2018
DOI: 10.1007/jhep10(2018)184
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Fitting high-energy Littlest Seesaw parameters using low-energy neutrino data and leptogenesis

Abstract: We show that the four high-energy Littlest Seesaw parameters in the flavour basis, namely two real Yukawa couplings plus the two right-handed neutrino masses, can be determined by an excellent fit to the seven currently constrained observables of low-energy neutrino data and leptogenesis. Taking into account renormalisation group corrections, we estimate χ 2 1.5 − 2.6 for the three d.o.f., depending on the high-energy scale and the type of non-supersymmetric Littlest Seesaw model. We extract allowed ranges of … Show more

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Cited by 25 publications
(51 citation statements)
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“…Hence, according to Ref. [26], we take the following benchmark values for the right-handed neutrino Majorana masses M 1 = 5.10 × 10 10 GeV and…”
Section: The Modelmentioning
confidence: 99%
“…Hence, according to Ref. [26], we take the following benchmark values for the right-handed neutrino Majorana masses M 1 = 5.10 × 10 10 GeV and…”
Section: The Modelmentioning
confidence: 99%
“…where J k L +k E (γ f , τ f ) = J k L +k E (γ 0 , τ 0 ) and J 2k L (γ f , τ f ) = J 2k L (γ 0 , τ 0 ) are certain phase factors 3 , as shown in Eq. (55). From Eq.…”
Section: Residual Modular Symmetry and Its Implicationmentioning
confidence: 99%
“…The so-called TM1 mixing matrix indicates the following sum rule among the Dirac CP phase δ CP and mixing angles cos δ CP = (3 − 5 cos 2θ 13 ) cot 2θ 23 4 sin θ 13 √ 3 cos 2θ 13 − 1 .…”
Section: Mixing Patterns Derived From S 4 With No Neutrino Massesmentioning
confidence: 99%
“…The neutrino masses m 2 2 and m 2 3 are dependent on free parameters m a and r. If we require that all the three lepton mixing angles and two mass squared differences lie in their corresponding experimentally 3σ intervals [1]. Then the lepton mixing parameters and the neutrino masses are predicted to be 0.3362 ≤ sin 2 θ 12 ≤ 0.3364, 0.02254 ≤ sin 2 θ 13 ≤ 0.02280, 0.556 ≤ sin 2 θ 23 We see that all mixing parameters and neutrino masses are restricted in rather narrow regions. It is straightforward to show that the model above is a powerful model to predicted lepton mixing parameters and neutrino masses, especially for mixing angle θ 12 .…”
Section: The Structure Of the Modelmentioning
confidence: 99%
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