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Higgs trilinear coupling in the standard model effective field theory at the high luminosity LHC and the FCC-ee
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Motivated by the updated high luminosity (HL)-LHC projections for Higgs pair production from ATLAS and CMS and by the release of the FCC-ee feasibility study, we critically revisit the sensitivity of the global standard model effective field theory (SMEFT) analysis to deformations of the Higgs self-coupling modifier
κ
3
. To this end, we quantify the impact of SMEFT operators modifying double Higgs production at the LHC and single Higgs production, including loop corrections, at the FCC-ee, and include renormalization group evolution throughout. We demonstrate that significantly improving on the legacy HL-LHC constraints on
κ
3
at the FCC-ee is not possible without the
s
=
365
GeV
run; that individual and marginalized determinations are similar at the HL-LHC while differing by up to a factor 3 at the FCC-ee; and that quadratic EFT corrections cannot be neglected, especially at the (HL-)LHC. This finding fundamentally alters the picture compared to strategic planning often based on one-parameter projections. Overall, the combination of HL-LHC and FCC-ee data offers unique potential to pin down the Higgs self-coupling with
∼
15
%
precision.
American Physical Society (APS)
Title: Higgs trilinear coupling in the standard model effective field theory at the high luminosity LHC and the FCC-ee
Description:
Motivated by the updated high luminosity (HL)-LHC projections for Higgs pair production from ATLAS and CMS and by the release of the FCC-ee feasibility study, we critically revisit the sensitivity of the global standard model effective field theory (SMEFT) analysis to deformations of the Higgs self-coupling modifier
κ
3
.
To this end, we quantify the impact of SMEFT operators modifying double Higgs production at the LHC and single Higgs production, including loop corrections, at the FCC-ee, and include renormalization group evolution throughout.
We demonstrate that significantly improving on the legacy HL-LHC constraints on
κ
3
at the FCC-ee is not possible without the
s
=
365
GeV
run; that individual and marginalized determinations are similar at the HL-LHC while differing by up to a factor 3 at the FCC-ee; and that quadratic EFT corrections cannot be neglected, especially at the (HL-)LHC.
This finding fundamentally alters the picture compared to strategic planning often based on one-parameter projections.
Overall, the combination of HL-LHC and FCC-ee data offers unique potential to pin down the Higgs self-coupling with
∼
15
%
precision.
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