Spin density matrix elements in exclusive ω meson muoproduction; European Physical Journal C; Vol. 81, iss. 2

Detalles Bibliográficos
Parent link:European Physical Journal C
Vol. 81, iss. 2.— 2021.— [126, 22 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
Outros autores: Alekseev G. D. Georgy Dmitrievich, Alekseev M. G. Maksim, Donskov S. V. Sergey Vasiljevich, 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, Vasilishin B. I. Bogdan Ivanovich
Summary:Title screen
We report on a measurement of Spin Density Matrix Elements (SDMEs) in hard exclusive ωω meson muoproduction on the proton at COMPASS using 160 GeV/c polarised μ+ and μ− beams impinging on a liquid hydrogen target. The measurement covers the range 5.0 GeV/c2 <W< 17.0 GeV/c2, with the average kinematics ⟨Q2⟩= 2.1 (GeV/c)2, ⟨W⟩=7.6⟨W⟩=7.6 GeV/c2, and ⟨p2T⟩=0.16 (GeV/c)2. Here, Q2 denotes the virtuality of the exchanged photon, W the mass of the final hadronic system and pT the transverse momentum of the ωω meson with respect to the virtual-photon direction. The measured non-zero SDMEs for the transitions of transversely polarised virtual photons to longitudinally polarised vector mesons (γ∗T→VL) indicate a violation of s-channel helicity conservation. Additionally, we observe a sizeable contribution of unnatural-parity-exchange (UPE) transitions that decreases with increasing W. The results provide important input for modelling Generalised Parton Distributions (GPDs). In particular, they may allow to evaluate in a model-dependent way the contribution of UPE transitions and assess the role of parton helicity-flip GPDs in exclusive ω production.
Idioma:inglés
Publicado: 2021
Subjects:
Acceso en liña:https://doi.org/10.1140/epjc/s10052-020-08740-y
Formato: Electrónico Capítulo de libro
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=668070

MARC

LEADER 00000naa0a2200000 4500
001 668070
005 20251106122907.0
035 |a (RuTPU)RU\TPU\network\39294 
035 |a RU\TPU\network\39293 
090 |a 668070 
100 |a 20220603d2021 k||y0rusy50 ba 
101 0 |a eng 
102 |a US 
135 |a drcn ---uucaa 
181 0 |a i  
182 0 |a b 
200 1 |a Spin density matrix elements in exclusive ω meson muoproduction  |f G. D. Alekseev, M. G. Alekseev, S. V. Donskov [et al.] 
203 |a Text  |c electronic 
300 |a Title screen 
320 |a [References: 30 tit.] 
330 |a We report on a measurement of Spin Density Matrix Elements (SDMEs) in hard exclusive ωω meson muoproduction on the proton at COMPASS using 160 GeV/c polarised μ+ and μ− beams impinging on a liquid hydrogen target. The measurement covers the range 5.0 GeV/c2 <W< 17.0 GeV/c2, with the average kinematics ⟨Q2⟩= 2.1 (GeV/c)2, ⟨W⟩=7.6⟨W⟩=7.6 GeV/c2, and ⟨p2T⟩=0.16 (GeV/c)2. Here, Q2 denotes the virtuality of the exchanged photon, W the mass of the final hadronic system and pT the transverse momentum of the ωω meson with respect to the virtual-photon direction. The measured non-zero SDMEs for the transitions of transversely polarised virtual photons to longitudinally polarised vector mesons (γ∗T→VL) indicate a violation of s-channel helicity conservation. Additionally, we observe a sizeable contribution of unnatural-parity-exchange (UPE) transitions that decreases with increasing W. The results provide important input for modelling Generalised Parton Distributions (GPDs). In particular, they may allow to evaluate in a model-dependent way the contribution of UPE transitions and assess the role of parton helicity-flip GPDs in exclusive ω production. 
461 |t European Physical Journal C 
463 |t Vol. 81, iss. 2  |v [126, 22 p.]  |d 2021 
610 1 |a электронный ресурс 
610 1 |a труды учёных ТПУ 
701 1 |a Alekseev  |b G. D.  |g Georgy Dmitrievich 
701 1 |a Alekseev  |b M. G.  |g Maksim 
701 1 |a Donskov  |b S. V.  |g Sergey Vasiljevich 
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 Vasilishin  |b B. I.  |c engineer-physicist  |c laboratory researcher at Tomsk Polytechnic University  |f 1990-  |g Bogdan Ivanovich  |3 (RuTPU)RU\TPU\pers\37572  |9 20428 
712 0 2 |a Национальный исследовательский Томский политехнический университет  |b Исследовательская школа физики высокоэнергетических процессов  |c (2017- )  |3 (RuTPU)RU\TPU\col\23551 
712 0 2 |a Национальный исследовательский Томский политехнический университет  |b Школа базовой инженерной подготовки  |b Отделение математики и информатики  |3 (RuTPU)RU\TPU\col\23555 
801 0 |a RU  |b 63413507  |c 20220603  |g RCR 
856 4 |u https://doi.org/10.1140/epjc/s10052-020-08740-y 
942 |c CF