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FCNC Effects in a Minimal Theory of Fermion Masses

High Energy Physics - Phenomenology · Submitted 18 May 2011

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Particularly stringent bounds, in a few TeV range, come from the corrections to the Z couplings.

how it is stated · asserted 0.99 read the record →

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arXiv ID1105.3725 (version 1)
Pith IDH3EF2TUN, Pith's permanent record of this paper and its review
CitationAndrzej J. Buras, Christophe Grojean, Robert Ziegler, Stefan Pokorski. "FCNC Effects in a Minimal Theory of Fermion Masses." arXiv:1105.3725 (2011). https://pith.science/paper/H3EF2TUN
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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,317 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.25 · human participants 0.01 · controlled comparison 0.04 · randomized assignment 0.01 · states quantitative result 0.92 · compares with prior results 0.11 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

As a minimal theory of fermion masses we extend the SM by heavy vectorlike fermions, with flavor-anarchical Yukawa couplings, that mix with chiral fermions such that small SM Yukawa couplings arise from small mixing angles. This model can be regarded as an effective description of the fermionic sector of a large class of existing flavor models and thus might serve as a useful reference frame for a further understanding of flavor hierarchies in the SM. Already such a minimal framework gives rise to FCNC effects through exchange of massive SM bosons whose couplings to the light fermions get modified by the mixing. We derive general formulae for these corrections and discuss the bounds on the heavy fermion masses. Particularly stringent bounds, in a few TeV range, come from the corrections to the Z couplings.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 As a minimal theory of fermion masses we extend the SM by heavy vectorlike fermions, with flavor-anarchical Yukawa couplings, that mix with chiral fermions such that small SM Yukawa couplings arise from small mixing angles. contribution 0.62 0.67 0.11 asserted 0.99
s1 This model can be regarded as an effective description of the fermionic sector of a large class of existing flavor models and thus might serve as a useful reference frame for a further understanding of flavor hierarchies in the SM. interpretation 0.81 0.15 0.07 hedged possibility 0.51
s2 Already such a minimal framework gives rise to FCNC effects through exchange of massive SM bosons whose couplings to the light fermions get modified by the mixing. result 0.85 0.44 0.31 asserted 0.98
s3 We derive general formulae for these corrections and discuss the bounds on the heavy fermion masses. contribution 0.85 0.94 0.11 asserted 0.98
s4 Particularly stringent bounds, in a few TeV range, come from the corrections to the Z couplings. result 1.00 0.84 0.43 asserted 0.99

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 1.00.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

As a minimal theory of fermion masses we extend the SM by heavy vectorlike fermions, with flavor-anarchical Yukawa couplings, that mix with chiral fermions such that small SM Yukawa couplings arise from small mixing angles. This model can be regarded as an effective description of the fermionic sector of a large class of existing flavor models and thus might serve as a useful reference frame for a further understanding of flavor hierarchies in the SM. Already such a minimal framework gives rise to FCNC effects through exchange of massive SM bosons whose couplings to the light fermions get modified by the mixing. We derive general formulae for these corrections and discuss the bounds on the heavy fermion masses. Particularly stringent bounds, in a few TeV range, come from the corrections to the Z couplings.

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References
How the literature uses it

25 arXiv papers cite this in 39 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 28 sentences without a confident label

Uses its data or values 3 papers
  • 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.].

    A 125 GeV composite Higgs boson versus flavour and electroweak precision tests · Flavour-changing $Z$ couplings · 0.99

  • 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 $s →d$.

    Implications of the discovery of a Higgs boson with a mass of 125 GeV · Flavour-changing $Z$ couplings · 0.96

  • 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.].

    Flavour and Higgs physics near the Fermi scale · Flavour-changing $Z$ couplings · 0.99

Cites it as support 1 paper
Cites it as background 6 papers

What it cites · 16 sentences without a confident label

Uses the method or tool of 1 paper
Uses data or values from 1 paper
Compares with 2 papers
  • 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 $γ0$.

    Composite Higgs-Mediated FCNC · Connection to Existing Models · 0.92

  • Let us now compare our results for heavy fermions with the studies that have been done in the context of composite higgs models [ref] .

    Warped/Composite Phenomenology Simplified · Connection to Existing Models · 0.96

Cites as background 6 papers
  • 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] .

    Higgs as a Holographic Pseudo-Goldstone Boson · Connection to Existing Models · 0.92

  • 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] .

    Warped/Composite Phenomenology Simplified · Connection to Existing Models · 0.92

  • 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] .

    Should Squarks Be Degenerate? · Introduction · 0.98

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