Isospin structure of electroweak penguin diagrams is different from the gluon-mediated or strong penguin. Given the large top mass, these electroweak contributions are significant. This has the consequence that some previous analyses which relied on a simple isospin structurte in charmless B meson decays become inapplicable. We present the general Hamiltonian in next-to-leading order QCD, and illustrate our conclusion quantitatively for B→ππ and B→Kπ decays in the factorization approximation. Some remarks on CP asymmetries in B meson decays are also made.
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Deshpande et al. (1995) studied this question.
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