{"arxiv_id":"1101.6023","incoming":{"papers":9,"sentences":27,"groups":[{"kind":"extends","label":"Builds on it","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2011.10926","title":"The 2HDM Doppelganger","url":"/paper/2011.10926","section":"Introduction","sentence":"The model is a variant of that presented in Ref. [ref] as the “Top Triangle Moose Model\", with one of the non-linear sigma model fields being replaced by a linear Higgs field.","intent_p":0.98,"contests_p":null},{"arxiv_id":"1207.0450","title":"Discovering Strong Top Dynamics at the LHC","url":"/paper/1207.0450","section":"Introduction","sentence":"Our goal in this paper is to further the phenomenological investigation of the top-pions and top-Higgs at the LHC that was started in [ref] .","intent_p":0.96,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2011.10926","title":"The 2HDM Doppelganger","url":"/paper/2011.10926","section":"Gauge Sector","sentence":"Following Refs. [ref] , we will treat $sinϕ$ in Eqn. [ref] as a small parameter and diagonalize the gauge boson mass matrices perturbatively in $sinϕ$ (which we will relabel as $x$ henceforth for notational simplicity).","intent_p":0.98,"contests_p":null},{"arxiv_id":"1112.3538","title":"Topcolor in the LHC Era","url":"/paper/1112.3538","section":"Introduction","sentence":"This theory, which combines Higgsless and topcolor models, can be used to investigate the phenomenology of TC2 theories [ref] and other theories with strong top dynamics, and we employ it in that capacity in this talk.","intent_p":0.81,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":3,"sentences":4,"quotes":[{"arxiv_id":"1207.0450","title":"Discovering Strong Top Dynamics at the LHC","url":"/paper/1207.0450","section":"Neutral top-pion phenomenology","sentence":"More details about the model can be found in Ref. [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"1301.6971","title":"Gauge theory of Lorentz group as a source of the dynamical electroweak symmetry breaking","url":"/paper/1301.6971","section":"Introduction","sentence":"The topcolor assisted technicolor (combines both technicolor and topcolor ingredients) was considered in [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1209.0204","title":"The Nambu sum rule and the relation between the masses of composite Higgs bosons","url":"/paper/1209.0204","section":"Introduction","sentence":"The so - called topcolor assisted technicolor that combines both technicolor and topcolor ingredients was considered, for example, in [ref] .","intent_p":0.93,"contests_p":null}]}],"unlabelled_sentences":19},"outgoing":{"papers":43,"sentences":68,"groups":[{"kind":"contests","label":"Contests","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1008.0280","title":"Constraints on two-lepton, two quark operators","url":"/paper/1008.0280","section":"Limits on $Δϵ^2_tL$: $ΔF=1$","sentence":"Using the limit $BR(B_s →μ^+ μ^-)< 4.3 ×10^-8$ [ref] and the techniques[We disagree with the numerical extraction of the bound on $ε$ presented in [ref] , though we agree with their method.] of ref.","intent_p":0.52,"contests_p":0.72}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":5,"sentences":6,"quotes":[{"arxiv_id":"0811.3458","title":"Mixed QCD-electroweak corrections to Higgs boson production in gluon fusion","url":"/paper/0811.3458","section":"Tevatron limits from Higgs searches","sentence":"We compute the cross section for $gg →H_t →WW$ according to the approximation [equation] where $Γ^SM(H →gg)$ is the SM partial width of $H$ to gluons computed using HDECAY [ref] , $Γ(H_t →gg)$ and BR($H_t →WW$) are the partial width of $H_t$ to gluons and the branching ratio of $H_t$ to $WW$, respectively, computed using our modified version of HDECAY, and $σ^SM(gg →H)$ is the SM Higgs gluon fusion cross section, which we take from Table 2 of Ref. [ref] for $M_H≤200$ GeV and compute using the public code RGHIGGS [ref] for $M_H> 200$ GeV.","intent_p":0.93,"contests_p":null},{"arxiv_id":"1008.3162","title":"Updated Predictions for Higgs Production at the Tevatron