Higgs – Induced Lepton Flavor Violation

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15 Dimension – 6 operators @ 2 loops Dimension – 6 operators contributing up to 0.1% of Yukawas Or, seen differently : Y (1) ij » Y ij ! M > 5 TeV Y (1) ij » 1 ! M > 2000 TeV
Dimension – 6 operators @ 2 loops 16 Θ 13 , Θ 23 < 10 − ¹ , Θ 12 < 10 − ² , φ's < 10 −¹ → The 13, 23 angles are more or less as previously, additional restrictions on the 12 mixing as well as the phases. The 2 – loop contributions induce new bounds on (previously unconstrained) parameters, and actually pretty tight ones!
Page 1 and 2: Higgs - Induced Lepton Flavor Viola
Page 3 and 4: Introduction - the fermion masses i
Page 5 and 6: HDYC : another option 5 → What if
Page 7 and 8: HDYC : the lepton sector 7 The supp
Page 9 and 10: Bounds on Higgs couplings 8 The hll
Page 11 and 12: Bounds on Higgs couplings 8 The hll
Page 13 and 14: Bounds on Higgs couplings : 1-loop
Page 15 and 16: Bounds on Higgs couplings : 2-loops
Page 17 and 18: Dimension - 6 operators : scan stra
Page 19 and 20: Dimension - 6 operators @ 1 loop Di
Page 21: Dimension - 6 operators @ 2 loops 1
Page 25 and 26: Higher - dimensional operators : fo
Page 27 and 28: Higher - dimensional operators : fo
Page 29 and 30: Higher - dimensional operators : re
Page 31 and 32: Merci !
Page 33 and 34: Observables @ 1-loop ¢L = ¡ y ij
Page 35 and 36: The Barr - Zee contributions 8 This
Page 37: Comparison to Froggatt - Nielsen me

Higgs – Induced Lepton Flavor Violation

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