Recognition: unknown
Dirac one-loop seesaw in a non-invertible fusion rule
Pith reviewed 2026-05-10 16:28 UTC · model grok-4.3
The pith
A non-invertible fusion rule from Z3 x Z3' gauging forces Dirac neutrino masses to arise only at one loop while stabilizing a dark matter candidate.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We propose a radiative Dirac neutrino mass model stabilized by a non-invertible fusion rule originating from a Z3 × Z3' gauging. The imposed symmetry forbids tree-level Yukawa couplings and ensures that neutrino masses are generated only at the one-loop level through the exchange of exotic fermions and inert scalars. This minimal framework simultaneously accommodates neutrino masses and mixings consistent with current oscillation data, while providing a viable dark matter candidate. We analyze lepton flavor violating processes and lepton anomalous magnetic moments, finding that all contributions remain well below present experimental bounds. In the dark matter sector, the bosonic singlet is
What carries the argument
The non-invertible fusion rule arising from Z3 × Z3' gauging, which functions as a selection rule that eliminates all tree-level Yukawa operators while permitting specific one-loop diagrams involving exotic fermions and inert scalars.
If this is right
- Neutrino oscillation parameters are reproduced by the one-loop mass matrix while satisfying all current bounds.
- Lepton-flavor-violating branching ratios and anomalous magnetic moments lie well below experimental limits across the viable parameter space.
- The bosonic singlet provides the correct thermal relic density, whereas the corresponding fermionic state is excluded by suppressed annihilation.
- The exotic fermions and inert scalars remain light enough to be produced at future colliders.
Where Pith is reading between the lines
- Similar non-invertible rules could be applied to other sectors to suppress unwanted operators without introducing new mass scales.
- Precision measurements of neutrino mixing angles at next-generation oscillation experiments could distinguish this one-loop pattern from tree-level alternatives.
- Direct searches for the inert scalars or exotic fermions at the LHC or future colliders would provide an independent test independent of neutrino data.
Load-bearing premise
The non-invertible fusion rule must be realized exactly so that it removes every tree-level Yukawa coupling yet still allows the chosen one-loop diagrams to generate the observed neutrino masses without extra suppression.
What would settle it
A direct measurement showing that the bosonic singlet cannot achieve the observed relic density for any parameter choice consistent with the one-loop neutrino mass, or the discovery that tree-level Yukawa couplings are present despite the gauged symmetry.
Figures
read the original abstract
We propose a radiative Dirac neutrino mass model stabilized by a non-invertible fusion rule originating from a $Z_3 \times Z_3'$ gauging. The imposed symmetry forbids tree-level Yukawa couplings and ensures that neutrino masses are generated only at the one-loop level through the exchange of exotic fermions and inert scalars. This minimal framework simultaneously accommodates neutrino masses and mixings consistent with current oscillation data, while providing a viable dark matter candidate. We analyze lepton flavor violating processes and lepton anomalous magnetic moments, finding that all contributions remain well below present experimental bounds. In the dark matter sector, the bosonic singlet emerges as a promising candidate with relic density compatible with cosmological observations, whereas the fermionic option is strongly disfavored due to suppressed annihilation cross sections. Our study demonstrates that non-invertible fusion rules can serve as a powerful organizing principle for constructing minimal and phenomenologically consistent extensions of the Standard Model, linking neutrino physics and dark matter within a unified radiative framework.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes a radiative Dirac neutrino mass model stabilized by a non-invertible fusion rule from Z_3 × Z_3' gauging. The symmetry is claimed to forbid all tree-level Yukawa couplings, generating neutrino masses at one loop via exotic fermions and inert scalars. The framework is asserted to accommodate neutrino oscillation data, keep lepton flavor violation and g-2 contributions below experimental bounds, and yield a viable bosonic singlet dark matter candidate with the correct relic density (while disfavoring the fermionic option).
