude. 
461 |t Physical Review D  |o particles, fields, gravitation, and cosmology 
463 |t Vol. 105, iss. 1  |v [012005, 30 p.]  |d 2022 
610 1 |a электронный ресурс 
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701 1 |a Alekseev  |b G. D.  |g Gennady Dmitrievich 
701 1 |a Alekseev  |b M. G.  |g Maksim Gennadjevich 
701 1 |a Amoroso  |b A. 
701 1 |a Burtsev  |b V. E.  |c mathematician  |c Senior Lecturer of Tomsk Polytechnic University  |f 1991-  |g Vitaly Evgenjevich  |3 (RuTPU)RU\TPU\pers\38282 
701 1 |a Chumakov  |b A. G.  |c physicist  |c laboratory assistant-researcher of Tomsk Polytechnic University  |f 1992-  |g Aleksandr Grigorjevich  |3 (RuTPU)RU\TPU\pers\41079 
701 1 |a Dusaev  |b R. R.  |c specialist in the field of nuclear physics  |c Engineer of Tomsk Polytechnic University  |f 1988-  |g Renat Ramilyevich  |3 (RuTPU)RU\TPU\pers\30972  |9 15210 
701 1 |a Lyubovitskiy (Lyubovitskij)  |b V. E.  |c physicist  |c Professor of Tomsk Polytechnic University, Doctor of physical and mathematical sciences, Professor of the University of Tubingen (Germany)  |f 1963-  |g Valery Efimovich  |3 (RuTPU)RU\TPU\pers\33385  |9 17080 
701 1 |a Mamon  |b S. A.  |c physicist  |c laboratory assistant-researcher of Tomsk Polytechnic University  |f 1989-  |g Sergey Aleksandrovich  |3 (RuTPU)RU\TPU\pers\43559 
701 1 |a Sharko  |b K. A.  |g Konstantin Andreevich 
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