Effects of local parity nonconservation in strong interactions in Pb-Pb collisions at LHC energy
- Авторлар: Kovalenko V.N.1
-
Мекемелер:
- Saint-Petersburg State University
- Шығарылым: Том 88, № 11 (2024)
- Беттер: 1777–1782
- Бөлім: Fundamental problems and applications of physics of atomic nucleus
- URL: https://cijournal.ru/0367-6765/article/view/682569
- DOI: https://doi.org/10.31857/S0367676524110198
- EDN: https://elibrary.ru/FKBZNA
- ID: 682569
Дәйексөз келтіру
Аннотация
Accounting for the effects of local parity nonconservation in a strongly interacting medium is implemented within the framework of the Monte Carlo model. Predictions are obtained for the distributions of the invariant masses of di-muons and di-electrons from the decays of light vector mesons in Pb-Pb collisions at the LHC energy, taking into account the resolution of the detecting systems. The influence of fluctuations of the axial chemical potential is estimated.
Толық мәтін

Авторлар туралы
V. Kovalenko
Saint-Petersburg State University
Хат алмасуға жауапты Автор.
Email: v.kovalenko@spbu.ru
Ресей, St. Petersburg, 199034
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Әрекет
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Fig. 1. Distribution of invariant masses of di-muons from decays of ρ- and ω-mesons without taking into account detector effects in the presence of a medium violating P-parity at μ5 = 0.1 GeV: without selection by the angle θA between leptons (a), under the condition 0.4 < θA < 0.5 (b).
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Fig. 2. Distribution of invariant masses of di-muons (a, c) and di-electrons (b, d) from decays of ρ- and ω-mesons under the conditions of the ALICE Run 2 experiment at μ5 = 0.1 GeV: without selection by angle θA (a, b), under the condition 0.4 < θA < 0.8 (c), under the condition 0.4 < θA < 0.5 (d).
Жүктеу (164KB)
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Fig. 3. Distribution of invariant masses of di-muons (a, c) and di-electrons (b, d) from decays of ρ- and ω-mesons under the expected conditions of the ALICE Run 3 experiment at μ5 = 0.1 GeV: without selection by angle θA (a, b), under the condition 0.4 < θA < 0.5 (c, d).
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Fig. 4. Effect of axial chemical potential fluctuations on the splitting of the spectral functions of ρ- and ω-mesons in the spectrum of invariant masses of di-muons (a, c) and di-electrons (b, d): 0.05 GeV < μ5 < 0.15 GeV (σμ ≈ 30%) (a, b), 0 GeV < μ5 < 0.2 GeV (σμ ≈ 60%) (c, d). The resolving power of the ALICE experiment under Run 3 conditions is taken into account.
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