{"arxiv_id":"hep-ph/9901206","incoming":{"papers":119,"sentences":173,"groups":[{"kind":"contests","label":"Contests it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2009.03877","title":"Modified lepton couplings and the Cabibbo-angle anomaly","url":"/paper/2009.03877","section":"Results and Conclusions","sentence":"This result shows that current data clearly favours the NP hypothesis, exclude conventional models with right-handed neutrinos leading to necessary destructive interference [ref] and promote the search for NP models as the ones presented in Refs. [ref] .","intent_p":0.73,"contests_p":0.73}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1909.02331","title":"Generalised $\\mu$-$\\tau$ symmetries and calculable gauge kinetic and mass mixing in $U(1)_{L_\\mu-L_\\tau}$ models","url":"/paper/1909.02331","section":"Kinetic mixing in the standard seesaw model","sentence":"In this we closely follow the treatment of radiative corrections given in [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"2106.16226","title":"Mapping the viable parameter space for testable leptogenesis","url":"/paper/2106.16226","section":"Introduction","sentence":"In our study of the parameter space we employ the usual Casas-Ibarra parametrization [ref] , [equation] where $U_ν$ is the PMNS matrix, $m_ν$ and $M_M$ are the mass matrices of the light and heavy neutrinos respectively.[ This parametrization can be modified to include radiative corrections [ref] by replacing $√(M_i) →M_i/√(M̃_i)$ [ref] , as well corrections from unitarity of the mixing matrix [ref] . ] The matrix $ℛ$ satisfies $ℛ ℛ^T=1$ and is usually parametrized by three complex Euler angles.","intent_p":1.0,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1712.07611","title":"Equivalence between massless neutrinos and lepton number conservation in fermionic singlet extensions of the Standard Model","url":"/paper/1712.07611","section":"The matrix $M$ as a necessary condition for massless light neutrinos: $M̂_l = 0 M$","sentence":"We computed the one-loop induced mass for neutrinos and found it to agree with [ref] , giving [equation] with $i,j ∈{ 1, 2, 3 }$, $α_W = g^2/4 π$ with $g$ the $SU(2)_L$ coupling constant, [equation] [equation] and [equation] where [equation] As $f(0)=0$, it is useful to define a diagonal matrix [equation] such that eq.([ref]) may be rewritten in matrix form as [equation]","intent_p":0.99,"contests_p":null},{"arxiv_id":"1903.07590","title":"Neutrino Masses from a Dark Neutrino Sector below the Electroweak Scale","url":"/paper/1903.07590","section":"Radiative corrections","sentence":"Turning off the $g^'$ gauge coupling, we recover the expression for the Type-I seesaw case [ref] : [equation]","intent_p":0.81,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":3,"sentences":3,"quotes":[{"arxiv_id":"2312.11165","title":"Testing Leptogenesis and Seesaw using Long-lived Particle Searches in the $B-L$ Model","url":"/paper/2312.11165","section":"Introduction","sentence":"If their decay can be detected, e.g., in LLP searches, we can probe the seesaw floor in a much broader range [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1711.02180","title":"Lepton Number Violation: Seesaw Models and Their Collider Tests","url":"/paper/1711.02180","section":"The Canonical Type I Seesaw Mechanism","sentence":"This leads to the well-known decoupling of observable lepton number violation in the minimal, high-scale Type I Seesaw scenario at colliders experiments [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1706.08524","title":"From the trees to the forest: a review of radiative neutrino mass models","url":"/paper/1706.08524","section":"Other 1-loop models","sentence":"This has been explicitly shown in Ref. 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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. 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A later paper is listed under a label only when the classifier gives one of its sentences that label at intent probability 0.8 or more (0.95 for support), Pith's reading of the sentence finds that the citing paper itself did it, and a second check of the paraphrase against the sentence passes. The section lists uses only: building on the paper, using its method, tool, data or values, comparing with it and citing it as support. It does not list criticism or disagreement, so their absence says nothing about how the paper has been received. Code counted the papers, wrote the summary from the listed entries, set the evidence level and linked each entry to its citing paper. Quotes are copied from the citing sentence and shown only when the citing paper's licence is CC BY, CC BY-SA or CC0; otherwise the paraphrase is shown. Papers that share an author with this one are listed apart. A paper with fewer citing papers gets a line counted by code, which names uses only: a later paper whose only label is a contest is counted as not described.","line":null,"summary":"2 later papers by other authors are listed below: 2 compared their own results with it."},"_links":{"html":"https://pith.science/paper/hep-ph/9901206"}}