Ioseph Buchbinder
(Laboratory of Theoretical Physics, Joint Institute for Nuclear Research)
11/08/2025, 09:40
Lecture
Andrei Barvinsky
11/08/2025, 10:30
Dmitry Kazakov
(JINR)
11/08/2025, 11:30
Victor Fadin
(Budker Institute of Nuclear Physics)
11/08/2025, 12:00
Mikhail Ivanov
(Joint Institute for Nuclear Research, Dubna, Russia)
11/08/2025, 12:30
Andrei Starinets
(University of Oxford)
12/08/2025, 10:00
Roman Lee
(Budker Institute of Nuclear Physics)
12/08/2025, 11:30
Vladimir Saleev
(Samara National Research University)
12/08/2025, 12:30
Andrey Grozin
(Budker Institute of Nuclear Physics)
13/08/2025, 09:30
Sergey Mikhailov
(BLTP, JINR)
13/08/2025, 10:30
Alexey Isaev
(BLTP, JINR)
13/08/2025, 11:30
Alexei Yung
(Petersburg Nuclear Physics Institute)
13/08/2025, 12:00
Andrei Marshakov
(HSE University & ITEP)
13/08/2025, 12:30
Mikhail Vasiliev
(LPI RAS)
14/08/2025, 09:30
Evgeny Ivanov
(BLTP JINR)
14/08/2025, 10:30
Oleg Tarasov
(JINR Dubna, Moscow Region, Russia)
14/08/2025, 12:30
Andrei Kataev
(Institute for Nuclear Research of RAS)
15/08/2025, 09:30
Konstantin Stepanyantz
(MSU)
15/08/2025, 10:00
Alexander Bednyakov
(Joint Institute for Nuclear Research)
15/08/2025, 11:30
Igor Volobuev
(Skobeltsyn Institute of Nuclear Physics (SINP MSU))
15/08/2025, 12:00
Vasiliy Neznamov
(Federal Nuclear Center-All-Russian Research Institute of Experimental Physics (FSUE "RFNC-VNIIEF"))
15/08/2025, 12:30
We examine the Foldy-Wouthuysen, Feynman-Gell-Mann, and self-adjoint representations of the Dirac equation for fermions with spinor wave functions. The analysis is conducted for electrons and positrons interacting with electromagnetic fields. Versions of quantum electrodynamics are considered both within the scope of perturbation theory and in the non-perturbative regime with strong...