{"arxiv_id":"hep-ph/0512068","incoming":{"papers":23,"sentences":28,"groups":[{"kind":"data_used","label":"Uses its data or values","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2404.09021","title":"Is Doublet-Triplet Splitting Necessary?","url":"/paper/2404.09021","section":"Cutoff Scale Limit","sentence":"Also, a model [ref] that $(i)$ uses perturbative couplings to generate neutrino masses, $(ii)$ relies on operators of Eq. [ref] to generate charged fermion masses, and $(iii)$ implements Eqs. [ref], [ref], and [ref] to suppress gauge mediated proton decay signatures, yields $α_GUT^-1=37.1$ and $y_t=0.42$, where $α_GUT$ is evaluated via the two-loop level gauge coupling unification analysis, whereas $y_t$, at $M_GUT$, is obtained through the one-loop level renormalisation group equation running.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1412.1894","title":"Unified dark matter with intermediate symmetry breaking scales","url":"/paper/1412.1894","section":"Phenomenological Constraints","sentence":"In some works such as [ref] the SU(5) scale is as low as $M_X$ $≈$ $4 ×10^15$ after the addition of extra Higgs multiplets.","intent_p":0.83,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2403.04644","title":"Leptoquark-Mediated Two-Loop Neutrino Mass in Unified Theory","url":"/paper/2403.04644","section":"Numerical analysis and results","sentence":"Unlike existing models that rely on non-colored multiplets (all tree-level neutrino mass models Refs. [ref] as well as radiative neutrino mass models Refs. [ref] ), ours operates at two-loop order, resulting in a unique implication: a set of leptoquarks remains light.","intent_p":0.9,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":5,"sentences":5,"quotes":[{"arxiv_id":"2403.04644","title":"Leptoquark-Mediated Two-Loop Neutrino Mass in Unified Theory","url":"/paper/2403.04644","section":"Introduction","sentence":"There have been numerous efforts to endow neutrinos with non-zero masses (see, for example, Refs. [ref] , where neutrinos get their masses at the tree-level, and Refs. [ref] , where neutrino masses appear at the loop level[For original radiative neutrino mass models, see Refs. [ref] .]).","intent_p":0.97,"contests_p":null},{"arxiv_id":"1202.0807","title":"Seesaw Scale in the Minimal Renormalizable SO(10) Grand Unification","url":"/paper/1202.0807","section":"The tree-level scalar spectrum","sentence":"Hence, as such, the tree-level Higgs spectrum is clearly unable to support the physically interesting breaking patterns with either $ω_BL≪ω_R$ or $ω_R≪ω_BL$, thus avoiding the intermediate flipped $SU(5)' ⊗U(1)_Z'$ stage. $SU(5)$ intermediate stages, $ω_BL, ω_R ≪σ$, are disfavoured as well[Recently, there were several attempts to reconcile the simplest non-SUSY $SU(5)$ scenarios with the gauge unification by means of intermediate-scale thresholds, see, e.g., [ref] and references therein.","intent_p":0.87,"contests_p":null},{"arxiv_id":"2504.16022","title":"Non-Renormalizable SU(5) GUTs: Leptoquark-Induced Neutrino Masses","url":"/paper/2504.16022","section":"Introduction","sentence":"(For alternative approaches to the proton decay suppression of interest, see Refs. [ref] .)","intent_p":0.93,"contests_p":null},{"arxiv_id":"1807.09769","title":"Axion mass prediction from minimal grand unification","url":"/paper/1807.09769","section":"Introduction","sentence":"Although we exemplified our predictions in the case of the WGG+$24_F$ model, it would be interesting to compare axion properties in other minimal extensions of the WGG model which can simultaneously address neutrino masses and gauge coupling unification (see e.g. [ref] ), or in realistic SO(10) models [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"2103.11702","title":"Novel Leptoquark Pair Production at LHC","url":"/paper/2103.11702","section":"Introduction","sentence":"For example, scalar leptoquarks can generate neutrino masses [ref] , produce observable shifts in anomalous magnetic moments of charged leptons [ref] , provide a source of gauge coupling unification [ref] , and/or accommodate the $B$-physics anomalies [ref] .","intent_p":0.82,"contests_p":null}]}],"unlabelled_sentences":20},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/hep-ph/0512068"}}