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Related papers: Universal Seesaw Leptogenesis

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We extend the DFSZ invisible axion model to simultaneously explain small Dirac neutrino masses and cosmic matter-antimatter asymmetry. After the Peccei-Quinn and electroweak symmetry breaking, the effective Yukawa couplings of the Dirac…

High Energy Physics - Phenomenology · Physics 2016-09-07 Pei-Hong Gu

The seesaw theory, the leading theory for particle interactions, provides a viable mechanism for generating the matter-antimatter asymmetry of the universe. Testing the leptogenesis mechanism directly requires measurement of the d=6…

High Energy Physics - Phenomenology · Physics 2008-11-26 Elizabeth Jenkins

We consider the Standard Model extended by right-handed neutrinos to explain massive neutrinos through the seesaw mechanism. The new fermion can be observed when it has a sufficiently small mass and large mixings to left-handed neutrinos.…

High Energy Physics - Phenomenology · Physics 2015-12-17 Takehiko Asaka , Takanao Tsuyuki

We investigate how the baryon asymmetry of our universe via leptogenesis can be achieved within the framework of the seesaw model with Fritzsch type lepton mass matrices proposed by Fukugita $et. al$. We study the cases with CP-violating…

High Energy Physics - Phenomenology · Physics 2008-11-26 Y. H. Ahn , Sin Kyu Kang , C. S. Kim , Jake Lee

In a $U(1)_{R-L}$-symmetric supersymmetric model, pseudo-Dirac bino and wino can act like right-handed neutrinos, generating the light neutrino masses through a hybrid Type I + III inverse seesaw mechanism. We investigate such a model to…

High Energy Physics - Phenomenology · Physics 2026-01-01 Cem Murat Ayber , Tammi Chowdhury , Seyda Ipek

Continuous $U(1)_{L_\mu-L_\tau}$ symmetry can generate quasi degenerate mass spectrum for both left handed light and right handed heavy Majorana neutrinos assuming that the symmetry preserving non zero parameters are nearly same. There is…

High Energy Physics - Phenomenology · Physics 2009-11-11 Biswajit Adhikary

In the framework of the seesaw mechanism with three heavy right-handed Majorana neutrinos and no Higgs triplets we carry out a systematic study of the structure of the right-handed neutrino sector. Using the current low-energy neutrino data…

High Energy Physics - Phenomenology · Physics 2009-11-10 Evgeny Kh. Akhmedov , Michele Frigerio , Alexei Yu. Smirnov

A non-supersymmetric renormalizable $SO(10)$ model is investigated for its viability in explaining the observed fermion masses and mixing parameters along with the baryon asymmetry produced via thermal leptogenesis. The Yukawa sector of the…

High Energy Physics - Phenomenology · Physics 2021-12-10 V. Suryanarayana Mummidi , Ketan M. Patel

In the left-right symmetric models, we can take the left-right symmetry to be the charge-conjugation and then impose a global symmetry under which the left- and right-handed fermion doublets carry equal but opposite charges. Consequently,…

High Energy Physics - Phenomenology · Physics 2010-11-11 Pei-Hong Gu

We discuss symmetries and scenarios leading to quasi-degenerate neutrinos in type-I seesaw models. The existence of degeneracy in the present approach is not linked to any specific structure for the Dirac neutrino Yukawa coupling matrix…

High Energy Physics - Phenomenology · Physics 2010-11-30 Anjan S. Joshipura , Ketan M. Patel , Sudhir K. Vempati

We consider an extended supersymmetric SO(10) seesaw model with only doublet Higgs scalars, in which neutrino masses are suppressed by the scale of D-parity violation. Leptogenesis can occur at the TeV scale through the decay of a singlet…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Hirsch , M. Malinsky , J. C. Romao , U. Sarkar , J. W. F. Valle

We discuss spontaneous Leptogenesis in the Type II Seesaw model of neutrino masses featuring an electroweak triplet scalar $T$ in a coherent pseudo Nambu-Goldstone boson (pNGB) background. In the "wash-in" scenario the inverse decays of…

High Energy Physics - Phenomenology · Physics 2026-04-20 Maximilian Berbig

Curiously in the minimal left right symmetric model, chiral symmetry that protects the electron's mass ($m_e$), due to parity (P), implies in the symmetry limit the vanishing of its neutrino mixing angles. We break the chiral symmetry…

High Energy Physics - Phenomenology · Physics 2024-12-16 Ravi Kuchimanchi

We demonstrate a unified scenario for neutrino mass, baryon asymmetry, dark matter and inflation. In addition to a fermion triplet for the so-called minimal dark matter, we extend the standard model by three heavy fields including a scalar…

High Energy Physics - Phenomenology · Physics 2017-01-25 Hang Zhou , Pei-Hong Gu

Both neutrinoless double beta decay and leptogenesis require neutrinos to be Majorana fermions. A relation between these two phenomena can be derived once the mechanism of neutrino mass generation is specified. We first derive the…

High Energy Physics - Phenomenology · Physics 2021-02-03 Nimmala Narendra , Narendra Sahu , S. Uma Sankar

In this paper, we investigate the implication of modular $\Gamma^{\prime}_5 \simeq A^{\prime}_5$ symmetry on neutrino oscillation phenomenology in the linear seesaw framework. In order to achieve the well defined mass structure for the…

High Energy Physics - Phenomenology · Physics 2022-03-30 Mitesh Kumar Behera , Rukmani Mohanta

We show that existing laboratory experiments have the potential to unveil the origin of matter by probing leptogenesis in the type-I seesaw model with three right-handed neutrinos and Majorana masses in the GeV range. The baryon asymmetry…

High Energy Physics - Phenomenology · Physics 2015-05-25 Laurent Canetti , Marco Drewes , Björn Garbrecht

We extend the $SU(3)_c \times SU(2)_L \times U(1)_Y$ standard model by a $U(1)_{Y'}$ gauge symmetry. Three right-handed neutrinos are introduced to cancel the gauge anomaly. One Higgs singlet is responsible for spontaneously breaking the…

High Energy Physics - Phenomenology · Physics 2023-01-11 Su-Ping Chen , Pei-Hong Gu

In many extensions of the Standard Model, including a broad class of left-right symmetric and Grand Unified theories, the light neutrino mass matrix is given by the left-right symmetric seesaw formula $M_\nu = f v_L - \frac{v^2}{v_R} Y_\nu…

High Energy Physics - Phenomenology · Physics 2009-11-11 Pierre Hosteins , Stephane Lavignac , Carlos A. Savoy

Left Right Symmetric Model (LRSM) being an extension of the Standard model of particle physics incorporates within itself Type-I and Type-II seesaw mass terms naturally. Both the mass terms can have significant amount of contribution to the…

High Energy Physics - Phenomenology · Physics 2024-03-05 Ankita Kakoti , Mrinal Kumar Das