{"arxiv_id":"hep-ph/0305212","incoming":{"papers":39,"sentences":57,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1212.4476","title":"The Higgs Mass beyond the CMSSM","url":"/paper/1212.4476","section":"Impacts on mSUGRA models","sentence":"We recall that, there is just one free parameter in addition to these, which may be taken as $A_0$: the electroweak vacuum conditions ([ref], [ref]) may be used to determine $tanβ$ at each point on the plane [ref] .","intent_p":0.83,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1209.0499","title":"Strong moduli stabilization and phenomenology","url":"/paper/1209.0499","section":"GM Supergravity and Super-GUT phenomenology","sentence":"Indeed it is known [ref] that only a limited portion of parameter space (defined by $m_0, m_1/2$ and $A_0$) possesses solutions for $tanβ$. 2) There is no guarantee that solutions with $μ^2 > 0$ exist when $m_0$ is very large.","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":12,"sentences":14,"quotes":[{"arxiv_id":"1102.4585","title":"Implications of Initial LHC Searches for Supersymmetry","url":"/paper/1102.4585","section":"Introduction","sentence":"Therefore, we have focused on making estimates within the constrained MSSM (CMSSM) [ref] in which soft SUSY-breaking mass parameters are assumed to be universal at the GUT scale, in the simplest generalization of this model in which the universality is relaxed to allow non-universal Higgs masses (NUHM1) [ref] , in a very constrained model in which a supplementary relation is imposed on trilinear and bilinear soft SUSY-breaking masses (VCMSSM) [ref] , and in minimal supergravity (mSUGRA) in which, in addition, the gravitino mass $m_3/2$ is set equal to the common soft SUSY-breaking scalar mass $m_0$ before renormalization [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"0710.5311","title":"Gravitino Dark Matter and Light Element Adundances","url":"/paper/0710.5311","section":"Results and Discussion","sentence":"Our framework is CMSSM and mSUGRA models [ref] , where the NSP could be either the lighter stau or the lightest neutralino.","intent_p":0.88,"contests_p":null},{"arxiv_id":"1106.2529","title":"Supersymmetry and Dark Matter in Light of LHC 2010 and Xenon100 Data","url":"/paper/1106.2529","section":"Introduction","sentence":"Therefore, we have focused on making estimates within simplified versions of the MSSM, specifically the constrained MSSM (the CMSSM) [ref] in which soft SUSY-breaking mass parameters are assumed to be universal at the GUT scale, in the simplest generalization of this model in which the universality is relaxed to allow non-universal Higgs masses (the NUHM1) [ref] , in a very constrained model in which the supplementary relation $A_0 = B_0 + m_0$ [We recall that our convention [ref] for the sign of $A_0$ is opposite to that of SoftSUSY.] is imposed on trilinear and bilinear soft SUSY-breaking masses in the CMSSM (the VCMSSM) [ref] , and in minimal supergravity (mSUGRA) in which, in addition, the gravitino mass $m_3/2$ is set equal to the common soft SUSY-breaking scalar mass $m_0$ before renormalization [ref] .","intent_p":0.93,"contests_p":null},{"arxiv_id":"1902.09084","title":"A Minimal SU(5) SuperGUT in Pure Gravity Mediation","url":"/paper/1902.09084","section":"SuperGUT Pure Gravity Mediation","sentence":"In minimal PGM, the Kähler potential is assumed to be flat, and hence the soft scalar masses are universal and equal to the gravitino mass $m_3/2$, as in mSUGRA [ref] : [equation] On the other hand, the gaugino masses and $A$-terms vanish at tree level—such a situation is naturally obtained if there is no singlet SUSY breaking field and/or in models with strong moduli stabilization [ref] .","intent_p":0.85,"contests_p":null},{"arxiv_id":"0805.2943","title":"Modulus-dominated SUSY-breaking soft terms in F-theory and their test at LHC","url":"/paper/0805.2943","section":"Radiative EW symmetry breaking and experimental constraints","sentence":"The constraints imposed by the full REWSB conditions have been analysed for models with universal soft parameters [ref] , as well as string-inspired scenarios [ref] .","intent_p":0.93,"contests_p":null}]}],"unlabelled_sentences":41},"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/0305212"}}