Skip to content
DraconiticResearch
Search Sources API
197,768 studies31 sourcesUpdated 53 min ago
PreprintCC BY 4.0arXiv

Current and future constraints on heavy New Physics from τ weak dipole moments

Abstract

We study the weak magnetic and electric dipole moments of the τ lepton as precision tests of the Standard Model (SM) and probes of heavy New Physics (NP). We present an updated SM prediction for the τ weak magnetic dipole moment at one loop, including a careful assessment of theoretical uncertainties from electroweak scheme dependence. Working within the SM Effective Field Theory, we derive comprehensive current constraints on the τ dipole operators from a combination of observables: the τ weak and electromagnetic dipole moments, high-mass Drell-Yan tails at the LHC, Z partial decay widths, and the electron electric dipole moment. Finally, we assess the prospects of measuring the SM value of the τ weak magnetic moment at the FCC-ee Tera-Z run, and project the sensitivities of the leading observables to heavy NP at FCC-ee and HL-LHC, incorporating informed assumptions about improvements of systematic uncertainties. We find that the τ weak dipole moments are already among the leading probes of the τ dipole operators, and will become increasingly dominant at future colliders.

Versions

Related

  1. Current and Future Constraints on the Primordial Power Spectrum
    Zachary Cheslog, Emily Finson, Amanda MacInnis +4
    arXivPreprintCC BY 4.0Full textCosmologyHigh-energy & particle physicsarXiv
  2. Dihadron azimuthal asymmetry and light-quark dipole moments at the Electron-Ion Collider
    Xin-Kai Wen, Bin Yan, