{"arxiv_id":"hep-ph/0512169","incoming":{"papers":18,"sentences":28,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2512.16645","title":"The Physics of Herwig 7","url":"/paper/2512.16645","section":"Little Higgs Models","sentence":"This model is implemented based on Ref. [ref] using the Feynman rules from [ref] .","intent_p":0.96,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1103.3014","title":"T-Quarks at the Large Hadron Collider: 2010-12","url":"/paper/1103.3014","section":"Introduction","sentence":"This is motivated by constraints from flavor-changing neutral currents in the LHT model [ref] , as well as desire for maximal simplicity.","intent_p":1.0,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":5,"sentences":6,"quotes":[{"arxiv_id":"1210.3904","title":"Flavor changing top quark decay and bottom-strange production in the littlest Higgs model with T-parity","url":"/paper/1210.3904","section":"Brief review of the model","sentence":"Here we briefly review the structure of the LHT model relevant to our analysis, and the detailed description can be found in the literature [ref] .","intent_p":1.0,"contests_p":null},{"arxiv_id":"0811.1214","title":"Symmetries and Asymmetries of B -> K* mu+ mu- Decays in the Standard Model and Beyond","url":"/paper/0811.1214","section":"Littlest Higgs Model with T–Parity (LHT)","sentence":"A prominent example of this class of models is the Littlest Higgs model with T-parity [ref] in which the interactions between SM quarks and heavy mirror quarks, mediated by new heavy charged and neutral gauge bosons, involve a new mixing matrix that differs from the CKM matrix [ref] and is parameterized by three new mixing angles and three new CP-violating phases [ref] .","intent_p":0.97,"contests_p":null},{"arxiv_id":"1012.4385","title":"Tau and muon lepton flavor violations in the littlest Higgs model with T-parity","url":"/paper/1012.4385","section":"Introduction","sentence":"In the early literature on this subject various observable quantities of FCNC and LFV processes were calculated in the LHT and showed that the effects of T-odd partners can be sizable and the correlations among various observable quantities can be different from other new physics model such as supersymmetric (SUSY) models [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"0809.4753","title":"Ultraviolet divergences of flavor changing amplitudes in the littlest Higgs model with T-parity","url":"/paper/0809.4753","section":"Introduction","sentence":"In order to assign the $Z_2$ symmetry for quarks and leptons, new heavy fermions have to be introduced, and flavor mixing matrices associated with the heavy fermions are independent of the Cabibbo-Kobayashi-Maskawa (CKM) [ref] or the Pontecorvo-Maki-Nakagawa-Sakata (PMNS) [ref] matrices [ref] .","intent_p":0.96,"contests_p":null},{"arxiv_id":"1507.06316","title":"Quark flavour observables in the Littlest Higgs model with T-parity after LHC Run 1","url":"/paper/1507.06316","section":"Introduction","sentence":"Further phenomenological discussions of flavour in the LHT model can be found in [ref] .","intent_p":0.98,"contests_p":null}]}],"unlabelled_sentences":20},"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/0512169"}}