2016
DOI: 10.1007/jhep05(2016)162
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Low energy behaviour of standard model extensions

Abstract: The integration of heavy scalar fields is discussed in a class of BSM models, containing more that one representation for scalars and with mixing. The interplay between integrating out heavy scalars and the Standard Model decoupling limit is examined. In general, the latter cannot be obtained in terms of only one large scale and can only be achieved by imposing further assumptions on the couplings. Systematic low-energy expansions are derived in the more general, non-decoupling scenario, including mixed tree-l… Show more

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Cited by 43 publications
(59 citation statements)
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“…We have explored the low-energy consequences of generic heavy states with different quantum numbers, coupled to the SM particles, i.e., the fingerprints they leave on the LECs. Similar studies have been done before for specific weakly-coupled models of new physics [83][84][85][86][87][88][89][90], within the much simpler linear framework with a SM doublet Higgs; in some cases, even at the one-loop level [91][92][93][94][95][96][97][98][99][100] in the usual perturbative expansion in powers of small couplings. However, the LECs of the generic non-linear EWET have remained largely unexplored until now [12,72,73].…”
Section: Jhep04(2017)012mentioning
confidence: 54%
“…We have explored the low-energy consequences of generic heavy states with different quantum numbers, coupled to the SM particles, i.e., the fingerprints they leave on the LECs. Similar studies have been done before for specific weakly-coupled models of new physics [83][84][85][86][87][88][89][90], within the much simpler linear framework with a SM doublet Higgs; in some cases, even at the one-loop level [91][92][93][94][95][96][97][98][99][100] in the usual perturbative expansion in powers of small couplings. However, the LECs of the generic non-linear EWET have remained largely unexplored until now [12,72,73].…”
Section: Jhep04(2017)012mentioning
confidence: 54%
“…techniques exist for doing so up to one-loop level [18][19][20][21][22][23][24][25][26][27][28][29]. 2 In practice, functional methods have typically been overlooked in favour of the more traditional Feynman diagram approach, where many tools have been developed to ease otherwise complicated calculations.…”
Section: Jhep08(2017)054mentioning
confidence: 99%
“…[40], that functional methods did not appear to account for one-loop matching involving both heavy and light particles in the loop. This was addressed by us [27] and others [25,26,28], each demonstrating different procedures for treating mixed heavy-light matching in the path integral approach. 3 We emphasised in particular that our method also allowed for the computation of universal terms [27], that could in principle be added to the original UOLEA.…”
Section: Jhep08(2017)054mentioning
confidence: 99%
“…The complete one-loop anomalous dimension matrix (ADM) for the dimension-six operators has been calculated very recently in this basis [3][4][5][6]. These advances, together with simultaneous theoretical developments occurring in the field (such as in the matching of specific models to the SMEFT at one loop [7][8][9][10][11][12]14,15] and in the automatization of calculations within the SMEFT [13]), pave the way to the systematic use of EFT methods in the analysis of new physics models. The power of the SMEFT approach is that it allows to relate physics at disparate energy scales, in our case properties of the high-energy dynamics at the scale , with measurements that take place at low energies, while performing an expansion in 1/ that allows to keep leading new physics effects in a consistent manner.…”
Section: Introductionmentioning
confidence: 99%