Significance. If the fusion rules rigorously enforce the absence of tree-level operators while permitting the specified one-loop topology, the work illustrates a potentially useful organizing principle for minimal SM extensions that simultaneously address neutrino masses and dark matter. The approach is novel in its application of non-invertible symmetries, but its significance hinges on explicit verification of the symmetry constraints and the robustness of the phenomenological fits.
major comments (2)
- [Abstract] Abstract: the central claim that the Z_3 × Z_3' non-invertible fusion rule forbids every tree-level Dirac Yukawa coupling (while allowing the one-loop diagram) is load-bearing for the entire radiative construction. The manuscript must explicitly list the charge assignments for L, H, N, the exotic fermions, and inert scalars, then compute the fusion products to demonstrate that no dimension-4 operator fuses to the identity.
- [Model construction] Model construction (likely §2–3): without the explicit fusion-rule verification above, the assertions that neutrino masses arise only radiatively, that DM stability is protected, and that LFV is suppressed all rest on an unconfirmed symmetry condition. If even one Yukawa term is allowed, the one-loop seesaw claim collapses.
minor comments (1)
- The abstract states consistency with oscillation data and relic density but provides no numerical values, loop integrals, or parameter ranges; including a brief table of benchmark points would improve clarity.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for highlighting the need for explicit verification of the symmetry constraints. We address the major comments point by point below and will incorporate the requested details in a revised version.
read point-by-point responses
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Referee: [Abstract] Abstract: the central claim that the Z_3 × Z_3' non-invertible fusion rule forbids every tree-level Dirac Yukawa coupling (while allowing the one-loop diagram) is load-bearing for the entire radiative construction. The manuscript must explicitly list the charge assignments for L, H, N, the exotic fermions, and inert scalars, then compute the fusion products to demonstrate that no dimension-4 operator fuses to the identity.
Authors: We agree that an explicit demonstration is required to substantiate the central claim. In the revised manuscript we will add a new subsection (in §2) that lists the Z_3 × Z_3' charge assignments for all relevant fields—lepton doublets L, the Higgs H, right-handed neutrinos N, the exotic fermions, and the inert scalars. We will then compute the fusion products of every possible dimension-4 operator and show that none fuse to the identity, while the operators appearing in the one-loop diagram are permitted. This addition will make the symmetry argument fully transparent and directly support the statements in the abstract. revision: yes
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Referee: [Model construction] Model construction (likely §2–3): without the explicit fusion-rule verification above, the assertions that neutrino masses arise only radiatively, that DM stability is protected, and that LFV is suppressed all rest on an unconfirmed symmetry condition. If even one Yukawa term is allowed, the one-loop seesaw claim collapses.
Authors: We acknowledge that the radiative nature of the neutrino masses, the stability of the dark-matter candidate, and the suppression of lepton-flavor violation all rely on the fusion rules being correctly enforced. The explicit calculations described in the response to the first comment will be placed in §2 and cross-referenced in §3. With these verifications in place, the revised text will confirm that no tree-level Yukawa operator is allowed, that the bosonic singlet remains stable, and that tree-level LFV contributions are absent. The one-loop topology remains the leading contribution, preserving the overall phenomenological conclusions. revision: yes
Circularity Check
No significant circularity; explicit symmetry construction checked against data
full rationale
The paper constructs a model by imposing a non-invertible fusion rule from Z3 × Z3' gauging that is stated to forbid all tree-level Yukawa operators while permitting a specific one-loop diagram involving exotic fermions and inert scalars. Neutrino masses/mixings, LFV rates, g-2 contributions, and DM relic density are then shown to be compatible with data via suitable parameter choices in the allowed Lagrangian. This is standard model-building: the symmetry assignments and fusion products are presented as the defining input, the one-loop topology follows directly from the charge rules, and numerical scans confirm viability without claiming parameter-free predictions or deriving the symmetry from the observables themselves. No load-bearing step reduces by construction to a fit, self-citation chain, or renamed ansatz; the central result (viability of the radiative framework) remains independent of the fitted values.
