# Large Top Mass and Non-Linear Representation of Flavour Symmetry

- Published: 11 Jan 2008

partment, 85747 Garching, Germany; Electronic address:

† Electronic address: mannel@hep.physik.uni-siegen.de [1] G. D'Ambrosio, G. F. Giudice, G. Isidori and A. Strumia,

Nucl. Phys. B 645, 155 (2002). [2] R. S. Chivukula and H. Georgi, Phys. Lett. B 188, 99

(1987). [3] R. D. Peccei and H. R. Quinn, Phys. Rev. D 16, 1791

(1977). [4] S. R. Coleman, J. Wess and B. Zumino, Phys. Rev. 177,

2239 (1969); C. G. Callan, S. R. Coleman, J. Wess and

B. Zumino, Phys. Rev. 177, 2247 (1969). [5] G. Buchalla, A. J. Buras and M. E. Lautenbacher, Rev.

Mod. Phys. 68 (1996) 1125. [6] J. F. Gunion and H. E. Haber, Nucl. Phys. B 272 (1986)

1 [Erratum-ibid. B 402 (1993) 567]. [7] T. Feldmann and T. Mannel, JHEP 0702, 067 (2007). [8] In the following, hatted quantities denote dimensionless

fields are spurions with canonical mass dimension. [9] Notice that for b → sγ the VEV for φD in (38) provides

an additional suppression factor vd/v = cos β. [10] We do not discuss the issue of broken Peccei-Quinn sym-

metry [3] here. A detailed discussion can be found in [1].