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Unconventional Neutrino Mass Generation, Neutrinoless Double Beta Decays, and Collider Phenomenology
High Energy Physics - Phenomenology · Submitted 11 Oct 2006
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Instead the short distance physics with doubly charged Higgs exchange gives the leading contribution.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We study a model in which lepton number violation is solely triggered by a dimension 4 hard breaking term in the scalar potential. A minimal model which contains a SU(2) triplet with hypercharge Y=2, and a pair of singlet doubly charged scalar fields in addition to the Standard Model (SM) Higgs doublet is constructed. The model is technically natural in the sense that lepton number is preserved in the limit that the hard term vanishes. SM phenomenology restricts the vacuum expectation value of the triplet scalar field $v_T<5.78$ GeV. Neutrino masses controlled by $v_T$ are generated at the two loop level and are naturally to the sub-eV range. In general they exhibit normal hierarchy structure. Here the neutrino mass term does not dominate neutrinoless double beta decays of nuclei. Instead the short distance physics with doubly charged Higgs exchange gives the leading contribution. We expect weak scale singly and doubly charged Higgs bosons to make their appearances at the LHC and the ILC.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study a model in which lepton number violation is solely triggered by a dimension 4 hard breaking term in the scalar potential. | contribution 0.97 | 0.85 | 0.10 | asserted 1.00 |
| s1 | A minimal model which contains a SU(2) triplet with hypercharge Y=2, and a pair of singlet doubly charged scalar fields in addition to the Standard Model (SM) Higgs doublet is constructed. | contribution 0.62 | 0.87 | 0.05 | asserted 1.00 |
| s2 | The model is technically natural in the sense that lepton number is preserved in the limit that the hard term vanishes. | interpretation 0.50 | 0.66 | 0.07 | asserted 1.00 |
| s3 | SM phenomenology restricts the vacuum expectation value of the triplet scalar field $v_T<5.78$ GeV. | result 0.80 | 0.33 | 0.06 | asserted 1.00 |
| s4 | Neutrino masses controlled by $v_T$ are generated at the two loop level and are naturally to the sub-eV range. | result 0.99 | 0.78 | 0.14 | asserted 0.97 |
| s5 | In general they exhibit normal hierarchy structure. | result 0.97 | 0.68 | 0.07 | asserted 0.76 |
| s6 | Here the neutrino mass term does not dominate neutrinoless double beta decays of nuclei. | result 0.90 | 0.77 | 0.17 | asserted 1.00 |
| s7 | Instead the short distance physics with doubly charged Higgs exchange gives the leading contribution. | result 0.78 | 0.74 | 0.27 | asserted 1.00 |
| s8 | We expect weak scale singly and doubly charged Higgs bosons to make their appearances at the LHC and the ILC. | interpretation 0.70 | 0.29 | 0.22 | hedged possibility 0.77 |
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The paper
Original abstract
We study a model in which lepton number violation is solely triggered by a dimension 4 hard breaking term in the scalar potential. A minimal model which contains a SU(2) triplet with hypercharge Y=2, and a pair of singlet doubly charged scalar fields in addition to the Standard Model (SM) Higgs doublet is constructed. The model is technically natural in the sense that lepton number is preserved in the limit that the hard term vanishes. SM phenomenology restricts the vacuum expectation value of the triplet scalar field $v_T<5.78$ GeV. Neutrino masses controlled by $v_T$ are generated at the two loop level and are naturally to the sub-eV range. In general they exhibit normal hierarchy structure. Here the neutrino mass term does not dominate neutrinoless double beta decays of nuclei. Instead the short distance physics with doubly charged Higgs exchange gives the leading contribution. We expect weak scale singly and doubly charged Higgs bosons to make their appearances at the LHC and the ILC.
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References
How the literature uses it
11 arXiv papers cite this in 22 sentences
Papers citing it · 12 sentences without a confident label
Builds on it 1 paper
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Here, we give an explicit example[Two possible scenarios have been mentioned in the footnote of Ref. [ref] .] to forbid the tree contributions to the neutrino masses.
Relating Neutrino Masses by dilepton modes of Doubly Charged Scalars · The model · 0.80
Compares with it 1 paper
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In contrast the dependence is linear in the estimate for the model in Refs. [ref] , showing that $χ$ must be assigned LN 2, as in see-saw models of type II.
A realistic model of neutrino masses with a large neutrinoless double beta decay rate · Neutrino mass generation and $θ_13$ expectation · 1.00
Cites it as background 6 papers
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The simplest version of the model has been given in Ref. [ref] with some of its phenomenologies presented in Ref. [ref] .
Relating Neutrino Masses by dilepton modes of Doubly Charged Scalars · The model · 0.89
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Various possibilities of such types of the models that can induce the $0ν2β$ decay have been considered [ref] .
Neutrinoless double beta decay and the muonium-to-antimuonium transition in models with a doubly charged scalar · Introduction · 0.94
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Another interesting class of models are based on internal electroweak gauge bosons, which are based on CLBZ-type topologies and discussed in Refs. [ref] .
From the trees to the forest: a review of radiative neutrino mass models · Models based on several topologies · 0.93
Discussion
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