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Scalar sextet in the 331 model with right-handed neutrinos
High Energy Physics - Phenomenology · Submitted 8 Dec 2005
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim As will be seen, the present sextet introduction leads to a rich neutrino mass structure.
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The abstract, sentence by sentence
A Higgs sextet is introduced in order to generate Dirac and Majorana neutrino masses in the 331 model with right-handed neutrinos. As will be seen, the present sextet introduction leads to a rich neutrino mass structure. The smallness of neutrino masses can be achieved via, for example, a seesaw limit. The fact that the masses of the charged leptons are not effected by their new Yukawa couplings to the sextet is convenient for generating small neutrino masses.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A Higgs sextet is introduced in order to generate Dirac and Majorana neutrino masses in the 331 model with right-handed neutrinos. | contribution 0.93 | 0.83 | 0.21 | asserted 1.00 |
| s1 | As will be seen, the present sextet introduction leads to a rich neutrino mass structure. | result 0.62 | 0.75 | 0.16 | asserted 0.92 |
| s2 | The smallness of neutrino masses can be achieved via, for example, a seesaw limit. | interpretation 0.40 | 0.29 | 0.11 | hedged possibility 0.94 |
| s3 | The fact that the masses of the charged leptons are not effected by their new Yukawa couplings to the sextet is convenient for generating small neutrino masses. | interpretation 0.82 | 0.69 | 0.09 | asserted 0.99 |
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The paper
Original abstract
A Higgs sextet is introduced in order to generate Dirac and Majorana neutrino masses in the 331 model with right-handed neutrinos. As will be seen, the present sextet introduction leads to a rich neutrino mass structure. The smallness of neutrino masses can be achieved via, for example, a seesaw limit. The fact that the masses of the charged leptons are not effected by their new Yukawa couplings to the sextet is convenient for generating small neutrino masses.
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References
How the literature uses it
3 arXiv papers cite this in 3 sentences
Papers citing it · 2 sentences without a confident label
Cites it as background 1 paper
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A scalar sextet of type, S=[ S^0_11 S^-_12√(2) S^q_13√(2); S^-_12√(2) S^–_22 S^q-1_23√(2); S^q_13√(2) S^q-1_23√(2) S^2q_33 ],often studied in the 3-3-1 models [ref] , can develop a vacuum value such as ⟨S⟩=1√(2)[ κ 0 0; 0 0 0; 0 0 0 ].Other fields if electrically neutral can also have a VEV.
Novel effects of the $W$-boson mass shift in the 3-3-1 model · Tree-level contribution of a sextet · 0.95
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