Bottom quark and tau lepton masses in a toy $$\textrm{SU}(6)$$ SU ( 6 ) model

[1]  A. Alves,et al.  Constraining 3-3-1 models at the LHC and future hadron colliders , 2022, Physical Review D.

[2]  C. A. Vaquera-Araujo,et al.  Scotogenic neutrino masses with gauged matter parity and gauge coupling unification , 2021, Journal of High Energy Physics.

[3]  Ning Chen,et al.  High-quality grand unified theories with three generations , 2021, Chinese Physics C.

[4]  A. Buras,et al.  The charm of 331 , 2021, Journal of High Energy Physics.

[5]  N. Chen,et al.  Axion model with the SU(6) unification , 2021, Physical Review D.

[6]  S. Kovalenko,et al.  An extended 3-3-1 model with radiative linear seesaw mechanism , 2021, Physics Letters B.

[7]  W. Y. Chan,et al.  Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in the $$\ell \ell bb$$ and $$\ell \ell WW$$ final states in pp collisions at $$\sqrt{s}=13$$ $$\text {TeV}$$ with the ATLAS detector , 2021, The European Physical Journal C.

[8]  Atlas Collaboration,et al.  Search for heavy resonances decaying into a pair of $Z$ bosons in the $\ell^+\ell^-\ell'^+\ell'^-$ and $\ell^+\ell^-\nu\bar\nu$ final states using 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector , 2020, 2009.14791.

[9]  Hoang Dai Nghia Nguyen,et al.  Search for heavy neutral Higgs bosons produced in association with b-quarks and decaying into b-quarks at √s = 13 TeV with the ATLAS detector , 2020 .

[10]  R. Mohapatra,et al.  Predictive Dirac and Majorana neutrino mass textures from SU(6) grand unified theories , 2020, 2005.05413.

[11]  S. M. Etesami,et al.  Search for a heavy Higgs boson decaying to a pair of W bosons in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV , 2020, Journal of High Energy Physics.

[12]  S. M. Etesami,et al.  Search for a heavy pseudoscalar Higgs boson decaying into a 125 GeV Higgs boson and a Z boson in final states with two tau and two light leptons at √s = 13 TeV , 2020 .

[13]  Hoang Dai Nghia Nguyen,et al.  Search for Heavy Higgs Bosons Decaying into Two Tau Leptons with the ATLAS Detector Using pp Collisions at sqrt[s]=13  TeV. , 2020, Physical review letters.

[14]  S. M. Etesami,et al.  Search for charged Higgs bosons decaying into a top and a bottom quark in the all-jet final state of pp collisions at √s = 13 TeV , 2020 .

[15]  S. Weinberg.  Models of lepton and quark masses , 2020, Physical Review D.

[16]  Mossolov,et al.  Search for a charged Higgs boson decaying into top and bottom quarks in events with electrons or muons in proton-proton collisions at √s = 13 TeV , 2019, 1908.09206.

[17]  Robert Feger,et al.  LieART 2.0 - A Mathematica application for Lie Algebras and Representation Theory , 2019, Comput. Phys. Commun..

[18]  S. M. Etesami,et al.  Search for heavy Higgs bosons decaying to a top quark pair in proton-proton collisions at $$ \sqrt{s} $$ = 13 TeV , 2019, Journal of High Energy Physics.

[19]  Atlas Collaboration.  Search for heavy neutral Higgs bosons produced in association with b -quarks and decaying into b -quarks at s=13  TeV with the ATLAS detector , 2019, Physical Review D.

[20]  Atlas Collaboration,et al.  Cross-section measurements of the Higgs boson decaying into a pair of τ-leptons in proton-proton collisions at s=13 TeV with the ATLAS detector , 2019 .

[21]  V. M. Ghete,et al.  Observation of Higgs Boson Decay to Bottom Quarks. , 2018, Physical review letters.

[22]  Hoang Dai Nghia Nguyen,et al.  Birmingham Observation of H bb decays and VH production with the ATLAS detector , 2018 .

[23]  Hoang Dai Nghia Nguyen,et al.  Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in the (cid:2)(cid:2) bb final state in pp collisions at √ s = 13 TeV with the ATLAS detector , 2018 .

[24]  V. M. Ghete,et al.  Observation of the Higgs boson decay to a pair of τ leptons with the CMS detector , 2018 .

[25]  U. Sarkar,et al.  331 models and grand unification: From minimal SU(5) to minimal SU(6) , 2016, 1608.05334.

[26]  M. Venturini,et al.  Search for the lepton flavour violating decay $$\mu ^+ \rightarrow \mathrm {e}^+ \gamma $$μ+→e+γ with the full dataset of the MEG experiment , 2016 .

[27]  M. Venturini,et al.  Search for the lepton flavour violating decay μ+→ e +γ with the full dataset of the MEG experiment: MEG Collaboration , 2016 .

[28]  S. Boucenna,et al.  Predicting charged lepton flavor violation from 3-3-1 gauge symmetry , 2015, 1502.07546.

[29]  S. Boucenna,et al.  Small neutrino masses and gauge coupling unification , 2014, 1411.0566.

[30]  S. Boucenna,et al.  Radiative neutrino mass in 3-3-1 scheme , 2014, 1405.2332.

[31]  J. Montero,et al.  Flavor-changing neutral currents in the minimal 3-3-1 model revisited , 2013 .

[32]  A. Buras,et al.  331 models facing new b → sμ+μ− data , 2013, 1311.6729.

