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Production of D (∗) D ¯ (∗) near the thresholds in e+e- annihilation. / Salnikov, S. G.; Milstein, A. I.

In: Physical Review D, Vol. 109, No. 11, 114015, 01.06.2024.

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

Harvard

Salnikov, SG & Milstein, AI 2024, 'Production of D (∗) D ¯ (∗) near the thresholds in e+e- annihilation', Physical Review D, vol. 109, no. 11, 114015. https://doi.org/10.1103/PhysRevD.109.114015

APA

Salnikov, S. G., & Milstein, A. I. (2024). Production of D (∗) D ¯ (∗) near the thresholds in e+e- annihilation. Physical Review D, 109(11), [114015]. https://doi.org/10.1103/PhysRevD.109.114015

Vancouver

Salnikov SG, Milstein AI. Production of D (∗) D ¯ (∗) near the thresholds in e+e- annihilation. Physical Review D. 2024 Jun 1;109(11):114015. doi: 10.1103/PhysRevD.109.114015

Author

Salnikov, S. G. ; Milstein, A. I. / Production of D (∗) D ¯ (∗) near the thresholds in e+e- annihilation. In: Physical Review D. 2024 ; Vol. 109, No. 11.

BibTeX

@article{08cb461f9784468a9e800eaeeb65291e,
title = "Production of D (∗) D ¯ (∗) near the thresholds in e+e- annihilation",
abstract = "It is shown that the nontrivial energy dependencies of DD¯, DD¯∗, and D∗D¯∗ pair production cross sections in e+e- annihilation are well described within the approach based on an account of the final-state interaction of produced particles. This statement is valid for the production of charged and neutral particles. Interaction of D(∗) and D¯(∗) is taken into account using the effective potential method. Its applicability is based on the fact that for near-threshold resonance the characteristic width of peak in the wave function is much larger than the interaction radius. The transition amplitudes between all three channels play an important role in the description of cross sections. These transitions are possible since all channels have the same quantum numbers JPC=1 - . ",
author = "Salnikov, {S. G.} and Milstein, {A. I.}",
year = "2024",
month = jun,
day = "1",
doi = "10.1103/PhysRevD.109.114015",
language = "English",
volume = "109",
journal = "Physical Review D",
issn = "2470-0010",
publisher = "AMER PHYSICAL SOC",
number = "11",

}

RIS

TY - JOUR

T1 - Production of D (∗) D ¯ (∗) near the thresholds in e+e- annihilation

AU - Salnikov, S. G.

AU - Milstein, A. I.

PY - 2024/6/1

Y1 - 2024/6/1

N2 - It is shown that the nontrivial energy dependencies of DD¯, DD¯∗, and D∗D¯∗ pair production cross sections in e+e- annihilation are well described within the approach based on an account of the final-state interaction of produced particles. This statement is valid for the production of charged and neutral particles. Interaction of D(∗) and D¯(∗) is taken into account using the effective potential method. Its applicability is based on the fact that for near-threshold resonance the characteristic width of peak in the wave function is much larger than the interaction radius. The transition amplitudes between all three channels play an important role in the description of cross sections. These transitions are possible since all channels have the same quantum numbers JPC=1 - .

AB - It is shown that the nontrivial energy dependencies of DD¯, DD¯∗, and D∗D¯∗ pair production cross sections in e+e- annihilation are well described within the approach based on an account of the final-state interaction of produced particles. This statement is valid for the production of charged and neutral particles. Interaction of D(∗) and D¯(∗) is taken into account using the effective potential method. Its applicability is based on the fact that for near-threshold resonance the characteristic width of peak in the wave function is much larger than the interaction radius. The transition amplitudes between all three channels play an important role in the description of cross sections. These transitions are possible since all channels have the same quantum numbers JPC=1 - .

UR - https://www.scopus.com/record/display.uri?eid=2-s2.0-85195868156&origin=inward&txGid=05e65d14ec7c616a7246170b71ce80f2

UR - https://www.mendeley.com/catalogue/1a05db84-4ba3-3f2b-94e7-631efc9ec0b6/

U2 - 10.1103/PhysRevD.109.114015

DO - 10.1103/PhysRevD.109.114015

M3 - Article

VL - 109

JO - Physical Review D

JF - Physical Review D

SN - 2470-0010

IS - 11

M1 - 114015

ER -

ID: 60874709