{"arxiv_id":"hep-ph/0402267","incoming":{"papers":21,"sentences":33,"groups":[{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1102.5530","title":"Cosmology with Mirror Dark Matter","url":"/paper/1102.5530","section":"Mirror baryons as cosmological dark matter","sentence":"In particular, various baryogenesis scenarios with a hidden sector [ref] [ref] support a mirror baryonic density at least equal to the ordinary one.[ As far as the two sectors have the same particle physics, it is natural to think that the mirror baryon number density $n'_b$ is determined by the baryogenesis mechanism which is similar to the one which fixes the ordinary baryon density $n_b$.","intent_p":0.97,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":19,"sentences":22,"quotes":[{"arxiv_id":"2210.11011","title":"Exploring the cosmological dark matter coincidence using infrared fixed points","url":"/paper/2210.11011","section":"Introduction","sentence":"This generally leads to models of mirror matter, where the mirror symmetry is either exact [ref] or judiciously broken [ref] (For other models of mirror matter, see Refs. [ref] ). * introduce new field content so that the running gauge couplings $α_s$ and $α_d$ approach infrared fixed points with similar magnitudes.","intent_p":0.87,"contests_p":null},{"arxiv_id":"2404.05999","title":"Explaining the cosmological dark matter coincidence in asymmetric dark QCD","url":"/paper/2404.05999","section":"Introduction","sentence":"The main approach to this problem is to introduce a dark QCD-like gauge group $SU(N_d)$ and some mechanism that relates the confinement scale $Λ_dQCD$ to the QCD confinement scale $Λ_QCD$; the DM candidate in these models is thus a dark baryon whose mass is similar to the proton mass [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"2209.08257","title":"Asymmetric Mediator in Scotogenic Model","url":"/paper/2209.08257","section":"Introduction","sentence":"Asymmetric dark matter (ADM) [ref] is one of the frameworks where the coincidence between the relic abundances of the DM and baryon is realized.","intent_p":0.95,"contests_p":null},{"arxiv_id":"1811.05999","title":"Displaced Lepton Jet Signatures from Self-Interacting Dark Matter Bound States","url":"/paper/1811.05999","section":"The SIDM model","sentence":"We consider an SIDM scenario, where a fermionic dark matter particle ($χ$) couples to a dark photon ($Z_d$) with mass $m_Z_d$ and kinetic mixing $ϵ_Z_d$ to the SM photon [ref] , [equation] The dark photon $Z_d$ mediates dark matter self-interactions and bind dark matter particles into a bound state.","intent_p":0.81,"contests_p":null},{"arxiv_id":"2409.16095","title":"Low-scale Mirror Standard Model Dark Matter and its Detection via Gravitational Waves and the Guitar Nebula","url":"/paper/2409.16095","section":"Introduction","sentence":"Regarding DM, there is a not so well popular class of DM theories, which have incredibly interesting phenomenological features, the mirror DM theories firstly introduced in [ref] and further developed in Refs. [ref] see also Refs. [ref] for further applications.","intent_p":0.98,"contests_p":null}]}],"unlabelled_sentences":10},"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/0402267"}}