[33]  A. Buras,et al.  The anatomy of quark flavour observables in 331 models in the flavour precision era , 2012, 1310.4614.

[34]  The Cms Collaboration.  Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC , 2012, 1207.7235.

[35]  Robert Feger,et al.  LieART - A Mathematica application for Lie algebras and representation theory , 2012, Comput. Phys. Commun..

[36]  H. Long,et al.  Question of Peccei-Quinn symmetry and quark masses in the economical 3-3-1 model , 2012, 1205.5648.

[37]  C. A. Pires,et al.  The minimal 3-3-1 model with only two Higgs triplets , 2011, 1109.0031.

[38]  S. Barr.  Doubly Lopsided Mass Matrices from Supersymmetric SU(N) Unification , 2008, 0805.4808.

[39]  P. Fox,et al.  Quark and lepton masses from top loops , 2008, 0805.0822.

[40]  S. Barr.  Doubly lopsided mass matrices from unitary unification , 2008, 0804.1356.

[41]  E. Ma.  Verifiable radiative seesaw mechanism of neutrino mass and dark matter , 2006, hep-ph/0601225.

[42]  A. G. Dias,et al.  Concerning the Landau pole in 3-3-1 models , 2004, hep-ph/0407141.

[43]  T. Appelquist,et al.  Fermion masses and mixing in extended technicolor models , 2003, hep-ph/0308061.

[44]  A. G. Dias,et al.  Stabilizing the invisible axion in 3-3-1 models , 2003, hep-ph/0308037.

[45]  W. Ponce,et al.  Minimal scalar sector of 3-3-1 models without exotic electric charges , 2002, hep-ph/0210026.

[46]  Elizabeth H. Simmons,et al.  Strong dynamics and electroweak symmetry breaking , 2002, hep-ph/0203079.

[47]  Naoyuki Haba,et al.  Anarchy and hierarchy , 2000, hep-ph/0009174.

[48]  Weiner,et al.  Neutrino mass anarchy , 1999, Physical review letters.

[49]  S. P. Martin,et al.  Perceptual Content , 1994 .

[50]  M. D. Tonasse.  The scalar sector of 3-3-1 models , 1996, hep-ph/9605230.

[51]  H. Long.  The 331 model with right handed neutrinos , 1995, hep-ph/9504274.

[52]  K. Lane.  Technicolor , 1995, My Wilderness.

[53]  Pál.  Strong-CP question in SU(3)c x SU(3)L x U(1)N models. , 1994, Physical review. D, Particles and fields.

[54]  Ng,et al.  Electroweak theory of SU(3) x U(1). , 1992, Physical review. D, Particles and fields.

[55]  V. Pleitez,et al.  Neutral currents and GIM mechanism in SU(3)-L x U(1)-N models for electroweak interactions , 1992, hep-ph/9212271.

[56]  H. Murayama,et al.  Radiative breaking of Peccei-Quinn symmetry at the intermediate mass scale , 1992 .

[57]  D. Seckel,et al.  Planck-scale corrections to axion models. , 1992, Physical review. D, Particles and fields.

[58]  L. Widrow,et al.  Solutions to the strong-CP problem in a world with gravity☆ , 1992, hep-ph/9203206.

[59]  M. Kamionkowski,et al.  Planck scale physics and the Peccei-Quinn mechanism , 1992, hep-th/9202003.

[60]  Jihn E. Kim,et al.  The μ-problem and the strong CP-problem , 1984 .

[61]  L. Ibáñez.  Radiative Fermion Masses in Grand Unified Theories , 1981 .

[62]  H. Georgi,et al.  Grand Unified Models With an Automatic {Peccei-Quinn} Symmetry , 1981 .

[63]  L. Susskind,et al.  Light composite fermions , 1980 .

[64]  S. Barr.  Light Fermion Mass Hierarchy and Grand Unification , 1980 .

[65]  E. Eichten,et al.  Dynamical breaking of weak interaction symmetries , 1980 .

[66]  P. Frampton.  Unification of Flavor , 1980 .

[67]  P. Frampton.  SU(N) grand unification with several quark-lepton generations , 1979 .

[68]  H. Georgi.  Towards a Grand Unified Theory of Flavor , 1979 .

[69]  L. Susskind,et al.  Mass Without Scalars , 1979 .

[70]  R. Shrock,et al.  SU(3) x U(1) gauge theory of weak and electromagnetic interactions , 1978 .

[71]  A. Zee,et al.  Calculating the electron mass in terms of measured quantities , 1978 .

[72]  Dimitri V. Nanopoulos,et al.  Aspects of the flipped unification of strong, weak and electromagnetic interactions , 1978 .

[73]  A. Zee,et al.  New approach to the electron-muon mass ratio , 1977 .

[74]  H. Fritzsch,et al.  Unified Interactions of Leptons and Hadrons , 1975 .

[75]  H. Georgi,et al.  Unity of All Elementary Particle Forces , 1974 .

[76]  H. Georgi,et al.  Attempts to calculate the electron mass , 1973 .

[77]  Search for heavy resonances decaying into a pair of Z bosons in the and final states using 139 of proton–proton collisions at TeV with the ATLAS detector , 2021 .

[78]  Arnulf Quadt,et al.  Oxford University Press : Review of Particle Physics, 2020-2021 , 2020 .

[79]  Pisano,et al.  Lepton masses in an SU(3)L , 1993, Physical review. D, Particles and fields.

[80]  H. Georgi,et al.  Spontaneously Broken Gauge Symmetry and Elementary Particle Masses , 1972 .