Abstract
In this comprehensive study, we investigate K-factors (\(K=\sigma _{\text {NLO}}/\sigma _{\text {LO}}\equiv 1+\delta K\)) for a broad array of Standard Model processes at the 14 TeV LHC, which are pivotal for background assessments in Beyond the Standard Model (BSM) searches. Using MadGraph5_aMC@NLO, we calculate the leading-order and next-to-leading-order (NLO) cross-sections and compute the corresponding K-factors for 111 processes. Our analysis reveals K-factors ranging from 1.005 for \(pp \rightarrow jjj\) to 4.221 for \(pp\rightarrow W^\pm \gamma \gamma \gamma \). Key findings include: (i) processes involving photons display significantly high K-factors, attributed to gluon-initiated processes at NLO; (ii) processes with multiple particle productions, particularly those involving vector bosons, exhibit elevated K-factors due to multiple real emission processes; (iii) there exists an inverse correlation between the number of jets and \(\delta K\), indicating that the addition of jets generally leads to a decrease in \(\delta K\). In addition, our investigation into differential K-factors relative to transverse momentum and invariant mass shows notable increases with higher \(p_T\), but minimal changes with invariant mass. This study highlights the indispensable role of precise K-factor evaluations for accurate interpretations of BSM search outcomes.
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Notes
Concerns may arise regarding processes with high scale uncertainty, exemplified by \(pp \rightarrow \gamma \gamma j\). At LO, this process yields a cross section of \(17.56^{+17.92\%}_{-15.77\%} ~\text{pb}\), while at NLO, it is \(41.11^{+16.15\%}_{-14.38\%}~\text{ pb }\). These computations follow the standard approach, considering nine choices for \(\mu _R\) and \(\mu _F\): \((\mu _R,\mu _F) = (\mu _0/2,\mu _0/2)\), \((\mu _0/2,\mu _0)\), \((\mu _0/2, 2\mu _0)\), \((\mu _0,\mu _0/2)\), \((\mu _0,\mu _0)\), \((\mu _0, 2\mu _0)\), \((2\mu _0,\mu _0/2)\), \((2\mu _0,\mu _0)\), \((2\mu _0, 2\mu _0)\). However, the uncertainty in the \(K\)-factor is remarkably reduced: \(K(\gamma \gamma j) = 2.34^{+5.66\%}_{-3.54\%}\)
For the sake of simplicity in our discussions, contributions from \(c\bar{s} \rightarrow \gamma W^+\), while not negligible, are not mentioned
The \(p_T^j\) dependence of \(K\)-factor was extensively studied in Ref. [56]
Event counts at the \(p_T\) threshold were adjusted to align with the differential cross sections.
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This paper was supported by Konkuk University in 2023.
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Kim, D., Lee, S., Jung, H. et al. A panoramic study of K-factors for 111 processes at the 14 TeV LHC. J. Korean Phys. Soc. (2024). https://doi.org/10.1007/s40042-024-01072-0
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DOI: https://doi.org/10.1007/s40042-024-01072-0