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/

Global: Zendy Plus annual

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

Global: Zendy Plus monthly

Global: Zendy Tools annual

Global: Zendy Tools monthly

Global: Zendy Free Plan

Under flavor $SU(3)$ symmetry (SU(3)$_F$), the final-state particles in $B\toPPP$ decays ($P$ is a pseudoscalar meson) are treated as identical, and the$PPP$ must be in a fully-symmetric (FS) state, a fully-antisymmetric (FA)state, or in one of four mixed states. In this paper, we present the formalismfor the FA states. We write the amplitudes for the 22 $B\to PPP$ decays thatcan be in an FA state in terms of both SU(3)$_F$ reduced matrix elements anddiagrams. This shows the equivalence of diagrams and SU(3)$_F$. We also give 15relations among the amplitudes in the SU(3)$_F$ limit, as well as theadditional four that appear when the diagrams $E$/$A$/$PA$ are neglected. Wepresent sets of $B \to PPP$ decays that can be used to extract $\gamma$ usingthe FA amplitudes. The value(s) of $\gamma$ found in this way can be comparedwith the value(s) found using the FS states.

Charmless $B\to PPP$ Decays: the Fully-Antisymmetric Final State