2013
DOI: 10.1103/physrevd.88.054510
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Higgs andWboson spectrum from lattice simulations

Abstract: The spectrum of energy levels is computed for all available angular momentum and parity quantum numbers in the SU(2)-Higgs model, with parameters chosen to match experimental data from the Higgs-W boson sector of the standard model. Several multiboson states are observed, with and without linear momentum, and all are consistent with weakly interacting Higgs and W bosons. The creation operators used in this study are gauge-invariant so, for example, the Higgs operator is quadratic rather than linear in the Lagr… Show more

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Cited by 15 publications
(15 citation statements)
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“…Moreover, the running gauge coupling, as will be seen below, runs much faster in the present theory as in the standard model, due to the lack of fermions and therefore a much larger β 0 [36]. Hence a quantitative comparison to the standard model is at the current time anyhow only of limited reliability, a problem recognized also in other investigations [55].…”
Section: Jhep04(2014)006mentioning
confidence: 75%
“…Moreover, the running gauge coupling, as will be seen below, runs much faster in the present theory as in the standard model, due to the lack of fermions and therefore a much larger β 0 [36]. Hence a quantitative comparison to the standard model is at the current time anyhow only of limited reliability, a problem recognized also in other investigations [55].…”
Section: Jhep04(2014)006mentioning
confidence: 75%
“…Of course, it is possible to doubt the correctness of the expansion 7 . But the prediction has been confirmed non-perturbatively in various lattice calculations for the weak-Higgs theory with one doublet [25,26,35,36]. Thus, the FMS mechanism appears to be indeed the correct description of the electroweak theory.…”
Section: The Fms Mechanismmentioning
confidence: 90%
“…tr(U (x, x, C ′ )) with C ′ a closed path [24] (in classical field theory it is proved, in quantum field theory it is believed). Non-perturbatively, these operators also carry all the information about the bound-state spectrum, if they have non-zero overlap with all states [25,26]. SU (2) L matrix (with no Higgs flavor indices) and so it satisfies…”
Section: Gauge-invariant Operatorsmentioning
confidence: 99%
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