Large <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mo stretchy="false">(</mml:mo><mml:mi>g</mml:mi><mml:mo>−</mml:mo><mml:mn>2</mml:mn><mml:msub><mml:mo stretchy="false">)</mml:mo><mml:mi>μ</mml:mi></mml:msub></mml:math> and signals of decays <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>e</mml:mi><mml:mi>b</mml:mi></mml:msub><mml:mo stretchy="false">→</mml:mo><mml:msub><mml:mi>e</mml:mi><mml:mi>a</mml:mi></mml:msub><mml:mi>γ</mml:mi></mml:math> in a <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mn>3</mml:mn><mml:mo>−</mml:mo><mml:mn>3</mml:mn><mml:mo>−</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:math> model with inverse seesaw neutrinos
L. T. Hue, Khiem Hong Phan, N. T. Tham, H. N. Long, Nguyễn Thanh Phong
Abstract
We show that under current experimental bounds of the decays ${e}_{a}\ensuremath{\rightarrow}{e}_{b}\ensuremath{\gamma}$, the recent experimental data of the muon anomalous magnetic dipole moment $(g\ensuremath{-}2{)}_{\ensuremath{\mu}}$ can be explained in the framework of the $3\ensuremath{-}3\ensuremath{-}1$ model with right-handed neutrinos. In addition, all of these branching ratios can reach closely the recent experimental upper bounds.
Topics & Concepts
MuonNeutrinoPhysicsParticle physicsDipoleAlgorithmComputer scienceQuantum mechanicsParticle physics theoretical and experimental studiesNeutrino Physics ResearchQuantum Chromodynamics and Particle Interactions