Joint Seminar LAPP/LAPTh
vendredi 24 novembre 2023 -
14:30
lundi 20 novembre 2023
mardi 21 novembre 2023
mercredi 22 novembre 2023
jeudi 23 novembre 2023
vendredi 24 novembre 2023
14:30
New Physics event re-weighting -- general conditions
-
Zbigniew Was
(
INP Cracovie
)
New Physics event re-weighting -- general conditions
Zbigniew Was
(
INP Cracovie
)
14:30 - 15:00
Room: Auditorium Marcel Vivargent
Usually new physics effects, such as of dark photons, anomalous magnetic/electric dipole moments are expected to be at the edge of observability. That is why, for their predictions, simultaneous control of Standard Model predictions of sufficient precision is essential. I will comment the two classes of solutions, when internal information from the main Monte Carlo of Standard Model predictions is used or if information stored in event record is used only. Advantages, disadvantages and practical difficulties for the users will be addressed.
15:00
Electron-positron, quark-antiquark and photon-photon production of tau-lepton pairs: spin effects induced by anomalous magnetic and electric dipole moments of tau lepton
-
Alexander Korchin
(
KIPT - Kharkov Institute of Physics and Technology
)
Electron-positron, quark-antiquark and photon-photon production of tau-lepton pairs: spin effects induced by anomalous magnetic and electric dipole moments of tau lepton
Alexander Korchin
(
KIPT - Kharkov Institute of Physics and Technology
)
15:00 - 15:30
Room: Auditorium Marcel Vivargent
Anomalous contributions to the magnetic and electric dipole moments of the tau lepton have brought renewed interest in the development of new CP violating signatures in tau-pair production at Belle II, and at higher energies of the LHC and the Future Circular Collider. We discuss spin correlations in the tau- tau+ pair produced in e- e+, q qbar -> tau- tau+ and gamma gamma -> tau- tau+ processes. Effects of anomalous dipole moments are introduced on top of precision simulations of these processes in the standard Model (SM). The tau decays are simulated along with radiative corrections, in particular, electroweak box contributions of WW and ZZ exchange diagrams are taken into account.