{"arxiv_id":"1305.7461","incoming":{"papers":23,"sentences":51,"groups":[{"kind":"extends","label":"Builds on it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2202.07830","title":"Higgsino Dark Matter in Pure Gravity Mediated Supersymmetry","url":"/paper/2202.07830","section":"Pure Gravity Mediation","sentence":"In this work, we examine a slightly more generic scenario with non-universal Higgs masses [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"1312.7108","title":"Flat Higgs Potential from Planck Scale Supersymmetry Breaking","url":"/paper/1312.7108","section":"Discussions","sentence":"It is also possible to extend this mechanism to more generic models in which the Higgs doublets emerge as Goldstone modes of approximate symmetries [ref] such as models with $SU(3)/SU(2)×U(1)$ [ref] .","intent_p":0.88,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1502.00034","title":"SU(5) Grand Unification in Pure Gravity Mediation","url":"/paper/1502.00034","section":"Results","sentence":"Note also that the Higgs masses calculated here differ slightly from those calculated in [ref] as here we are not imposing strict gauge coupling unification at the GUT scale.] for $tanβ$ roughly between 4–9 as shown by the red dot-dashed curves.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1602.04812","title":"Naturalizing Supersymmetry with a Two-Field Relaxion Mechanism","url":"/paper/1602.04812","section":"The MSSM sector","sentence":"Note, however, that the $A$-terms in this case are not suppressed by a loop factor contrary to other split-SUSY models based on anomaly mediation [ref] (see, for instance, Refs. 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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. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/1305.7461"}}