4,182 research outputs found

    An S4ƗSU(5)S_4 \times SU(5) SUSY GUT of flavour in 6d

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    We propose a 6d model with a SUSY SU(5)SU(5) gauge symmetry. After compactification, it explains the origin of the S4S_4 Family Symmetry with CSD3 vacuum alignment, as well as SU(5)SU(5) breaking with doublet-triplet splitting. The model naturally accounts for all quark and lepton (including neutrino) masses and mixings, incorporating the highly predictive Littlest Seesaw structure. It spontaneously breaks CP symmetry, resulting in successful CP violation in the quark and lepton sectors, while solving the Strong CP problem. It also explains the Baryon Asymmetry of the Universe (BAU) through leptogenesis, with the leptogenesis phase directly linked to the Dirac and Majorana phases.Comment: 23 pages, 6 figures. v3: Version published in JHE

    The Output Cost of Disinflation in Traditional and Vector Autoregressive Models

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    macroeconomics, vector autoregressive model, disinflation

    Generalised CP and A4A_4 Family Symmetry

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    We perform a comprehensive study of family symmetry models based on A4A_4 combined with the generalised CP symmetry HCPH_{\rm{CP}}. We investigate the lepton mixing parameters which can be obtained from the original symmetry A4ā‹ŠHCPA_4\rtimes H_{\rm{CP}} breaking to different remnant symmetries in the neutrino and charged lepton sectors. We find that only one case is phenomenologically viable, namely GCPĪ½ā‰…Z2SƗHCPĪ½G^{\nu}_{\rm{CP}}\cong Z^{S}_2\times H^{\nu}_{\rm{CP}} in the neutrino sector and GCPlā‰…Z3Tā‹ŠHCPlG^{l}_{\rm{CP}}\cong Z^{T}_3\rtimes H^{l}_{\rm{CP}} in the charged lepton sector, leading to the prediction of no CP violation, namely Ī“CP\delta_{CP} and the Majorana phases Ī±21\alpha_{21} and Ī±31\alpha_{31} are all equal to either zero or Ļ€\pi. We then propose an effective supersymmetric model based on the symmetry A4ā‹ŠHCPA_4\rtimes H_{\rm{CP}} in which trimaximal lepton mixing is predicted together with either zero CP violation or Ī“CPā‰ƒĀ±Ļ€/2\delta_{CP}\simeq\pm \pi/2 with non-trivial Majorana phases. An ultraviolet completion of the effective model yields a neutrino mass matrix which depends on only three real parameters. As a result of this, all three CP phases and the absolute neutrino mass scale are determined, the atmospheric mixing angle is maximal, and the Dirac CP can either be preserved with Ī“CP=0,Ļ€\delta_{CP}=0,\pi or maximally broken with Ī“CP=Ā±Ļ€/2\delta_{CP}=\pm \pi /2 and sharp predictions for the Majorana phases and neutrinoless double beta decay.Comment: 38 pages, 3 figure

    SO(10)ƗS4\mathbf{SO(10)}\times \mathbf{S_4} Grand Unified Theory of Flavour and Leptogenesis

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    We propose a Grand Unified Theory of Flavour, based on SO(10)SO(10) together with a non-Abelian discrete group S4S_4, under which the unified three quark and lepton 16-plets are unified into a single triplet 3ā€²3'. The model involves a further discrete group Z4RƗZ43 \mathbb{Z}_4^R\times \mathbb{Z}_4^3 which controls the Higgs and flavon symmetry breaking sectors. The CSD2 flavon vacuum alignment is discussed, along with the GUT breaking potential and the doublet-triplet splitting, and proton decay is shown to be under control. The Yukawa matrices are derived in detail, from renormalisable diagrams, and neutrino masses emerge from the type I seesaw mechanism. A full numerical fit is performed with 15 input parameters generating 19 presently constrained observables, taking into account supersymmetry threshold corrections. The model predicts a normal neutrino mass ordering with a CP oscillation phase of 260āˆ˜260^{\circ}, an atmospheric angle in the first octant and neutrinoless double beta decay with mĪ²Ī²=11m_{\beta \beta}= 11 meV. We discuss N2N_2 leptogenesis, which fixes the second right-handed neutrino mass to be M2ā‰ƒ2Ɨ1011M_2\simeq 2\times 10^{11} GeV, in the natural range predicted by the model.Comment: 26 pages, 10 figure
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