{"arxiv_id":"1012.1597","incoming":{"papers":11,"sentences":15,"groups":[{"kind":"background","label":"Cites it as background","papers":1,"sentences":1,"quotes":[{"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":14},"outgoing":{"papers":40,"sentences":108,"groups":[{"kind":"extends","label":"Builds on","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1009.0003","title":"Supersymmetric Leptogenesis","url":"/paper/1009.0003","section":"Chemical equilibrium conditions and conservation laws","sentence":"Let us note at this point that the $3×5$ submatrix $A_ℓ_αb$ for the lepton densities represents the generalization of the $A$ matrix introduced in [ref] , $A_H̃_u b$ generalizes the Higgs $C$-vector first introduced in [ref] , and $A_g̃ b$ generalizes the $C$-vector for the gauginos first introduced in [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"hep-ph/9911315","title":"Baryogenesis through leptogenesis","url":"/paper/hep-ph/9911315","section":"Chemical equilibrium conditions and conservation laws","sentence":"Let us note at this point that the $3×5$ submatrix $A_ℓ_αb$ for the lepton densities represents the generalization of the $A$ matrix introduced in [ref] , $A_H̃_u b$ generalizes the Higgs $C$-vector first introduced in [ref] , and $A_g̃ b$ generalizes the $C$-vector for the gauginos first introduced in [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"hep-ph/0512052","title":"On Higgs and sphaleron effects during the leptogenesis 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the so called Purely Flavoured Leptogenesis (PFL) scenarios [ref] where the vanishing of the total CP asymmetry resulting from the sum over lepton flavours $ϵ=∑_αϵ_α=0$ ($α=e,μ,τ$) does not imply a vanishing baryon asymmetry $ΔB∝∑_αη_αϵ_α≠0$.","intent_p":0.84,"contests_p":null},{"arxiv_id":"hep-ph/0601084","title":"The importance of flavor in leptogenesis","url":"/paper/hep-ph/0601084","section":"Introduction","sentence":"This situation is reminiscent of the so called Purely Flavoured Leptogenesis (PFL) scenarios [ref] where the vanishing of the total CP asymmetry resulting from the sum over lepton flavours $ϵ=∑_αϵ_α=0$ ($α=e,μ,τ$) does not imply a vanishing baryon asymmetry $ΔB∝∑_αη_αϵ_α≠0$.","intent_p":0.84,"contests_p":null},{"arxiv_id":"1009.0003","title":"Supersymmetric Leptogenesis","url":"/paper/1009.0003","section":"Boltzmann Equations","sentence":"that, incidentally, coincides with the matrix given in [ref] for the case of all Yukawa couplings in equilibrium.","intent_p":0.96,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0707.0378","title":"CP violation in scatterings, three body processes and the Boltzmann equations for leptogenesis","url":"/paper/0707.0378","section":"Boltzmann Equations","sentence":"Fortunately, in the strong washout regime for leptogenesis, the effects of CP asymmetries in scattering have been found to be subdominant with respect to CP asymmetries in decays [ref] , and since in this paper we focus precisely on strong washouts, neglecting the scattering CP asymmetries is justified.","intent_p":1.0,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":13,"sentences":15,"quotes":[{"arxiv_id":"1009.0003","title":"Supersymmetric Leptogenesis","url":"/paper/1009.0003","section":"Chemical equilibrium conditions and conservation laws","sentence":"The set of conditions that constrain the particle abundances at 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specific to supersymmetry known as `soft leptogenesis' [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"hep-ph/0407063","title":"New Ways to Soft Leptogenesis","url":"/paper/hep-ph/0407063","section":"Vanishing of the CP asymmetry in decay","sentence":"The new sources of direct CP violation from vertex corrections involving the gauginos were first introduced in soft leptogenesis in [ref] .","intent_p":0.9,"contests_p":null}]}],"unlabelled_sentences":83},"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/1012.1597"}}