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Neutrino Mass and Dark Matter from Gauged $U(1)_{B-L}$ Breaking
High Energy Physics - Phenomenology · Submitted 8 May 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that this model can satisfy current bounds from neutrino oscillation data, the lepton flavor violation, the relic abundance of the dark matter, and the direct search for the dark matter.
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The abstract, sentence by sentence
We propose a new model where the Dirac mass term for neutrinos, the Majorana mass term for right-handed neutrinos, and the other new fermion masses arise via the spontaneous breakdown of the $U(1)_{B-L}$ gauge symmetry. The anomaly-free condition gives four sets of assignment of the B-L charge to new particles, and three of these sets have an associated global $U(1)_{DM}$ symmetry which stabilizes dark matter candidates. The dark matter candidates contribute to generating the Dirac mass term for neutrinos at the one-loop level. Consequently, tiny neutrino masses are generated at the two-loop level via a Type-I-Seesaw-like mechanism. We show that this model can satisfy current bounds from neutrino oscillation data, the lepton flavor violation, the relic abundance of the dark matter, and the direct search for the dark matter. This model would be tested at future collider experiments and dark matter experiments.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We propose a new model where the Dirac mass term for neutrinos, the Majorana mass term for right-handed neutrinos, and the other new fermion masses arise via the spontaneous breakdown of the $U(1)_{B-L}$ gauge symmetry. | contribution 0.94 | 0.83 | 0.15 | asserted 0.83 |
| s1 | The anomaly-free condition gives four sets of assignment of the B-L charge to new particles, and three of these sets have an associated global $U(1)_{DM}$ symmetry which stabilizes dark matter candidates. | result 0.65 | 0.80 | 0.11 | asserted 1.00 |
| s2 | The dark matter candidates contribute to generating the Dirac mass term for neutrinos at the one-loop level. | method 0.43 | 0.72 | 0.08 | asserted 1.00 |
| s3 | Consequently, tiny neutrino masses are generated at the two-loop level via a Type-I-Seesaw-like mechanism. | result 0.75 | 0.80 | 0.22 | asserted 1.00 |
| s4 | We show that this model can satisfy current bounds from neutrino oscillation data, the lepton flavor violation, the relic abundance of the dark matter, and the direct search for the dark matter. | result 0.98 | 0.89 | 0.48 | hedged possibility 0.50 |
| s5 | This model would be tested at future collider experiments and dark matter experiments. | future work 0.97 | 0.12 | 0.11 | hedged possibility 0.84 |
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The paper
Original abstract
We propose a new model where the Dirac mass term for neutrinos, the Majorana mass term for right-handed neutrinos, and the other new fermion masses arise via the spontaneous breakdown of the $U(1)_{B-L}$ gauge symmetry. The anomaly-free condition gives four sets of assignment of the B-L charge to new particles, and three of these sets have an associated global $U(1)_{DM}$ symmetry which stabilizes dark matter candidates. The dark matter candidates contribute to generating the Dirac mass term for neutrinos at the one-loop level. Consequently, tiny neutrino masses are generated at the two-loop level via a Type-I-Seesaw-like mechanism. We show that this model can satisfy current bounds from neutrino oscillation data, the lepton flavor violation, the relic abundance of the dark matter, and the direct search for the dark matter. This model would be tested at future collider experiments and dark matter experiments.
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References
How the literature uses it
41 arXiv papers cite this in 43 sentences
Papers citing it · 13 sentences without a confident label
Builds on it 1 paper
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In this work we continue these analyses by considering the classically conformal B–L model introduced originally in Refs. [ref] and further studied in Refs. [ref] [We refer the reader to Refs. [ref] for analyses of non-conformal B–L models.].
Phase transition and vacuum stability in the classically conformal B-L model · Introduction · 0.81
Cites it as background 29 papers
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Thus a vast literature has recently arisen along this idea [ref] .
An Extended Colored Zee-Babu Model · Introduction · 0.97
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The above idea of DM-generated neutrino mass has been extensively exploited in the literature [ref] .
Radiative Neutrino Mass with $Z_3$ Dark matter: From Relic Density to LHC Signatures · Introduction · 0.95
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This is because a vast literature has recently arisen along thought of this subject [ref] .
Radiative Seesaw in Minimal 3-3-1 Model · Introduction · 0.88
What it cites · 3 sentences without a confident label
Uses data or values from 1 paper
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Even for a maximal mixing $cosθ_0 = 1/√(2)$, the observed abundance of the dark matter [ref] requires $v_σ^ ≲10$.
Planck 2013 results. XVI. Cosmological parameters · Dark Matter · 0.97
Cites as background 2 papers
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A variety of models where the Dirac mass term for neutrinos is radiatively generated has been studied in Refs. [ref] (See also Ref. [ref] ).
Two loop Induced Dirac Neutrino Model and Dark Matters with Global $U(1)'$ Symmetry · Introduction · 0.97
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Collider phenomenology on the $(1)_$ gauge symmetry is discussed in e.g., Ref. [ref] .
Phenomenology of the minimal B-L extension of the Standard Model at the LHC · Introduction · 0.99
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