{"arxiv_id":"1105.3725","incoming":{"papers":25,"sentences":39,"groups":[{"kind":"data_used","label":"Uses its data or values","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1211.5085","title":"A 125 GeV composite Higgs boson versus flavour and electroweak precision tests","url":"/paper/1211.5085","section":"Flavour-changing $Z$ couplings","sentence":"In the $b→s$ case, a global analysis of inclusive and exclusive $b→sℓ^+ℓ^-$ decays [ref] finds $|δg_Zbs^L,R|≲8×10^-5$, while in the $s→d$ case, one finds $|δg_Zsd^L,R|≲6×10^-7$ from the $K_L→μ^+μ^-$ decay [ref] [The decay $K^+→π^+νν̅$ leads to a bound $|δg_Zsd^L,R|≲3 ×10^-6$ at 95% C.L. and is thus currently weaker than $K_L→μ^+μ^-$, even though it is theoretically much cleaner.].","intent_p":0.99,"contests_p":null},{"arxiv_id":"1403.6535","title":"Implications of the discovery of a Higgs boson with a mass of 125 GeV","url":"/paper/1403.6535","section":"Flavour-changing $Z$ couplings","sentence":"In the $b→s$ case, a global analysis of inclusive and exclusive $b→sℓ^+ℓ^-$ decays [ref] finds $|δg_Zbs^L,R|≲8×10^-5$, while in the $s→d$ case, one finds $|δg_Zsd^L,R|≲6×10^-7$ from the $K_L→μ^+μ^-$ decay [ref] .[The decay $K^+→π^+νν̅$ leads to a bound $|δg_Zsd^L,R|≲3 ×10^-6$ at 95% C.L. and is thus currently weaker than $K_L→μ^+μ^-$, even though it is theoretically much cleaner.] Using ([ref]) one finds that the resulting constraints on the left-handed coupling are comparable for $b→s$ and $s →d$.","intent_p":0.96,"contests_p":null},{"arxiv_id":"1312.1393","title":"Flavour and Higgs physics near the Fermi scale","url":"/paper/1312.1393","section":"Flavour-changing $Z$ couplings","sentence":"In the $b→s$ case, a global analysis of inclusive and exclusive $b→sℓ^+ℓ^-$ decays [ref] finds $|δg_Zbs^L,R|≲8×10^-5$, while in the $s→d$ case, one finds $|δg_Zsd^L,R|≲6×10^-7$ from the $K_L→μ^+μ^-$ decay [ref] [The decay $K^+→π^+νν̅$ leads to a bound $|δg_Zsd^L,R|≲3 ×10^-6$ at 95% C.L. and is thus currently weaker than $K_L→μ^+μ^-$, even though it is theoretically much cleaner.].","intent_p":0.99,"contests_p":null}]},{"kind":"supports_this_paper","label":"Cites it as support","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1301.5498","title":"Particle-Antiparticle Mixing, CP Violation and Rare K and B Decays in a Minimal Theory of Fermion Masses","url":"/paper/1301.5498","section":"Procedure in the Trivially Unitary Model","sentence":"As shown in [ref] for such values of $M$ the model is also consistent with electroweak constraints.","intent_p":0.99,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":6,"sentences":7,"quotes":[{"arxiv_id":"1301.5498","title":"Particle-Antiparticle Mixing, CP Violation and Rare K and B Decays in a Minimal Theory of Fermion Masses","url":"/paper/1301.5498","section":"Introduction","sentence":"In a “minimal theory of fermion masses\" (MTFM) [ref] the fermionic content of the SM is extended by heavy vectorlike fermions, with flavor-anarchical Yukawa couplings, that mix with SM chiral quarks.","intent_p":0.97,"contests_p":null},{"arxiv_id":"1203.4218","title":"Flavour physics from an approximate U(2)^3 symmetry","url":"/paper/1203.4218","section":"Summary and outlook","sentence":"We defer to later work a detailed analysis of the phenomenological consequences for flavour violating as well as flavour conserving observables, as done e.g. in [ref] in the general case and in [ref] for the $U(3)^3$ case.","intent_p":0.81,"contests_p":null},{"arxiv_id":"2603.21414","title":"From Higgs physics to lepton flavour violation: current bounds and future prospects for vector-like lepton models","url":"/paper/2603.21414","section":"Introduction","sentence":"For general investigations on vector-like fermions we refer to Refs. [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"2312.09255","title":"Quark-lepton mass relations from modular flavor symmetry","url":"/paper/2312.09255","section":"Introduction","sentence":"less progress has been made concerning the formulation of a fully convincing theory of fermion mass hierarchies, though there have been many proposals in this direction [ref] .","intent_p":0.99,"contests_p":null},{"arxiv_id":"1708.00794","title":"Higgs Physics","url":"/paper/1708.00794","section":"The flavor preserving nature of the SM Higgs","sentence":"This nice property is no longer true if the SM fermions mix with