{"arxiv_id":"1207.3971","incoming":{"papers":50,"sentences":108,"groups":[{"kind":"contests","label":"Contests it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"1810.00033","title":"Faint Light from Dark Matter: Classifying and Constraining Dark Matter-Photon Effective Operators","url":"/paper/1810.00033","section":"Non-relativistic Operator Matching and Cross Sections","sentence":"An explicit expression is given in Appendix A of Ref. [ref] (which corrects a number of mistakes in the derivation of Ref. [ref] ).","intent_p":0.51,"contests_p":0.74},{"arxiv_id":"2105.12116","title":"Two-photon exchange in leptophilic dark matter scenarios","url":"/paper/2105.12116","section":"Conclusions","sentence":"Note, however, that by following the effective approach of Ref. 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[ref] , we compute the averaged per nucleon scattering cross-section with, [equation] where $A$ is the isotope-averaged number of nucleons, $μ_A=m_Am_ϕ, χ/(m_A+m_ϕ, χ)$ is the reduced mass (see Appendix A), the charge form factor $F_Ray(q̅)$ drops with rising momentum transfer.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1711.11376","title":"Model-independent analysis of the DAMPE excess","url":"/paper/1711.11376","section":"Dark matter direct detection","sentence":"We have checked that with the kinetic recoil energy of the nucleus $E_d∈[1,10]$ keV for Xenon, $F(q)$ lies in $[0.9995,0.9950]$ using formula in [ref] and $F̃(q)$ lies in $[0.9999,0.9998]$ using formula in [ref] .], [equation] where $α_em$ is the fine structure constant, $M$ is the mediator mass, $μ_N ≡m_N m_χ / (m_N+m_χ)$ is the reduced mass of the DM-nucleus two particle system, $v=0.001c$ is the velocity of the DM near the Earth, $μ$ is the scale at which the logarithmic divergence is cut off, $m_N$, $Z$ and $A$ are the target nucleus' mass, charge and mass number respectively.","intent_p":0.93,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1408.5046","title":"Dark matter direct detection constraints from gauge bosons loops","url":"/paper/1408.5046","section":"Loop-induced direct detection","sentence":"At zero-momentum transfer the corresponding form factor reads $f_F^N ≃0.08, 0.10$ and $0.12$ for xenon, germanium and argon targets, respectively [ref] .","intent_p":1.0,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":3,"sentences":6,"quotes":[{"arxiv_id":"2105.12116","title":"Two-photon exchange in leptophilic dark matter scenarios","url":"/paper/2105.12116","section":"Comparison with previous results and discussion","sentence":"We compare our result for the scalar mediator case to [ref]","intent_p":1.0,"contests_p":null},{"arxiv_id":"1503.04205","title":"Direct Detection of Stealth Dark Matter through Electromagnetic Polarizability","url":"/paper/1503.04205","section":"Introduction","sentence":"With the factor of $3$ in Eq. 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[ref] , there are examples where this large separation of scales has remarkable implications when a comparison with experiments is attempted.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1208.6082","title":"The 130 GeV Fingerprint of Right-Handed Neutrino Dark Matter","url":"/paper/1208.6082","section":"Introduction","sentence":"This was recently shown [ref] for an effective description of the $2γ$ vertex.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1702.02430","title":"Review of LHC Dark Matter Searches","url":"/paper/1702.02430","section":"Direct detection","sentence":"Indeed, it has been shown that renormalization group evolution can lead to important effects, in particular for models where the tree-level calculation predicts a strong suppression of the event rates [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"2011.04735","title":"Probing light dark scalars with future experiments","url":"/paper/2011.04735","section":"Introduction and framework","sentence":"In fact, it has been shown that, for vector currents, the renormalization group evolution of the effective operators from the scale $Λ$ to the scale of low energy experiments is small [ref] .","intent_p":0.98,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":18,"sentences":20,"quotes":[{"arxiv_id":"1807.03817","title":"Interplay of the LHC and non-LHC Dark Matter searches in the Effective Field Theory approach","url":"/paper/1807.03817","section":"Direct detection and Running effect of the EFT operators","sentence":"The first radiative effects to be considered were the QCD ones [ref] , while only later it has been realized that EW loops could be important as well [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"2006.12768","title":"Dark Matter Search at Colliders and Neutrino Floor","url":"/paper/2006.12768","section":"Introduction","sentence":"These loop effects or RGE effects have been widely studied assuming DM interacts with gauge bosons [ref] and with leptons [ref] .","intent_p":0.85,"contests_p":null},{"arxiv_id":"2105.12116","title":"Two-photon exchange in leptophilic dark matter scenarios","url":"/paper/2105.12116","section":"Conclusions","sentence":"Two-body one-loop processes had also been considered, under different approximations, in effective DM scenarios, where DM couples to photons through a Rayleigh-like operator [ref] .","intent_p":0.84,"contests_p":null},{"arxiv_id":"1503.04205","title":"Direct Detection of Stealth Dark Matter through Electromagnetic Polarizability","url":"/paper/1503.04205","section":"Introduction","sentence":"Various attempts to perturbatively estimate this matrix element have been performed with varying levels of complexity [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1401.2527","title":"Right Sneutrino Dark Matter and a Monochromatic Photon Line","url":"/paper/1401.2527","section":"Introduction","sentence":"Following reference [ref] , various models have been proposed to explain the monochromatic feature of the $γ$-ray, see e.g. [ref] .","intent_p":0.89,"contests_p":null}]}],"unlabelled_sentences":71},"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. 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A paper with fewer citing papers gets a line counted by code, which names uses only: a later paper whose only label is a contest is counted as not described.","line":null,"summary":"2 later papers by other authors are listed below: 1 used its method or tool and 1 compared its own results with it."},"_links":{"html":"https://pith.science/paper/1207.3971"}}