Axiom & Free-Parameter Ledger
free parameters (1)
- masses and couplings of exotic fermions and inert scalars
axioms (1)
- domain assumption Z3 x Z3' gauging produces a non-invertible fusion rule that forbids tree-level Yukawa couplings.
invented entities (2)
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exotic fermions and inert scalars
no independent evidence
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bosonic singlet
no independent evidence
Forward citations
Cited by 1 Pith paper
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A theoretical account of tiny multi-Higgs vacuum expectation values from non-invertible symmetry
Non-invertible symmetry from the minimal Fibonacci fusion rule forbids tree-level VEVs for multi-Higgs fields H4 and H5, generating them radiatively at one-loop with naturally small values of 10^{-3}-10^{-2} GeV that ...
Reference graph
Works this paper leans on
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Bosonic DM case:Sstate SinceSdoes not couple to Standard Model fields through Yukawa interactions, its only portal to the visible sector arisesviascalar interactions in the Higgs potential. In such a 8 case, detailed analysis is already explored, and the correct relic density of DM is obtained near the half of Higgs mass by the resonant enhancement [89] w...
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[2]
Then, the mass ofXis given byM ψ1
Fermionic DM case:ψ 1 state The lightest exotic fermionψ 1 is stabilized by the non-invertible symmetry. Then, the mass ofXis given byM ψ1. SinceXdoes not directly couple to quark sector, we can neglect the constraints of direct detection searches. The relevant annihilation processes areX ¯X→ℓ i ¯ℓj(νσ¯νρ) and they are s-wave dominant due to the Dirac fer...
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[3]
Bosonic DM:Sstate In case of bosonic DM, we impose the following condition ˜m1 ≤1.2×( ˜Mψ1,˜m2).(38) where 1.2 is roughly evaluated by suppressing co-annihilation cross sections [92]. Fig. 2, we show the allowed regions of ˜m1,2 (left-up panel), ˜Mψ1,2 (right-up panel),|f 33|−|g 33| (left-down panel), andP Dν −|κν|in meV unit (right-down panel), respectiv...
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[4]
Fermionic DM:ψ 1 state In case of fermionic DM, we impose the following condition ˜Mψ1 ≤1.2×( ˜Mψ2,˜m1,˜m2).(39) where 1.2 is rough estimation to suppress the co-annihilation cross sections. Fig. 4, we show the allowed regions of ˜m1,2 (left-up panel), ˜Mψ1,2 (right-up panel),|f 33|−|g 33| (left-down panel), and P Dν − |κν|in meV unit (right-down panel), ...
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[5]
The corresponding 14 FIG
Bosonic DM:Sstate Table II lists the BP that minimizes ∆χ 2, where our DM is fixed to be half of the SM Higgs mass∼63 GeV and the resulting minimum value is approximately 0.200. The corresponding 14 FIG. 6: Allowed region of the DM cross section to explain the relic density in terms of DM mass. All the color legends and the line are the same as the ones i...
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The resulting minimum value is approximately 0.148
Fermionic DM:ψ 1 state Table III lists the BP that minimizes ∆χ 2. The resulting minimum value is approximately 0.148. The corresponding values for ˜gand ˜fare also provided as follows: ˜g×103 ≈ 75.3899−79.9135i−1.10263 + 0.0792865i0.0115587−0.0801839i −7.77716 + 26.6837i−459.569−3588.96i−2.9311 + 11.6813i 0.0249052 + 0.108523i8.89349 + 16.6716i10 ...
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The model is consistent with current neutrino oscillation data, including NuFit 6.1 and JUNO constraints
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Lepton flavor violating processes such asµ→eγremain well below experimental bounds
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Contributions to the lepton anomalous magnetic moments are small, ensuring com- patibility with precision measurements
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The bosonic singletSemerges as a promising DM candidate, while the fermionic option is strongly disfavored due to insufficient annihilation cross sections.. The significance of this work lies in demonstrating that non-invertible fusion rules can serve as a powerful organizing principle for constructing minimal and phenomenologically viable extensions of t...
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