{"arxiv_id":"hep-ph/0308031","incoming":{"papers":25,"sentences":89,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":3,"sentences":4,"quotes":[{"arxiv_id":"2211.00422","title":"PeV-scale leptogenesis, gravity waves and black holes from a SUSY-breaking phase transition","url":"/paper/2211.00422","section":"CP asymmetry","sentence":"Using the resummation approach for unstable particle propagators described in [ref] , the one-loop amplitude for the sneutrino decays $_i'→a_α$, with $a_α= _αH_u$ or $L_α_u$ is 𝒜̂^a_α_i = A_i^a_α - i ∑_j≠i A_j^a_α Σ^_ji/p^2-M_j^2+iΣ^_jj In this expression, $A_i^a_α$ is the tree-level amplitude of the $_i'→a_α$ decay and $Σ_ji^$ is the absorptive part of the $_i'→_j'$ self-energy, which we evaluated with the Cutkosky rules [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"0901.0008","title":"On Gaugino Contributions to Soft Leptogenesis","url":"/paper/0901.0008","section":"CP Asymmetry in Quantum Mechanics","sentence":"In this section we recompute the asymmetry using a quantum mechanical (QM) approach, based on an effective (non hermitic) Hamiltonian [ref] .","intent_p":0.88,"contests_p":null},{"arxiv_id":"0905.4834","title":"On the full Boltzmann equations for Leptogenesis","url":"/paper/0905.4834","section":"Approximated Boltzmann Equations","sentence":"One possibility, which was used in [ref] and [ref] , is to neglect all the thermal corrections except for the ones that are crucial to get a non vanishing CP asymmetry, which are evaluated in the approximation of decay at rest of the heavy sneutrinos.","intent_p":0.98,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1007.3323","title":"Soft Leptogenesis and Gravitino Dark Matter in Gauge Mediation","url":"/paper/1007.3323","section":"Soft Leptogenesis","sentence":"The maximum value of $η$ is $𝒪(0.1)$ for $m_1 ≃10^-(3-4)eV$ [ref] , where [equation] and $v=174 GeV$ is the vacuum expectation value of Higgs.","intent_p":0.81,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":5,"sentences":5,"quotes":[{"arxiv_id":"0710.3905","title":"The (ir)Relevance of Initial Conditions in Soft Leptogenesis","url":"/paper/0710.3905","section":"Lepton Asymmetries","sentence":"This agrees with [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1911.03363","title":"Soft leptogenesis in the NMSSM with a singlet right-handed neutrino superfield","url":"/paper/1911.03363","section":"$Ñ$ decays","sentence":"We also note that while the usual soft leptogenesis done in the MSSM [ref] , to the leading order in soft terms ($M^2≪M_1^2, A_N^2≪M_1^2$), necessarily requires thermal phase space factors for the final state bosons ($c_B$) and fermions ($c_F$) to have $ε∝Δ_BF=c_B-c_F/c_B+c_F$, we get an asymmetry even without thermal mass corrections to the decay products at the leading order in soft terms.","intent_p":1.0,"contests_p":null},{"arxiv_id":"2211.00422","title":"PeV-scale leptogenesis, gravity waves and black holes from a SUSY-breaking phase transition","url":"/paper/2211.00422","section":"CP asymmetry","sentence":"This is to be contrasted with the standard case of soft leptogenesis where bosonic and fermionic decay channels have opposite CP asymmetry and leptogenesis requires thermal effects to avoid exact cancellation between them [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"0905.4834","title":"On the full Boltzmann equations for Leptogenesis","url":"/paper/0905.4834","section":"Results and discussion","sentence":"In the case $K=0.1$, we observe (in agreement with [ref] ) the flipping of the lepton asymmetry sign when the bosonic channel is open, both in the full (solid blue) and in the approximated calculations.","intent_p":0.86,"contests_p":null},{"arxiv_id":"0804.4471","title":"Flavoured Soft Leptogenesis","url":"/paper/0804.4471","section":"The Boltzmann Equations","sentence":"Our results show good agreement with those in Refs. [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":12,"sentences":17,"quotes":[{"arxiv_id":"1007.3323","title":"Soft Leptogenesis and Gravitino Dark Matter in Gauge Mediation","url":"/paper/1007.3323","section":"Introduction","sentence":"Soft leptogenesis [ref] is an attractive way of generating baryon asymmetry.","intent_p":0.91,"contests_p":null},{"arxiv_id":"0710.3905","title":"The (ir)Relevance of Initial Conditions in Soft Leptogenesis","url":"/paper/0710.3905","section":"Definitions and Approximations","sentence":"As stated above, in this work we consider the Soft Leptogenesis scenario [ref] , which employs the minimal supersymmetric standard model plus singlet neutrino chiral superfields.","intent_p":0.88,"contests_p":null},{"arxiv_id":"1012.1597","title":"Early Universe effective theories: The Soft Leptogenesis and R-Genesis Cases","url":"/paper/1012.1597","section":"Soft leptogenesis: review and motivations","sentence":"This allows for a different leptogenesis scenario that is specific to supersymmetry known as `soft leptogenesis' [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"1107.5312","title":"Leptogenesis from Soft Supersymmetry Breaking (Soft Leptogenesis)","url":"/paper/1107.5312","section":"Final Remarks and Conclusions","sentence":"This scenario, termed soft leptogenesis [ref] (SL) has been the subject of this review.","intent_p":0.88,"contests_p":null},{"arxiv_id":"1911.03363","title":"Soft leptogenesis in the NMSSM with a singlet right-handed neutrino superfield","url":"/paper/1911.03363","section":"Introduction","sentence":"Soft leptogenesis [ref] pertains to generating lepton asymmetry at the tree-level itself due to mixing between the particle and anti-particle states of the RH singlet sneutrino, $Ñ$, because of the presence of soft SUSY breaking terms[Soft leptogenesis in different types of SUSY framework can be found in [ref] .].","intent_p":0.95,"contests_p":null}]}],"unlabelled_sentences":62},"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/0308031"}}