and the LHC","url":"/paper/1008.3162","section":"Tevatron limits from Higgs searches","sentence":"We compute the cross section for $gg →H_t →WW$ according to the approximation [equation] where $Γ^SM(H →gg)$ is the SM partial width of $H$ to gluons computed using HDECAY [ref] , $Γ(H_t →gg)$ and BR($H_t →WW$) are the partial width of $H_t$ to gluons and the branching ratio of $H_t$ to $WW$, respectively, computed using our modified version of HDECAY, and $σ^SM(gg →H)$ is the SM Higgs gluon fusion cross section, which we take from Table 2 of Ref. [ref] for $M_H≤200$ GeV and compute using the public code RGHIGGS [ref] for $M_H> 200$ GeV.","intent_p":0.93,"contests_p":null},{"arxiv_id":"hep-ph/9704448","title":"HDECAY: a Program for Higgs Boson Decays in the Standard Model and its Supersymmetric Extension","url":"/paper/hep-ph/9704448","section":"Tevatron limits from Higgs searches","sentence":"We compute the cross section for $gg →H_t →WW$ according to the approximation [equation] where $Γ^SM(H →gg)$ is the SM partial width of $H$ to gluons computed using HDECAY [ref] , $Γ(H_t →gg)$ and BR($H_t →WW$) are the partial width of $H_t$ to gluons and the branching ratio of $H_t$ to $WW$, respectively, computed using our modified version of HDECAY, and $σ^SM(gg →H)$ is the SM Higgs gluon fusion cross section, which we take from Table 2 of Ref. [ref] for $M_H≤200$ GeV and compute using the public code RGHIGGS [ref] for $M_H> 200$ GeV.","intent_p":0.93,"contests_p":null},{"arxiv_id":"0808.3008","title":"Origin of the Large Perturbative Corrections to Higgs Production at Hadron Colliders","url":"/paper/0808.3008","section":"Tevatron limits from Higgs searches","sentence":"We compute the cross section for $gg →H_t →WW$ according to the approximation [equation] where $Γ^SM(H →gg)$ is the SM partial width of $H$ to gluons computed using HDECAY [ref] , $Γ(H_t →gg)$ and BR($H_t →WW$) are the partial width of $H_t$ to gluons and the branching ratio of $H_t$ to $WW$, respectively, computed using our modified version of HDECAY, and $σ^SM(gg →H)$ is the SM Higgs gluon fusion cross section, which we take from Table 2 of Ref. [ref] for $M_H≤200$ GeV and compute using the public code RGHIGGS [ref] for $M_H> 200$ GeV.","intent_p":0.93,"contests_p":null},{"arxiv_id":"0809.4283","title":"Renormalization-Group Improved Prediction for Higgs Production at Hadron Colliders","url":"/paper/0809.4283","section":"Tevatron limits from Higgs searches","sentence":"We compute the cross section for $gg →H_t →WW$ according to the approximation [equation] where $Γ^SM(H →gg)$ is the SM partial width of $H$ to gluons computed using HDECAY [ref] , $Γ(H_t →gg)$ and BR($H_t →WW$) are the partial width of $H_t$ to gluons and the branching ratio of $H_t$ to $WW$, respectively, computed using our modified version of HDECAY, and $σ^SM(gg →H)$ is the SM Higgs gluon fusion cross section, which we take from Table 2 of Ref. [ref] for $M_H≤200$ GeV and compute using the public code RGHIGGS [ref] for $M_H> 200$ GeV.","intent_p":0.93,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":4,"sentences":6,"quotes":[{"arxiv_id":"1005.3216","title":"Combined Tevatron upper limit on gg->H->W+W- and constraints on the Higgs boson mass in fourth-generation fermion models","url":"/paper/1005.3216","section":"Tevatron limits from Higgs searches","sentence":"We can now translate the Tevatron bounds on the cross-section [ref] into constraints on the $sinω$–$M_H_t$ parameter space as follows.","intent_p":0.94,"contests_p":null},{"arxiv_id":"0908.1811","title":"Search for charged Higgs bosons in top quark decays","url":"/paper/0908.1811","section":"Lower bound on the top-pion mass","sentence":"The relevant limit is BR($t →Π_t^+ b) ≲0.2$ based on D0 data [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"0907.1269","title":"Search for charged Higgs bosons in decays of top quarks in p-pbar collisions at sqrt(s) = 1.96 TeV","url":"/paper/0907.1269","section":"Lower bound on the top-pion mass","sentence":"The Tevatron experiments have searched for this process in