Skip to content
DraconiticResearch
Search Sources API
194,067 studies31 sourcesUpdated 12 min ago
PreprintCC BY 4.0arXiv

FCC-μe: High Energy, High Luminosity Muon-Electron Collider & Neutrino Factory at CERN

Abstract

The concept is presented of making at the FCC-ee (or CEPC) facility μ+e- collisions at the centre-of-mass energy between 1 and 2 TeV and the average luminosity above 1034cm−2s−1, concurrently to the e+e- collisions. First, a concise scientific motivation is given, including the exciting prospect of measurements of the Higgs boson self-interaction, and is followed by a presentation of the FCC-μe layout -- from the source of ultra-cold anti-muons, through the muon booster, to the main muon ring. Basic considerations are also given regarding the machine-detector interface and the performance of the FCC-μe and associated neutrino factory. The paper concludes with an outlook underlying relevance of such anti-muon beams for any future high energy storage ring as well as for neutrino science.

Related

  1. Precision luminosity measurement in proton-proton collisions at a center-of-mass energy of 13 TeV with the CMS detector at the Large Hadron Collider
    A. Gevorgyan, A. Hayrapetyan, V. Makarenko +2,527
    Physical Review XPeer-reviewedPublisher termsAtomic, molecular & optical physicsCrossref
  2. LHμC: A high energy, high luminosity muon-hadron collider at CERN
    Krzysztof Piotrzkowski
    arXivPreprintCC BY 4.0Full textApplied physics & instrumentationHigh-energy & particle physicsarXiv
  3. Precision luminosity measurement in proton-proton collisions at a center-of-mass energy of 13 TeV with the CMS detector at the Large Hadron Collider
    CMS Collaboration
    arXivPreprintCC BY 4.0Full textApplied physics & instrumentationHigh-energy & particle physicsarXiv
  4. A High-Energy Neutrino Collider within a Muon Collider
    Innes Bigaran, André de Gouvêa, Tao Han +4
    arXivPreprintCC BY 4.0Full textHigh-energy & particle physicsarXiv
  5. Partial reconstruction of the decay Bs0→ ϕ(K+K−)η' (π+π−η) at a future high-luminosity Z factory
    Jeremiah D. Juevesano, Marlon P. Brade, Dennis C. Arogancia +1
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsarXiv
BibTeX
@misc{piotrzkowski2026fccμe,
  title = {{FCC-μe: High Energy, High Luminosity Muon-Electron Collider & Neutrino Factory at CERN}},
  author = {K. Piotrzkowski},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.40451},
  eprint = {2610.40451},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.40451},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - FCC-μe: High Energy, High Luminosity Muon-Electron Collider & Neutrino Factory at CERN
AU  - K. Piotrzkowski
PY  - 2026
DA  - 2026/10/29
PB  - arXiv
DO  - 10.48550/arxiv.2610.40451
UR  - https://arxiv.org/abs/2610.40451
AB  - The concept is presented of making at the FCC-ee (or CEPC) facility μ^+e^- collisions at the centre-of-mass energy between 1 and 2 TeV and the average luminosity above 10^34cm^−2s^−1, concurrently to the e^+e^- collisions. First, a concise scientific motivation is given, including the exciting prospect of measurements of the Higgs boson self-interaction, and is followed by a presentation of the FCC-μe layout -- from the source of ultra-cold anti-muons, through the muon booster, to the main muon ring. Basic considerations are also given regarding the machine-detector interface and the performance of the FCC-μe and associated neutrino factory. The paper concludes with an outlook underlying relevance of such anti-muon beams for any future high energy storage ring as well as for neutrino science.
ER  -