2016
DOI: 10.1007/jhep03(2016)180
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The universal one-loop effective action

Abstract: We present the universal one-loop effective action for all operators of dimension up to six obtained by integrating out massive, non-degenerate multiplets. Our general expression may be applied to loops of heavy fermions or bosons, and has been checked against partial results available in the literature. The broad applicability of this approach simplifies one-loop matching from an ultraviolet model to a lower-energy effective field theory (EFT), a procedure which is now reduced to the evaluation of a combinati… Show more

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Cited by 119 publications
(218 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: 55%
“…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: 55%
“…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%
“…The logical step is then to eliminate such unnecessary calculations by doing them once-and-for-all. The expression obtained in this way is the so-called Universal One-Loop Effective Action (UOLEA) [23,24]. It allows one to bypass the need for either Feynman diagram or functional methods entirely when deriving Wilson coefficients for operators up to dimension six.…”
Section: Jhep08(2017)054mentioning
confidence: 99%
“…Therefore, we have adopted a top-down approach where there is a model and the aim has been to implement a systematic procedure for getting the low-energy theory, including all loop generated local operators. We have extended the covariant derivative expansion [9,10], taking into account SM extensions where heavy fields are coupled to (light) SM fields with linear (or higher) couplings that are proportional to the scale of new physics. Specific examples have been provided for the singlet extension of the SM and for THDM (I, II,X and Y) models [35].…”
Section: Discussionmentioning
confidence: 99%
“…A second problem, as observed in ref. [6], is that there are cases where the so-called covariant derivative expansion [7][8][9][10] (CDE) does not reproduce all the local operators in the lowenergy sector.…”
Section: Jhep05(2016)162mentioning
confidence: 99%