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      Final State Interactions and New Physics in B -> pi K Decays

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          Abstract

          Within the Standard Model, and if one assumes that soft rescattering effects are negligible, the CP asymmetry A^dir_CP (B^\pm -> \pi^\pm K) is predicted to be very small and the ratio R = BR(B_d -> \pi^\mp K^\pm)/BR(B^\pm -> \pi^\pm K) provides a bound on the angle \gamma of the unitarity triangle, sin^2 \gamma \leq R. We estimate the corrections from soft rescattering effects using an approach based on Regge phenomenology, and find effects of order 10% with large uncertainties. In particular, we conclude that A^dir_CP \sim 0.2 and sin^2 \gamma \sim 1.2 R could not be taken unambiguously to signal New Physics. Using SU(3) relations, we suggest experimental tests that could constrain the size of the soft rescattering effects thus reducing the related uncertainty. Finally, we study the effect of various models of New Physics on A^dir_CP and on R.

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          Weak Decays Beyond Leading Logarithms

          We review the present status of QCD corrections to weak decays beyond the leading logarithmic approximation including particle-antiparticle mixing and rare and CP violating decays. After presenting the basic formalism for these calculations we discuss in detail the effective hamiltonians for all decays for which the next-to-leading corrections are known. Subsequently, we present the phenomenological implications of these calculations. In particular we update the values of various parameters and we incorporate new information on m_t in view of the recent top quark discovery. One of the central issues in our review are the theoretical uncertainties related to renormalization scale ambiguities which are substantially reduced by including next-to-leading order corrections. The impact of this theoretical improvement on the determination of the Cabibbo-Kobayashi-Maskawa matrix is then illustrated in various cases.
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            CPNoninvariance in the Decays of Heavy Charged Quark Systems

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              Systematics of soft final state interactions in \(B\) decay

              By using very general and well established features of soft strong interactions we show, contrary to conventional expectations, that (i) soft final state interactions (FSI) do not disappear for large \(m_B\), (ii) inelastic rescattering is expected to be the main source of soft FSI phases, and (iii) flavor off-diagonal FSI are suppressed by a power of \(m_B\), but are quite likely to be significant at \(m_B\simeq 5\)~GeV. We briefly discuss the influence of these interactions on tests of CP-violation and on theoretical calculations of weak decays.
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                Author and article information

                Journal
                01 December 1997
                1997-12-08
                Article
                10.1103/PhysRevD.57.4290
                hep-ph/9712225
                0b8fb634-4d73-4116-85af-c8933ea6c31a
                History
                Custom metadata
                JHU--TIPAC--97018, UCHEP-79, WIS-97/36/Dec-PH
                Phys.Rev.D57:4290-4300,1998
                20 pages, RevTex, no figures; a few typos corrected, references added, brief additional discussion of uncertanties is added
                hep-ph

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