{"arxiv_id":"hep-ph/0506296","incoming":{"papers":184,"sentences":258,"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":"extends","label":"Builds on it","papers":4,"sentences":5,"quotes":[{"arxiv_id":"1206.3516","title":"Phenomenology of the minimal supersymmetric $U(1)_{B-L}\\times U(1)_R$ extension of the standard model","url":"/paper/1206.3516","section":"Introduction","sentence":"This latter possibility is the case we have studied in a previous paper [ref] using the minimal $U(1)_B-L×U(1)_R$ models of [ref] .","intent_p":0.81,"contests_p":null},{"arxiv_id":"1107.3412","title":"Soft masses in SUSY SO(10) GUTs with low intermediate scales","url":"/paper/1107.3412","section":"Introduction","sentence":"We will construct variants of the models proposed in [ref] and will also consider a completely new model, in which $v_R$ can be brought down to the electro-weak scale with the help of an intermediate Pati-Salam scale [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1301.6085","title":"Supersymmetric SO(10) GUTs with sliding scales","url":"/paper/1301.6085","section":"Summary and conclusions","sentence":"We have discussed that one can not only construct sliding models in which an inverse or linear seesaw is consistent with GCU, as done in earlier work [ref] , but also all other known types of seesaws can, in principle, be found.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1705.06320","title":"Predictive Pati-Salam theory of fermion masses and mixing","url":"/paper/1705.06320","section":"The model","sentence":"More explicitly, the standard model fermions are written in component form as [equation] Notice that we have extended the fermion sector of the original Pati-Salam model [ref] by introducing three fermion singlets $S_i$, in order to implement inverse and/or linear seesaw mechanisms for the generation of light active neutrino masses [ref] .","intent_p":0.85,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":5,"sentences":6,"quotes":[{"arxiv_id":"1005.1377","title":"Type I and $new$ seesaw in left-right symmetric theories","url":"/paper/1005.1377","section":"$new$ seesaw in left-right symmetric theories","sentence":"The form of the mass matrix is same as in reference [ref] but the mechanism and the elements are different.","intent_p":1.0,"contests_p":null},{"arxiv_id":"2307.04840","title":"Dynamical scoto-seesaw mechanism with gauged $B-L$","url":"/paper/2307.04840","section":"Dynamical scoto-seesaw mechanism","sentence":"At this point we also stress that, in contrast to low-scale inverse [ref] or linear seesaw schemes [ref] , the presence of TeV-scale neutrino-mass-mediators does not require the addition of extra gauge singlets beyond the “right-handed neutrinos”.","intent_p":0.88,"contests_p":null},{"arxiv_id":"2304.06080","title":"Large lepton number violation at colliders: predictions from the minimal linear seesaw mechanism","url":"/paper/2304.06080","section":"Introduction","sentence":"In contrast to most previous formulations [ref] , here we assume just the minimal gauge structure.","intent_p":0.85,"contests_p":null},{"arxiv_id":"1908.09587","title":"Electroweak Breaking and Higgs Boson Profile in the Simplest Linear Seesaw Model","url":"/paper/1908.09587","section":"Basic Theory Setup","sentence":"Notice that, in contrast to the original left-right symmetric formulations [ref] , here we realize the linear seesaw mechanism just in terms of the standard gauge structure, having the existence of the majoron as its characteristic feature.","intent_p":0.87,"contests_p":null},{"arxiv_id":"2305.00994","title":"Phenomenology of the simplest linear seesaw mechanism","url":"/paper/2305.00994","section":"Introduction","sentence":"In contrast to most previous formulations [ref] , here we do not impose left-right symmetry.","intent_p":0.81,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":94,"sentences":105,"quotes":[{"arxiv_id":"1709.04012","title":"Exploring the supersymmetric U(1)$_{B-L} \\times$ U(1)$_{R}$ model with dark matter, muon $g-2$ and $Z^\\prime$ mass limits","url":"/paper/1709.04012","section":"Introduction","sentence":"In [ref] , an extended supersymmetric model based on $SU(3)_c ×SU(2)_L ×U(1)_R ×U(1)_B-L$ was proposed.","intent_p":0.89,"contests_p":null},{"arxiv_id":"2312.13417","title":"The Minimal Massive Majoron Seesaw Model","url":"/paper/2312.13417","section":"The Low-Scale Seesaw models","sentence":"Two popular models in this scenario are the ones obtained by setting $ϵm_S=μ'=0$, dubbed as Inverse Seesaw (ISS) [ref] or by imposing $μ=μ'=0$, dubbed as Linear Seesaw (LSS) [ref] , that predict the following active neutrino masses respectively m_ν^ISS≃- μ m_N m_N^TΛ_NS^2 , m_ν^LSS≃- ϵ m_S m_N^T + m_N m_S^TΛ_NS .","intent_p":0.87,"contests_p":null},{"arxiv_id":"1409.1868","title":"Neutrinos with a linear seesaw mechanism in a scenario of gauged B-L symmetry","url":"/paper/1409.1868","section":"Introduction","sentence":"Instead, if the small parameter is the block $[M^(ν)]_13 ≡ε$, the model is called linear Seesaw [ref] , because the light neutrino masses are linear in $m_D$, of order $m_ν∼ε m_D/M_R$.","intent_p":0.82,"contests_p":null},{"arxiv_id":"1709.01737","title":"$A_4$ realization of Linear Seesaw and Neutrino Phenomenology","url":"/paper/1709.01737","section":"Introduction","sentence":"Depending on the position of the zero elements in the mass matrix in the basis $(ν, N_R, S)$, active neutrinos receive masses through two different mechanisms called inverse seesaw [ref] and linear seesaw [ref] .","intent_p":0.9,"contests_p":null},{"arxiv_id":"2408.13232","title":"Non-unitary limits on different textures for low-scale seesaw models","url":"/paper/2408.13232","section":"Introduction","sentence":"This work will focus on the low-scale type-I seesaw mechanism, specifically the linear [ref] and inverse models [ref] [For readers interested in a thorough analysis of the Type-I Seesaw family of neutrino models, see reference [ref] .].","intent_p":0.9,"contests_p":null}]}],"unlabelled_sentences":141},"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/0506296"}}