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Polarized ZZ pairs in gluon fusion and vector boson fusion at the LHC
Pair production of helicity-polarized weak bosons \((V_\lambda=W^\pm_\lambda, Z_\lambda)\) from gluon fusion \((gg\to V_\lambda V'_{\lambda'})\) and weak boson fusion \((V_1V_2\to V_\lambda V'_{\lambda'})\) are powerful probes of the Standard Model, new physics, and properties of...
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Published in: | arXiv.org 2024-06 |
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Main Authors: | , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | Pair production of helicity-polarized weak bosons \((V_\lambda=W^\pm_\lambda, Z_\lambda)\) from gluon fusion \((gg\to V_\lambda V'_{\lambda'})\) and weak boson fusion \((V_1V_2\to V_\lambda V'_{\lambda'})\) are powerful probes of the Standard Model, new physics, and properties of quantum systems. Measuring cross sections of polarized processes is a chief objective of the Large Hadron Collider's (LHC) Run 3 and high luminosity programs, but progress is limited by the simulation tools that are presently available. We propose a method for computing polarized cross sections that works by directly modifying Feynman rules instead of (squared) amplitudes. The method is applicable to loop-induced processes, and can capture the interference between arbitrary polarization configurations, interference with non-resonant diagrams, as well as off-shell/finite-width effects. By construction, previous results that work at the (squared) amplitude level are recoverable. As a demonstration, we report the prospect of observing and studying polarized \(Z_\lambda Z_{\lambda'}\) pairs when produced via gluon fusion and electroweak processes in final-states with four charged leptons at the LHC, using the new method to simulate the gluon fusion process. Our Feynman rules are publicly available as a set of \textit{Universal FeynRules Object} libraries called \texttt{SM\_Loop\_VPolar}. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.2401.17365 |