{"arxiv_id":"1204.4722","incoming":{"papers":58,"sentences":81,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1302.2614","title":"Improved Electroweak Phase Transition with Subdominant Inert Doublet Dark Matter","url":"/paper/1302.2614","section":"Introduction","sentence":"[ref] for the analysis of the phase transition.","intent_p":1.0,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1504.05949","title":"The Electroweak Phase Transition in the Inert Doublet Model","url":"/paper/1504.05949","section":"Introduction","sentence":"Indeed, we will confirm the findings of Refs. [ref] that this is the only region of parameter space that can successfully saturate the DM abundance and provide a strong-enough first-order EWPT.","intent_p":0.97,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":35,"sentences":36,"quotes":[{"arxiv_id":"1504.05949","title":"The Electroweak Phase Transition in the Inert Doublet Model","url":"/paper/1504.05949","section":"Introduction","sentence":"The nature and strength of the electroweak phase transition in the IDM has been subject of several studies, with increasingly refined treatment of the effective potential [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"1207.0084","title":"Inert Dark Matter and Strong Electroweak Phase Transition","url":"/paper/1207.0084","section":"Introduction","sentence":"Phase transitions in this model were studied in [ref] .","intent_p":0.89,"contests_p":null},{"arxiv_id":"2012.15113","title":"Filtered pseudo-scalar dark matter and gravitational waves from first order phase transition","url":"/paper/2012.15113","section":"Introduction","sentence":"The interplay of DM with cosmological phase transitions has been vastly investigated [ref] , which shows that both the freeze-out temperature and the number density of DM can be tightly correlated with the phase transition if a DM mass originates from the spontaneous symmetry breaking.","intent_p":0.94,"contests_p":null},{"arxiv_id":"2204.04834","title":"Correlating Gravitational Waves with $W$-boson Mass, FIMP Dark Matter, and Majorana Seesaw Mechanism","url":"/paper/2204.04834","section":"Introduction","sentence":"EWPT in the scotogenic scalar sector has been extensively studied [ref] .","intent_p":0.8,"contests_p":null},{"arxiv_id":"2312.04627","title":"Phase Transitions and Gravitational Waves in a Model of $\\mathbb{Z}_{3}$ Scalar Dark Matter","url":"/paper/2312.04627","section":"Introduction","sentence":"First-order phase transitions in the IDM were studied in [ref] and the GW phenomenology of the inert doublet model was elucidated in [ref] .","intent_p":0.85,"contests_p":null}]}],"unlabelled_sentences":43},"outgoing":{"papers":17,"sentences":28,"groups":[{"kind":"extends","label":"Builds on","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1110.5334","title":"Dark Matter as the Trigger of Strong Electroweak Phase Transition","url":"/paper/1110.5334","section":"Introduction","sentence":"In this way we are able to extend the results of [ref] , confirming that there exists a significant (though finely tuned) region of parameter space in the IDM where the strength of the EWPT is sufficiently enhanced for electroweak baryogenesis while satisfying other necessary constraints.","intent_p":0.99,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":3,"quotes":[{"arxiv_id":"1107.3559","title":"Electroweak Baryogenesis in Two Higgs Doublet Models and B meson anomalies","url":"/paper/1107.3559","section":"Methodology","sentence":"[ref] , which considered the most general two-Higgs doublet potential.","intent_p":0.99,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1108.0671","title":"Higgs searches and singlet scalar dark matter: Combined constraints from XENON 100 and the LHC","url":"/paper/1108.0671","section":"Methodology","sentence":"[ref] puts at $f=0.26-0.63$, corresponding to a factor of 6 uncertainty in the direct detection cross section.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1202.1408","title":"Combined search for the Standard Model Higgs boson using up to 4.9 fb-1 of pp collision data at sqrt(s) = 7 TeV with the ATLAS detector at the LHC","url":"/paper/1202.1408","section":"Collider Mass Bounds","sentence":"Following the recent LHC exclusion of SM-like Higgs masses in the region $127-600 GeV$ [ref] - [ref] , we restrict $m_h$ to the window $115-130 GeV$, with special attention to the currently favored value $m_h≅126$ GeV.","intent_p":0.82,"contests_p":null},{"arxiv_id":"1202.1414","title":"Search for the Standard Model Higgs boson in the diphoton decay channel with 4.9 fb-1 of pp collisions at sqrt(s) = 7 TeV with ATLAS","url":"/paper/1202.1414","section":"Collider Mass Bounds","sentence":"Following the recent LHC exclusion of SM-like Higgs masses in the region $127-600 GeV$ [ref] - [ref] , we restrict $m_h$ to the window $115-130 GeV$, with special attention to the currently favored value $m_h≅126$ GeV.","intent_p":0.82,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":1,"sentences":2,"quotes":[{"arxiv_id":"1110.5334","title":"Dark Matter as the Trigger of Strong Electroweak Phase Transition","url":"/paper/1110.5334","section":"Conclusions","sentence":"[ref] finds allowed masses $m_±≅m_A$ in the range $280-370$ GeV, we find a more restricted range $260-320$ GeV, correlated with our limit $λ_1 < 3$ in contrast to theirs, $λ_1 < 4$.","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":7,"sentences":7,"quotes":[{"arxiv_id":"1201.2644","title":"h\\to \\gamma \\gamma In Inert Higgs Doublet Model","url":"/paper/1201.2644","section":"Introduction","sentence":"The Inert Doublet Model (IDM) is a widely studied setting for scalar dark matter [ref] that can have rich phenomenological consequences [ref] - [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"0708.2939","title":"Observing the Dark Scalar Doublet and its Impact on the Standard-Model Higgs Boson at Colliders","url":"/paper/0708.2939","section":"Introduction","sentence":"The Inert Doublet Model (IDM) is a widely studied setting for scalar dark matter [ref] that can have rich phenomenological consequences [ref] - [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"1202.1316","title":"Complex Scalar Singlet Dark Matter: Vacuum Stability and Phenomenology","url":"/paper/1202.1316","section":"Introduction","sentence":"There has been considerable interest in the interplay between dark matter and the electroweak phase transition in recent years [ref] - [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1108.0671","title":"Higgs searches and singlet scalar dark matter: Combined constraints from XENON 100 and the LHC","url":"/paper/1108.0671","section":"Methodology","sentence":"[ref] , and more recently in [ref] ; in particular the quark matrix element $σ_πN$ upon which $f$ depends is poorly determined.","intent_p":0.91,"contests_p":null},{"arxiv_id":"0806.4099","title":"Interpreting the recent results on direct search for dark matter particles in terms of relic neutralino","url":"/paper/0806.4099","section":"Methodology","sentence":"[ref] , and more recently in [ref] ; in particular the quark matrix element $σ_πN$ upon which $f$ depends is poorly determined.","intent_p":0.91,"contests_p":null}]}],"unlabelled_sentences":12},"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":{"arxiv_id":"1204.4722","kind":"model","paper_version":7,"prompt_version":"held-up-v3.5","generated_at":"2026-10-27T21:19:51+00:00","loaded_at":"2026-10-28T01:04:07.794958+00:00","evidence":"thin","account":[],"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"entries":[],"papers_all":1,"self_papers":1,"self_entries":[{"p":1.0,"quote":null,"citing":[{"self":true,"year":2013,"title":"Improved Electroweak Phase Transition with Subdominant Inert Doublet Dark Matter","arxiv_id":"1302.2614"}],"verified":true,"paraphrase":"Used the same one-loop finite temperature effective potential as described in this paper for its analysis of the phase transition."}]}],"counts":{"by_kind":{"method_or_tool":1,"supports_this_paper":1},"dropped":{"relied_on":0,"unknown_ids":0,"account_lines":0,"contest_vetoed":0,"below_threshold":0,"contest_drawback":0,"contest_without_basis":0,"contest_not_one_sentence":0,"contest_on_group_citation":0},"papers_read":4,"self_papers":5,"citing_papers":60,"sentences_read":8,"citing_sentences":83,"unambiguous_read":8,"typed_independent":1,"independent_papers":55,"by_kind_independent":{"supports_this_paper":1}},"input_sha256":"0cb8c9c42b649808a957e442e40e4222a4281b625281cce42635e6d2ee94473f","method":"For a paper with five or more citing arXiv papers, Pith selected up to 40 citing sentences its citation classifier typed, read those whose citation markers point at this paper alone, and wrote one paraphrase for each later paper in each group, each resting on one sentence. A later paper is listed under a label only when the classifier gives one of its sentences that label at intent probability 0.8 or more (0.95 for support), Pith's reading of the sentence finds that the citing paper itself did it, and a second check of the paraphrase against the sentence passes. The section lists uses only: building on the paper, using its method, tool, data or values, comparing with it and citing it as support. It does not list criticism or disagreement, so their absence says nothing about how the paper has been received. Code counted the papers, wrote the summary from the listed entries, set the evidence level and linked each entry to its citing paper. Quotes are copied from the citing sentence and shown only when the citing paper's licence is CC BY, CC BY-SA or CC0; otherwise the paraphrase is shown. Papers that share an author with this one are listed apart. 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":"1 paper by the same authors is listed below: 1 used its method or tool."},"_links":{"html":"https://pith.science/paper/1204.4722"}}