the context of two-Higgs-doublet models and set upper bounds of about 10–20% on the branching fraction of $t →H^+ b$, with $H^+$ decaying to $τν$ or $c s̅$ [ref] - we can use this to set a lower bound on the top-pion mass.","intent_p":0.9,"contests_p":null},{"arxiv_id":"0707.0636","title":"Model-independent constraints on Delta F=2 operators and the scale of New Physics","url":"/paper/0707.0636","section":"Limits on $Δϵ^2_tL$: $ΔF=2$","sentence":"where, since GIM cancellation is exact when $Δϵ^2_tL=0$, we find [equation] where the bounds given by the last inequality in each expression come from Ref. [ref] .","intent_p":0.88,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":1,"sentences":2,"quotes":[{"arxiv_id":"0906.5567","title":"The Top Triangle Moose: Combining Higgsless and Topcolor Mechanisms for Mass Generation","url":"/paper/0906.5567","section":"Discovery prospects at the LHC","sentence":"Comparing the branching ratio plot Fig. [ref] to the one for the heavy-$U$ in [ref] , we see that the branching ratio to $Wj$ is enhanced for the heavy-$T$, while that to $Zj$ is suppressed by roughly the same amount.","intent_p":0.95,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":13,"sentences":13,"quotes":[{"arxiv_id":"hep-ph/0607124","title":"A Three Site Higgsless Model","url":"/paper/hep-ph/0607124","section":"Introduction","sentence":"The most economical deconstructed Higgsless model constructed along these lines (a “three site” model) was presented in [ref] , and had, in addition to the SM spectrum, one heavy partner for each fermion and the $W$ and $Z$ bosons.","intent_p":0.83,"contests_p":null},{"arxiv_id":"0904.2137","title":"A Flavor Protection for Warped Higgsless Models","url":"/paper/0904.2137","section":"Introduction","sentence":"Inspired by the idea that one could maintain perturbative unitarity in extra-dimensional models through heavy vector resonance exchanges in lieu of a Higgs [ref] , Higgsless models were intially introduced in an extra-dimensional context as $SU(2)×SU(2)×U(1)$ gauge theories living in a slice of $AdS_5$, with symmetry breaking codified in the boundary condition of the gauge fields [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"hep-ph/0111016","title":"Unitarity of Compactified Five Dimensional Yang-Mills Theory","url":"/paper/hep-ph/0111016","section":"Introduction","sentence":"Inspired by the idea that one could maintain perturbative unitarity in extra-dimensional models through heavy vector resonance exchanges in lieu of a Higgs [ref] , Higgsless models were intially introduced in an extra-dimensional context as $SU(2)×SU(2)×U(1)$ gauge theories living in a slice of $AdS_5$, with symmetry breaking codified in the boundary condition of the gauge fields [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"hep-ph/0201164","title":"Unitarity of Deconstructed Five-Dimensional Yang-Mills Theory","url":"/paper/hep-ph/0201164","section":"Introduction","sentence":"Inspired by the idea that one could maintain perturbative unitarity in extra-dimensional models through heavy vector resonance exchanges in lieu of a Higgs [ref] , Higgsless models were intially introduced in an extra-dimensional context as $SU(2)×SU(2)×U(1)$ gauge theories living in a slice of $AdS_5$, with symmetry breaking codified in the boundary condition of the gauge fields [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"hep-ph/0302263","title":"Unitarity of the Higher Dimensional Standard Model","url":"/paper/hep-ph/0302263","section":"Introduction","sentence":"Inspired by the idea that one could maintain perturbative unitarity in extra-dimensional models through heavy vector resonance exchanges in lieu of a Higgs [ref] , Higgsless models were intially introduced in an extra-dimensional context as $SU(2)×SU(2)×U(1)$ gauge theories living in a slice of $AdS_5$, with symmetry breaking codified in the boundary condition of the gauge fields [ref] .","intent_p":0.96,"contests_p":null}]}],"unlabelled_sentences":40},"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/1101.6023"}}