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Dirac leptogenesis in left-right symmetric models

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Left-right symmetric models which employ a generalized seesaw mechanism to generate quark and charged lepton masses are known to solve the strong C P problem via parity symmetry, without the need for the axion. These models lead to naturally light Dirac neutrinos with their masses arising through radiative corrections. In this work, we show how baryogenesis via Dirac leptogenesis can be implemented in this framework. A pair of left-right symmetric scalar doublets ϕ L , R carrying ( B − L ) charge of 3 is introduced for this purpose, which preserves the parity solution to the strong C P problem. Small neutrino masses are generated through one-loop diagrams mediated by these scalars. The decay of vectorlike leptons ( E i ) involved in the seesaw mechanism to generate charged lepton masses, E i → ν ¯ j R ϕ R − , creates a right-handed neutrino ( ν R ) asymmetry, while preserving total lepton number. The compensating lepton asymmetry is converted to baryon asymmetry via electroweak sphalerons. We show that for a large range of model parameters successful baryogenesis can be realized, with the W R ± gauge boson mass of order 10 11     GeV .
American Physical Society (APS)
Title: Dirac leptogenesis in left-right symmetric models
Description:
Left-right symmetric models which employ a generalized seesaw mechanism to generate quark and charged lepton masses are known to solve the strong C P problem via parity symmetry, without the need for the axion.
These models lead to naturally light Dirac neutrinos with their masses arising through radiative corrections.
In this work, we show how baryogenesis via Dirac leptogenesis can be implemented in this framework.
A pair of left-right symmetric scalar doublets ϕ L , R carrying ( B − L ) charge of 3 is introduced for this purpose, which preserves the parity solution to the strong C P problem.
Small neutrino masses are generated through one-loop diagrams mediated by these scalars.
The decay of vectorlike leptons ( E i ) involved in the seesaw mechanism to generate charged lepton masses, E i → ν ¯ j R ϕ R − , creates a right-handed neutrino ( ν R ) asymmetry, while preserving total lepton number.
The compensating lepton asymmetry is converted to baryon asymmetry via electroweak sphalerons.
We show that for a large range of model parameters successful baryogenesis can be realized, with the W R ± gauge boson mass of order 10 11     GeV .

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