Standard

Manifestation of a1(1260) meson in the process e+e– → π+π–π0. / Образцов, Иван Васильевич; Руденко, Александр Сергеевич; Мильштейн, Александр Ильич.

In: Physical Review D, Vol. 110, 094003, 2024.

Research output: Contribution to journal › Article › peer-review

Harvard

Образцов, ИВ, Руденко, АС & Мильштейн, АИ 2024, 'Manifestation of a1(1260) meson in the process e+e– → π+π–π0', Physical Review D, vol. 110, 094003. https://doi.org/10.1103/PhysRevD.110.094003

APA

Образцов, И. В., Руденко, А. С., & Мильштейн, А. И. (2024). Manifestation of a1(1260) meson in the process e+e– → π+π–π0. Physical Review D, 110, [094003]. https://doi.org/10.1103/PhysRevD.110.094003

Vancouver

Образцов ИВ, Руденко АС, Мильштейн АИ. Manifestation of a1(1260) meson in the process e+e– → π+π–π0. Physical Review D. 2024;110:094003. doi: 10.1103/PhysRevD.110.094003

Author

Образцов, Иван Васильевич ; Руденко, Александр Сергеевич ; Мильштейн, Александр Ильич. / Manifestation of a1(1260) meson in the process e+e– → π+π–π0. In: Physical Review D. 2024 ; Vol. 110.

BibTeX

@article{faf57368a9c2442ca387b18e2741b338,
title = "Manifestation of a1(1260) meson in the process e+e– → π+π–π0",
abstract = "The charge asymmetry in the process 푒+⁢푒− →휋+⁢휋−⁢휋0 is studied taking into account a longitudinal polarization of electrons (positrons). The asymmetry arises due to interference of amplitudes corresponding to production of pions in states with charge parity odd and charge parity even. It is a manifestation of 푎1⁡(1260) meson in the intermediate state. Polarization leads to additional correlations in the differential cross section, which simplifies the experimental study of the process. It is shown that the charge asymmetry can reach several percent.",
author = "Образцов, {Иван Васильевич} and Руденко, {Александр Сергеевич} and Мильштейн, {Александр Ильич}",
note = "We are grateful to V. P. Druzhinin and E. P. Solodov for useful discussions. The work of I. V. O. was supported by the Foundation for the Advancement of Theoretical Physics and Mathematics “BASIS” under Grant No. 24-1-5-3-1.",
year = "2024",
doi = "10.1103/PhysRevD.110.094003",
language = "English",
volume = "110",
journal = "Physical Review D",
issn = "2470-0010",
publisher = "AMER PHYSICAL SOC",

}

RIS

TY - JOUR

T1 - Manifestation of a1(1260) meson in the process e+e– → π+π–π0

AU - Образцов, Иван Васильевич

AU - Руденко, Александр Сергеевич

AU - Мильштейн, Александр Ильич

N1 - We are grateful to V. P. Druzhinin and E. P. Solodov for useful discussions. The work of I. V. O. was supported by the Foundation for the Advancement of Theoretical Physics and Mathematics “BASIS” under Grant No. 24-1-5-3-1.

PY - 2024

Y1 - 2024

N2 - The charge asymmetry in the process 푒+⁢푒− →휋+⁢휋−⁢휋0 is studied taking into account a longitudinal polarization of electrons (positrons). The asymmetry arises due to interference of amplitudes corresponding to production of pions in states with charge parity odd and charge parity even. It is a manifestation of 푎1⁡(1260) meson in the intermediate state. Polarization leads to additional correlations in the differential cross section, which simplifies the experimental study of the process. It is shown that the charge asymmetry can reach several percent.

AB - The charge asymmetry in the process 푒+⁢푒− →휋+⁢휋−⁢휋0 is studied taking into account a longitudinal polarization of electrons (positrons). The asymmetry arises due to interference of amplitudes corresponding to production of pions in states with charge parity odd and charge parity even. It is a manifestation of 푎1⁡(1260) meson in the intermediate state. Polarization leads to additional correlations in the differential cross section, which simplifies the experimental study of the process. It is shown that the charge asymmetry can reach several percent.

UR - https://elibrary.ru/item.asp?id=79240335

U2 - 10.1103/PhysRevD.110.094003

DO - 10.1103/PhysRevD.110.094003

M3 - Article

VL - 110

JO - Physical Review D

JF - Physical Review D

SN - 2470-0010

M1 - 094003

ER -

ID: 64626522