vector-like partners or in the presence of generic higher dimension Yukawa interactions (see for instance Ref. [ref] for a general phenomenological discussion):","intent_p":0.88,"contests_p":null}]}],"unlabelled_sentences":28},"outgoing":{"papers":15,"sentences":27,"groups":[{"kind":"method_or_tool","label":"Uses the method or tool of","papers":1,"sentences":1,"quotes":[{"arxiv_id":"0712.1419","title":"Updated Values of Running Quark and Lepton Masses","url":"/paper/0712.1419","section":"Phenomenology","sentence":"Then we use the results of Ref. [ref] to fit quark masses at 1 TeV by certain powers of $$ (which are not uniquely determined since $$ is not particularly small).","intent_p":0.85,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":1,"sentences":1,"quotes":[{"arxiv_id":"hep-ph/0311084","title":"On the short-distance constraints from K_{L,S} -> mu^+ mu^-","url":"/paper/hep-ph/0311084","section":"Phenomenology","sentence":"Constraints on $K_L →μ^+ μ^-$ require $|δg_L,R^ds| ≤6 ×10^-7$ as we found using the upper bound in Ref. [ref] .","intent_p":0.96,"contests_p":null}]},{"kind":"comparison","label":"Compares with","papers":2,"sentences":3,"quotes":[{"arxiv_id":"0906.1542","title":"Composite Higgs-Mediated FCNC","url":"/paper/0906.1542","section":"Connection to Existing Models","sentence":"In Ref. [ref] the bounds on heavy fermion masses have been obtained from tree-level higgs exchange contributions to the FCNC processes, for flavour violating couplings to the higgs boson corresponding to our general case with $γ0$.","intent_p":0.92,"contests_p":null},{"arxiv_id":"hep-ph/0612180","title":"Warped/Composite Phenomenology Simplified","url":"/paper/hep-ph/0612180","section":"Connection to Existing Models","sentence":"Let us now compare our results for heavy fermions with the studies that have been done in the context of composite higgs models [ref] .","intent_p":0.96,"contests_p":null}]},{"kind":"background","label":"Cites as background","papers":6,"sentences":6,"quotes":[{"arxiv_id":"hep-ph/0306259","title":"Higgs as a Holographic Pseudo-Goldstone Boson","url":"/paper/hep-ph/0306259","section":"Connection to Existing Models","sentence":"Lagrangian ([ref]) has been widely used as a simplified formulation [ref] for the fermionic sector of composite Higgs models [ref] that are dual to certain warped 5d models [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"hep-ph/0612180","title":"Warped/Composite Phenomenology Simplified","url":"/paper/hep-ph/0612180","section":"Connection to Existing Models","sentence":"Lagrangian ([ref]) has been widely used as a simplified formulation [ref] for the fermionic sector of composite Higgs models [ref] that are dual to certain warped 5d models [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"hep-ph/9304307","title":"Should Squarks Be Degenerate?","url":"/paper/hep-ph/9304307","section":"Introduction","sentence":"Several theoretical ideas have been proposed to explain the peculiar pattern of fermion masses and mixings, such as horizontal symmetries [ref] , fermion localization in extra dimensional models of Randall–Sundrum (RS) type [ref] or wave function renormalization (WFR) [ref] by new strong interactions [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"hep-ph/9903417","title":"Hierarchies without Symmetries from Extra Dimensions","url":"/paper/hep-ph/9903417","section":"Introduction","sentence":"Several theoretical ideas have been proposed to explain the peculiar pattern of fermion masses and mixings, such as horizontal symmetries [ref] , fermion localization in extra dimensional models of Randall–Sundrum (RS) type [ref] or wave function renormalization (WFR) [ref] by new strong interactions [ref] .","intent_p":0.98,"contests_p":null},{"arxiv_id":"0711.3376","title":"Solving the flavour problem with hierarchical fermion wave functions","url":"/paper/0711.3376","section":"Introduction","sentence":"Several theoretical ideas have been proposed to explain the peculiar pattern of fermion masses and mixings, such as horizontal symmetries [ref] , fermion localization in extra dimensional models of Randall–Sundrum (RS) type [ref] or wave function renormalization (WFR) [ref] by new strong interactions [ref] .","intent_p":0.98,"contests_p":null}]}],"unlabelled_sentences":16},"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/1105.3725"}}