001 | 916232 | ||
005 | 20240610121330.0 | ||
024 | 7 | _ | |a 10.48550/ARXIV.2212.07794 |2 doi |
024 | 7 | _ | |a 2128/33281 |2 Handle |
037 | _ | _ | |a FZJ-2022-06033 |
041 | _ | _ | |a English |
100 | 1 | _ | |a Akdag, Hakan |0 P:(DE-HGF)0 |b 0 |e Corresponding author |
245 | _ | _ | |a $C$ and $CP$ violation in effective field theories |
260 | _ | _ | |c 2022 |b arXiv |
336 | 7 | _ | |a Preprint |b preprint |m preprint |0 PUB:(DE-HGF)25 |s 1671702283_17299 |2 PUB:(DE-HGF) |
336 | 7 | _ | |a WORKING_PAPER |2 ORCID |
336 | 7 | _ | |a Electronic Article |0 28 |2 EndNote |
336 | 7 | _ | |a preprint |2 DRIVER |
336 | 7 | _ | |a ARTICLE |2 BibTeX |
336 | 7 | _ | |a Output Types/Working Paper |2 DataCite |
490 | 0 | _ | |v 2212.07794 |
520 | _ | _ | |a The quest for new sources of the simultaneous violation of $C$ and $CP$ symmetry was popular in the 1960s and has since been mostly neglected for more than half a century. In this work we revisit fundamental quark-level operators that break $C$ and $CP$ up to and including mass dimension 8 for flavor-conserving transitions, relying on the complete operator sets of the so-called Standard Model effective field theory and the low-energy effective field theory. With the formalism of chiral perturbation theory, we match these quark operators to light-meson physics, derive $C$- and $CP$-odd Lagrangians for several processes in the $η$, $η'$, and pion sectors, and furthermore, as a proof of principle, give estimates for the respective observables in explicit dependence of the underlying high-energy scale for new physics. |
536 | _ | _ | |a 5111 - Domain-Specific Simulation & Data Life Cycle Labs (SDLs) and Research Groups (POF4-511) |0 G:(DE-HGF)POF4-5111 |c POF4-511 |f POF IV |x 0 |
588 | _ | _ | |a Dataset connected to DataCite |
650 | _ | 7 | |a High Energy Physics - Phenomenology (hep-ph) |2 Other |
650 | _ | 7 | |a Nuclear Theory (nucl-th) |2 Other |
650 | _ | 7 | |a FOS: Physical sciences |2 Other |
700 | 1 | _ | |a Kubis, Bastian |0 P:(DE-HGF)0 |b 1 |
700 | 1 | _ | |a Wirzba, Andreas |0 P:(DE-Juel1)131377 |b 2 |u fzj |
773 | _ | _ | |a 10.48550/ARXIV.2212.07794 |
856 | 4 | _ | |u https://juser.fz-juelich.de/record/916232/files/2212.07794.pdf |y OpenAccess |
909 | C | O | |o oai:juser.fz-juelich.de:916232 |p openaire |p open_access |p VDB |p driver |p dnbdelivery |
910 | 1 | _ | |a Forschungszentrum Jülich |0 I:(DE-588b)5008462-8 |k FZJ |b 2 |6 P:(DE-Juel1)131377 |
913 | 1 | _ | |a DE-HGF |b Key Technologies |l Engineering Digital Futures – Supercomputing, Data Management and Information Security for Knowledge and Action |1 G:(DE-HGF)POF4-510 |0 G:(DE-HGF)POF4-511 |3 G:(DE-HGF)POF4 |2 G:(DE-HGF)POF4-500 |4 G:(DE-HGF)POF |v Enabling Computational- & Data-Intensive Science and Engineering |9 G:(DE-HGF)POF4-5111 |x 0 |
914 | 1 | _ | |y 2022 |
915 | _ | _ | |a OpenAccess |0 StatID:(DE-HGF)0510 |2 StatID |
920 | _ | _ | |l yes |
920 | 1 | _ | |0 I:(DE-Juel1)IAS-4-20090406 |k IAS-4 |l Theorie der Starken Wechselwirkung |x 0 |
920 | 1 | _ | |0 I:(DE-Juel1)IKP-3-20111104 |k IKP-3 |l Theorie der starken Wechselwirkung |x 1 |
980 | 1 | _ | |a FullTexts |
980 | _ | _ | |a preprint |
980 | _ | _ | |a VDB |
980 | _ | _ | |a UNRESTRICTED |
980 | _ | _ | |a I:(DE-Juel1)IAS-4-20090406 |
980 | _ | _ | |a I:(DE-Juel1)IKP-3-20111104 |
981 | _ | _ | |a I:(DE-Juel1)IAS-4-20090406 |
Library | Collection | CLSMajor | CLSMinor | Language | Author |
---|