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Электронный каталог: Volkov, M. K. - Description of the Processes e*+e*- *> *p*+*p*- and *t*- *> *p*-*p*0*n&sub(*t) in the NJL Model w...
Volkov, M. K. - Description of the Processes e*+e*- *> *p*+*p*- and *t*- *> *p*-*p*0*n&sub(*t) in the NJL Model w...

Статья
Автор: Volkov, M. K.
Nuclear Physics A: Description of the Processes e*+e*- *> *p*+*p*- and *t*- *> *p*-*p*0*n&sub(*t) in the NJL Model w...
б.г.
ISBN отсутствует
Автор: Volkov, M. K.
Nuclear Physics A: Description of the Processes e*+e*- *> *p*+*p*- and *t*- *> *p*-*p*0*n&sub(*t) in the NJL Model w...
б.г.
ISBN отсутствует
Статья
Volkov, M.K.
Description of the Processes e*+e*- *> *p*+*p*- and *t*- *> *p*-*p*0*n&sub(*t) in the NJL Model with Value of the Vector Coupling Constant g&sub(*r) = 6 / M.K.Volkov, A.A.Pivovarov, K.Nurlan. – Text : electronic // Nuclear Physics A. – 2025. – Vol. 1054. – P. 122992. – URL: https://doi.org/10.1016/j.nuclphysa.2024.122992. – Bibliogr.: 40.
It is shown that the processes e*+e*- *> *p*+*p*- and *t*- *> *p*-*p*0*n&sub(*t) can be described in a unified approach in satisfactory agreement with experiment using the vector coupling constant g&sub(*r)= 6. In this case, in addition to quark loops, it is also necessary to take into account meson loops corresponding to the next order in 1/N&sub(c). These loops must be taken into account when describing the *g(W) *> *r transition, as well as in interaction of mesons in the final state.
Спец.(статьи,препринты) = С 332.7 - Встречные е+е- и мю+мю- пучки
Спец.(статьи,препринты) = С 324.1д - Квантовая хромодинамика$
ОИЯИ = ОИЯИ (JINR)2025
Бюллетени = 15/025
Volkov, M.K.
Description of the Processes e*+e*- *> *p*+*p*- and *t*- *> *p*-*p*0*n&sub(*t) in the NJL Model with Value of the Vector Coupling Constant g&sub(*r) = 6 / M.K.Volkov, A.A.Pivovarov, K.Nurlan. – Text : electronic // Nuclear Physics A. – 2025. – Vol. 1054. – P. 122992. – URL: https://doi.org/10.1016/j.nuclphysa.2024.122992. – Bibliogr.: 40.
It is shown that the processes e*+e*- *> *p*+*p*- and *t*- *> *p*-*p*0*n&sub(*t) can be described in a unified approach in satisfactory agreement with experiment using the vector coupling constant g&sub(*r)= 6. In this case, in addition to quark loops, it is also necessary to take into account meson loops corresponding to the next order in 1/N&sub(c). These loops must be taken into account when describing the *g(W) *> *r transition, as well as in interaction of mesons in the final state.
Спец.(статьи,препринты) = С 332.7 - Встречные е+е- и мю+мю- пучки
Спец.(статьи,препринты) = С 324.1д - Квантовая хромодинамика$
ОИЯИ = ОИЯИ (JINR)2025
Бюллетени = 15/025