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B, D and K decays

G. Buchalla T. K. Komatsubara F. Muheim L. Silvestrini 1 M. Artuso D. M. Asner P. Ball E. Baracchini G. Bell M. Beneke J. Berryhill A. Bevan I. I. Bigi 2, 3, 4, 5 M. Blanke Ch. Bobeth M. Bona 6 F. Borzumati T. Browder T. Buanes O. Buchmuller A. J. Buras S. Burdin 3, 7, 8 D. G. Cassel 9 R. Cavanaugh M. Ciuchini 10 P. Colangelo G. Crosetti A. Dedes F. de Fazio S. Descotes-Genon 5 J. Dickens Z. Dolezal S. Durr U. Egede C. Eggel G. Eigen S. Fajfer 11, 12 Th. Feldmann Rosalinda Ferrandes 13 P. Gambino T. Gershon V. Gibson M. Giorgi 14, 15 V. V. Gligorov B. Golob A. Golutvin Y. Grossman D. Guadagnoli U. Haisch M. Hazumi S. Heinemeyer G. Hiller D. Hitlin T. Huber T. Hurth T. Iijima A. Ishikawa G. Isidori S. Jager A. Khodjamirian P. Koppenburg 16 T. Lagouri U. Langenegger C. Lazzeroni A. Lenz V. Lubicz 10 W. Lucha H. Mahlke D. Melikhov F. Mescia 17 M. Misiak M. Nakao J. Napolitano N. Nikitin U. Nierste K. Oide Y. Okada P. Paradisi F. Parodi 3, 18 M. Patel 19 A. A. Petrov 20 T. N. Pham 21 M. Pierini 3 S. Playfer G. Polesello A. Policicchio A. Poschenrieder P. Raimondi S. Recksiegel P. Reznicek A. Robert 22 S. Robertson 23, 24 J. L. Rosner G. Ruggiero A. Sarti O. Schneider 25 F. Schwab S. Simula S. Sivoklokov Pietro Slavich 26, 27 C. Smith 28, 29, 30 M. Smizanska A. Soni T. Speer P. Spradlin M. Spranger A. Starodumov B. Stech A. Stocchi 3 S. Stone C. Tarantino F. Teubert S. t'Jampens 6 K. Toms Karim Trabelsi 31 S. Trine S. Uhlig 32 V. Vagnoni 33 J. J. van Hunen G. Weiglein A. Weiler G. Wilkinson Y. Xie 34 M. Yamauchi G. Zhu 21, 35 J. Zupan R. Zwicky
13 G-SCOP_SIREP [?-2015] - Système d’Information, conception RobustE des Produits [?-2015]
G-SCOP [2006-2015] - Laboratoire des sciences pour la conception, l'optimisation et la production [2006-2015]
Abstract : With the advent of the LHC, we will be able to probe New Physics (NP) up to energy scales almost one order of magnitude larger than it has been possible with present accelerator facilities. While direct detection of new particles will be the main avenue to establish the presence of NP at the LHC, indirect searches will provide precious complementary information, since most probably it will not be possible to measure the full spectrum of new particles and their couplings through direct production. In particular, precision measurements and computations in the realm of flavour physics are expected to play a key role in constraining the unknown parameters of the Lagrangian of any NP model emerging from direct searches at the LHC. The aim of Working Group 2 was twofold: on one hand, to provide a coherent, up-to-date picture of the status of flavour physics before the start of the LHC; on the other hand, to initiate activities on the path towards integrating information on NP from high-pT and flavour data.
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G. Buchalla, T. K. Komatsubara, F. Muheim, L. Silvestrini, M. Artuso, et al.. B, D and K decays. European Physical Journal C: Particles and Fields, Springer Verlag (Germany), 2008, pp.309-492. ⟨10.1140/epjc/s10052-008-0716-1⟩. ⟨hal-00204334⟩



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