2017
DOI: 10.1103/physrevd.96.075008
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Distinguishing a Higgs-like dilaton scenario with a complete bosonic effective field theory basis

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Cited by 30 publications
(19 citation statements)
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“…The other common non-trivial features of near-conformal gauge theories are the emergence of a light scalar resonance. Such a new degree of freedom at low energy may be identified as a dilaton arising from the spontaneous breaking of scale symmetry, and can be used to extend the Higgs sector of the standard model of particle physics [31][32][33][34][35][36][37][38][39][40][41]. Interestingly, recent lattice studies of SU (3) gauge theories with 8 fundamental Dirac fermions [42][43][44][45], as well as 2 two-index symmetric Dirac fermions [46][47][48][49][50], performed with moderate sizes of the fermion mass found a relatively light scalar in the spectrum.…”
Section: Introductionmentioning
confidence: 99%
“…The other common non-trivial features of near-conformal gauge theories are the emergence of a light scalar resonance. Such a new degree of freedom at low energy may be identified as a dilaton arising from the spontaneous breaking of scale symmetry, and can be used to extend the Higgs sector of the standard model of particle physics [31][32][33][34][35][36][37][38][39][40][41]. Interestingly, recent lattice studies of SU (3) gauge theories with 8 fundamental Dirac fermions [42][43][44][45], as well as 2 two-index symmetric Dirac fermions [46][47][48][49][50], performed with moderate sizes of the fermion mass found a relatively light scalar in the spectrum.…”
Section: Introductionmentioning
confidence: 99%
“…An alternative would be to considered a non-linear realisation and the corresponding effective Lagrangian dubbed HEFT [181][182][183][184][185][186]. In this context, however, a much larger number of operators should be taken into consideration and a slightly different phenomenology is expected [187][188][189][190][191][192][193][194][195][196]. The focus in this paper is on the linear EWSB realisation and therefore the HEFT Lagrangian will not be considered in what follows.…”
Section: (34)mentioning
confidence: 99%
“…In order to reproduce the expected value of the EW VEV, v ≡ 245 GeV fixed through the W gauge boson mass, it is then necessary to invoke a large value of the Higgs quartic coupling λ, describing in this way a strongly interacting scenario with a non-linearly realised EWSB mechanism. This is an intriguing possibility, especially considering the recent interest in non-SM descriptions of the Higgs sector, such as composite Higgs models [87][88][89][90][91][92][93][94][95], dilaton models [96][97][98][99][100][101][102][103], or general effective Lagrangians [104][105][106][107][108][109][110][111][112][113][114][115][116][117][118][119][120][121]. In this letter, however, the traditional EWSB mechanism will be considered, and this requires to invoke a fine tuning: either there is cancellation between µ 2 and λ HΦ v 2 Φ , or λ HΦ is artificially small.…”
Section: Jhep10(2017)168mentioning
confidence: 99%