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Energy-Enhanced Dimension Eight SMEFT Effects in VBF Higgs production

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arxiv 2410.21563 v2 pith:JXHXRFCS submitted 2024-10-28 hep-ph

Energy-Enhanced Dimension Eight SMEFT Effects in VBF Higgs production

classification hep-ph
keywords smeftoperatorsbosondimension-eighteffectsfusionlambdaproduction
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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We study Higgs boson production via vector boson fusion at the LHC, focusing on the process $pp \to H + jj$ and capturing the leading energy-enhanced contributions within the Standard Model Effective Field Theory (SMEFT) up to order $1/\Lambda^4$. Employing energy-scaling arguments, we predict the magnitude of each higher-dimensional operator's contribution. Utilizing the geometric formulation of SMEFT, our analysis incorporates dimension-eight operators not previously considered. We find that the kinematics of vector boson fusion - characterized by two highly forward jets - tend to suppress contributions from higher-dimensional operators, requiring a lower scale $\Lambda$ for SMEFT effects to become observable. This suggests that the SMEFT remains valid for lower $\Lambda$ than expected. Combined with the fact that LEP constrains the dimension-six operators with the most considerable impact on vector boson fusion, a regime exists where dimension-eight operators can have significant effects. In many cases, these dimension-eight operators also influence associated production processes like $pp \to H V(jj)$, though differences in analysis cuts and kinematics mean this is not always the case. Our findings provide insights that could refine the search for SMEFT signals in collider experiments.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. EFT Validity and Truncation Uncertainty from few Nuisance Parameters

    hep-ph 2026-07 accept novelty 7.0

    SMEFT truncation uncertainty at O(Λ^{-4}) can be modeled by K≪N representative Wilson coefficients plus a decorrelated α=√2 PCA prior that covers full next-order effects in DY, Zh, and VBF.

  2. Renormalization of the SMEFT to Dimension Eight: Fermionic Interactions II

    hep-ph 2026-06 unverdicted novelty 5.0

    Computes one-loop mixing of bosonic and two-fermion interactions into two-fermion operators in dim-8 SMEFT, leaving only four-fermion to two-fermion mixing to finish the renormalization program.

  3. USMEFT as a tool for discovery of universal new physics at high luminosity LHC

    hep-ph 2026-05 unverdicted novelty 3.0

    Universal SMEFT fits to pseudo-data from neutral and charged Drell-Yan processes at HL-LHC can detect universal new physics and extract its properties stably across EFT truncation orders.