English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Zendy Plus

Presents the access of premium content as premium feature

Premium Content

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Zendy Tools

Zendy Open

The strongly interacting sector in the E6 inspired composite Higgs model(E6CHM) with baryon number violation possesses SU(6)\times U(1)_L globalsymmetry. In the weakly-coupled sector of this model the U(1)_L symmetryassociated with lepton number conservation is broken down to a Z^L_2 discretesymmetry, which stabilizes the proton. Near the scale f > 10 TeV the SU(6)symmetry is broken down to its SU(5) subgroup, giving rise to a set ofpseudo-Nambu-Goldstone bosons (pNGBs) that involves the SM-like Higgs doublet,a scalar coloured triplet and a SM singlet boson. Because f is so high, allbaryon number violating operators are sufficiently strongly suppressed.Nevertheless, in this variant of the E6CHM the observed matter-antimatterasymmetry can be induced if CP is violated. The pNGB scalar coloured tripletplays a key role in this process and leads to a distinct signature that may bedetected at the LHC in the near future.

Generation of baryon asymmetry in the E6CHM