{"arxiv_id":"hep-ph/9605288","incoming":{"papers":312,"sentences":374,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2407.17549","title":"Baryogenesis and first-order QCD transition with gravitational waves from a large lepton asymmetry","url":"/paper/2407.17549","section":"The perturbative approach and motivation to go beyond","sentence":"A full prescription to deal with the infrared divergences at finite temperature was presented in [ref] , by matching the full 4-dimensional theory to an effective 3-dimensional theory, which can then be solved with lattice Monte Carlo methods [ref] .","intent_p":0.89,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":5,"sentences":5,"quotes":[{"arxiv_id":"2606.12533","title":"Constraining the real scalar singlet extension of the SM","url":"/paper/2606.12533","section":"Numerical results","sentence":"The transition is first-order for $x_c ≡λ̃_3(T_c)/g̃_3^2(T_c) ≲0.11$ and a crossover above this value [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"2608.22240","title":"Primordial Asymmetries, Primordial Equation of State & Primordial Black Holes","url":"/paper/2608.22240","section":"Introduction","sentence":"However, the measured Higgs boson mass $m_H = 125 GeV$ from [ref] suggests a smooth crossover [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"2012.03953","title":"Cosmological phase transitions: is effective field theory just a toy?","url":"/paper/2012.03953","section":"Introduction","sentence":"Lattice calculations show that in the standard model, a SFO-EWPT is only achieved for a Higgs mass $m_h0 ≲65$GeV [ref] well below the measured value $m_h0 ≊125.1$GeV [ref] .","intent_p":0.86,"contests_p":null},{"arxiv_id":"2207.02867","title":"First-Order Electroweak Phase Transition and Baryogenesis from a Naturally Light Singlet Scalar","url":"/paper/2207.02867","section":"Effect of Coleman-Weinberg correction to the phase transition","sentence":"In the SM, lattice simulation [ref] has shown that the strong first order phase transition can be achieved for $m_h ≲43$ for a top quark mass $m_t ≃173$.","intent_p":0.91,"contests_p":null},{"arxiv_id":"2107.05650","title":"Cornering the Two Higgs Doublet Model Type II","url":"/paper/2107.05650","section":"Electroweak Phase Transition","sentence":"In the SM this could be achieved for $m_h^0≲70$ GeV [ref] , however the measurement of the SM Higgs boson mass as $m_h^0 = 125.1 ±0.14$ GeV [ref] means we now require BSM physics to achieve a SFOEWPT; a 2HDM is in principle capable of generating this.","intent_p":0.8,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1912.07189","title":"The Electroweak Phase Transition: A Collider Target","url":"/paper/1912.07189","section":"The Electroweak Temperature","sentence":"Nevertheless, for lighter values of $m_H$ consistent with a first order transition, the lattice values for the transition temperature are consistent with those obtained using Eq. ([ref]) (see, e.g., Ref. [ref] ).","intent_p":0.81,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":4,"sentences":4,"quotes":[{"arxiv_id":"2510.13770","title":"Gauge-independent Gravitational Waves from Cogenesis in a $B-L$ Conserving Universe","url":"/paper/2510.13770","section":"Introduction","sentence":"Thus the electroweak baryogenesis within the standard model cannot generate a sufficient CP violation to explain the observed baryon asymmetry in the universe, and the first-order phase transitions in the standard model do not produce gravitational waves at detectable levels [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"1407.2122","title":"The Higgs and the Excessive Success of the Standard Model","url":"/paper/1407.2122","section":"Baryogenesis via leptogenesis from heavy $ν_R$ decay","sentence":"However, a more quantitative analysis [ref] shows that baryogenesis is not possible in the SM because there is not enough CP violation and the phase transition is not sufficiently strong first order, because the Higgs mass is too heavy.","intent_p":0.96,"contests_p":null},{"arxiv_id":"2205.06669","title":"Multi-step phase transitions and gravitational waves in the inert doublet model","url":"/paper/2205.06669","section":"Phase transition patterns","sentence":"This is motivated by the fact that for small $v_c/T_c$, perturbative analysis does not allow to clearly determine if a PT is of the first kind or not [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"2512.17002","title":"Intrinsic Properties of Large CP Violation in the Complex Two-Higgs-Doublet Model","url":"/paper/2512.17002","section":"Introduction","sentence":"First, for a 125 GeV Higgs boson, the electroweak phase transition is a smooth crossover [ref] , failing to provide the required departure from thermal equilibrium.","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":42,"sentences":42,"quotes":[{"arxiv_id":"2003.00099","title":"$CP$ violation from $\\tau$, $t$ and $b$ dimension-6 Yukawa couplings -- interplay of baryogenesis, EDM and Higgs physics","url":"/paper/2003.00099","section":"The baryon asymmetry $Y_B$","sentence":"Electroweak baryogenesis requires two ingredients that go beyond the SM: * New sources of $CP$ violation [ref] ; * Modification of the EWPT such that it is strongly first order (rather than a smooth crossover, as is the case in the SM [ref] ).","intent_p":0.87,"contests_p":null},{"arxiv_id":"1903.11604","title":"Nonperturbative analysis of the gravitational waves from a first-order electroweak phase transition","url":"/paper/1903.11604","section":"Introduction","sentence":"In the past, dimensional reduction has been applied to the SM [ref] , the MSSM [ref] the Two-Higgs-Doublet model (2HDM) [ref] , as well as the real scalar singlet [ref] (xSM) and triplet [ref] ($Σ$SM) extensions of the SM (see also Ref. [ref] ).","intent_p":0.94,"contests_p":null},{"arxiv_id":"1005.0752","title":"Fast Electroweak Symmetry Breaking and Cold Electroweak Baryogenesis","url":"/paper/1005.0752","section":"Introduction","sentence":"It is well known that electroweak baryogenesis within the Standard Model is subject to a double kill: the electroweak phase transition is a cross-over [ref] so that the requirement for non-equilibrium is never fulfilled; and at the electroweak phase transition temperatures, the CP-violation in the fermion mass matrix is too small by many orders of magnitude (see [ref] for a review).","intent_p":0.81,"contests_p":null},{"arxiv_id":"2202.04221","title":"Gravitational waves in models with multicritical-point principle","url":"/paper/2202.04221","section":"Introduction","sentence":"In particular, stochastic GWs originating from first-order phase transitions (FOPTs) [ref] have received much attention in recent years, as many new physics models predict them in the early Universe, contrary to the pure Standard Model (SM), which shows a crossover electroweak (EW) transition [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"2108.11394","title":"The Electro-Weak Phase Transition at Colliders: Discovery Post-Mortem","url":"/paper/2108.11394","section":"Introduction","sentence":"The Standard Model (SM) predicts a smooth crossover [ref] , but new states at the electro-weak scale can alter this picture dramatically (see, e.g. [ref] , for a review see [ref] ).","intent_p":0.85,"contests_p":null}]}],"unlabelled_sentences":321},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"claims":[{"relation":"same_result","label":"States the same result","papers":[{"arxiv_id":"hep-lat/9612023","url":"/paper/hep-lat/9612023","title":"Four-dimensional Simulation of the Hot Electroweak Phase Transition with the SU(2) Gauge-Higgs Model","main_claim":"Our results suggest that the first-order transition terminates around $M_H \\sim 80$GeV.","p":0.82}]}],"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/9605288"}}