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Broken SU(3) Symmetry in Two-Body B Decays

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arxiv hep-ph/9504326 v2 pith:RXGVOAGY submitted 1995-04-18 hep-ph

Broken SU(3) Symmetry in Two-Body B Decays

classification hep-ph
keywords decaysinvolvingbrokeneffectsfinalsymmetrytwo-bodyanalysis
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The decays of $B$ mesons to two-body hadronic final states are analyzed within the context of broken flavor SU(3) symmetry, extending a previous analysis involving pairs of light pseudoscalars to decays involving one or two charmed quarks in the final state. A systematic program is described for learning information {}from decay rates regarding (i) SU(3)-violating contributions, (ii) the magnitude of exchange and annihilation diagrams (effects involving the spectator quark), and (iii) strong final-state interactions. The implication of SU(3)-breaking effects for the extraction of weak phases is also examined. The present status of data on these questions is reviewed and suggestions for further experimental study are made.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. A Phenomenological Model of Mesons for Charged Current Weak Decays

    hep-ph 2026-05 unverdicted novelty 6.0

    A symmetry-guided phenomenological model organizes leading current-current operators for charged-current decays of heavy-light mesons and reproduces heavy-quark scaling relations for decay constants and form factors.

  2. QCD-factorization amplitudes from flavour symmetries: beyond the $SU(3)$ symmetric case

    hep-ph 2026-04 unverdicted novelty 5.0

    A data-driven SU(3)-breaking analysis of B to PP decays yields QCD-factorization amplitudes that resemble dynamical predictions and require no enhanced annihilation terms.

  3. Studying the tensor resonance contributions in $B \to PP\ell^+\ell^-$ and $B \to PV\ell^+\ell^-$ decays

    hep-ph 2026-07 conditional novelty 4.0

    Tensor-resonance contributions to B → PPℓ⁺ℓ⁻ and B → PVℓ⁺ℓ⁻ are small compared with measured totals once SU(3)-related B → Tℓ⁺ℓ⁻ rates are fixed to Bs → f′₂(1525)μ⁺μ⁻.