Measuring the electron Yukawa coupling via resonant s-channel Higgs production at FCC-ee
Abstract
The Future Circular Collider (FCC-ee) offers the unique opportunity of studying the Higgs Yukawa coupling to the electron, \(y_\mathrm {e}\), via resonant s-channel production, \(\mathrm {e^+e^-}\rightarrow \mathrm {H}\), in a dedicated run at \(\sqrt{s} = m_\mathrm {H}\). The signature for direct Higgs production is a small rise in the cross sections for particular final states, consistent with Higgs decays, over the expectations for their occurrence due to Standard Model (SM) background processes involving \(\mathrm {Z}^*\), \(\gamma ^*\), or t-channel exchanges alone. Performing such a measurement is remarkably challenging for four main reasons. First, the low value of the e\(^\pm \) mass leads to a tiny \(y_\mathrm {e}\) coupling and correspondingly small cross section: \(\sigma _\mathrm {ee\rightarrow H} \propto m_\mathrm {e}^2 = 0.57\) fb accounting for initial-state \(\gamma \) radiation. Second, the \(\mathrm {e^+e^-}\) beams must be monochromatized such that the spread of their centre-of-mass (c.m.) energy is commensurate with the narrow width of the SM Higgs boson, \(\varGamma _\mathrm {H} = 4.1\) MeV, while keeping large beam luminosities. Third, the Higgs mass must also be known beforehand with a few-MeV accuracy in order to operate the collider at the resonance peak, \(\sqrt{s} = m_\mathrm {H}\). Last but not least, themore »
- Authors:
-
- European Organization for Nuclear Research (CERN), Geneva (Switzerland)
- Ludwig Maximilian Univ. of Munich, Munich (Germany)
- SLAC National Accelerator Lab., Menlo Park, CA (United States)
- Publication Date:
- Research Org.:
- SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States)
- Sponsoring Org.:
- USDOE Office of Science (SC), Basic Energy Sciences (BES)
- OSTI Identifier:
- 1856255
- Grant/Contract Number:
- AC02-76SF00515
- Resource Type:
- Accepted Manuscript
- Journal Name:
- European Physical Journal Plus
- Additional Journal Information:
- Journal Volume: 137; Journal Issue: 2; Journal ID: ISSN 2190-5444
- Publisher:
- Springer
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
Citation Formats
d’Enterria, David, Poldaru, Andres, and Wojcik, George. Measuring the electron Yukawa coupling via resonant s-channel Higgs production at FCC-ee. United States: N. p., 2022.
Web. doi:10.1140/epjp/s13360-021-02204-2.
d’Enterria, David, Poldaru, Andres, & Wojcik, George. Measuring the electron Yukawa coupling via resonant s-channel Higgs production at FCC-ee. United States. https://doi.org/10.1140/epjp/s13360-021-02204-2
d’Enterria, David, Poldaru, Andres, and Wojcik, George. Fri .
"Measuring the electron Yukawa coupling via resonant s-channel Higgs production at FCC-ee". United States. https://doi.org/10.1140/epjp/s13360-021-02204-2. https://www.osti.gov/servlets/purl/1856255.
@article{osti_1856255,
title = {Measuring the electron Yukawa coupling via resonant s-channel Higgs production at FCC-ee},
author = {d’Enterria, David and Poldaru, Andres and Wojcik, George},
abstractNote = {The Future Circular Collider (FCC-ee) offers the unique opportunity of studying the Higgs Yukawa coupling to the electron, \(y_\mathrm {e}\), via resonant s-channel production, \(\mathrm {e^+e^-}\rightarrow \mathrm {H}\), in a dedicated run at \(\sqrt{s} = m_\mathrm {H}\). The signature for direct Higgs production is a small rise in the cross sections for particular final states, consistent with Higgs decays, over the expectations for their occurrence due to Standard Model (SM) background processes involving \(\mathrm {Z}^*\), \(\gamma ^*\), or t-channel exchanges alone. Performing such a measurement is remarkably challenging for four main reasons. First, the low value of the e\(^\pm \) mass leads to a tiny \(y_\mathrm {e}\) coupling and correspondingly small cross section: \(\sigma _\mathrm {ee\rightarrow H} \propto m_\mathrm {e}^2 = 0.57\) fb accounting for initial-state \(\gamma \) radiation. Second, the \(\mathrm {e^+e^-}\) beams must be monochromatized such that the spread of their centre-of-mass (c.m.) energy is commensurate with the narrow width of the SM Higgs boson, \(\varGamma _\mathrm {H} = 4.1\) MeV, while keeping large beam luminosities. Third, the Higgs mass must also be known beforehand with a few-MeV accuracy in order to operate the collider at the resonance peak, \(\sqrt{s} = m_\mathrm {H}\). Last but not least, the cross sections of the background processes are many orders-of-magnitude larger than those of the Higgs decay signals. A preliminary generator-level study of 11 Higgs decay channels using a multivariate analysis, which exploits boosted decision trees to discriminate signal and background events, identifies two final states as the most promising ones in terms of statistical significance: \(\mathrm {H}\rightarrow gg\) and \(\mathrm {H}\rightarrow \mathrm {W}\mathrm {W}^*\!\rightarrow \ell \nu \) + 2 jets. For a benchmark monochromatization with 4.1-MeV c.m. energy spread (leading to \(\sigma _\mathrm {ee\rightarrow H} = 0.28\) fb) and 10 ab\(^{-1}\) of integrated luminosity, a \(1.3\sigma \) signal significance can be reached, corresponding to an upper limit on the e\(^\pm \) Yukawa coupling at 1.6 times the SM value: |ye| < 1.6|yeSM| at 95% confidence level, per FCC-ee interaction point per year. Directions for future improvements of the study are outlined.},
doi = {10.1140/epjp/s13360-021-02204-2},
journal = {European Physical Journal Plus},
number = 2,
volume = 137,
place = {United States},
year = {Fri Feb 04 00:00:00 EST 2022},
month = {Fri Feb 04 00:00:00 EST 2022}
}
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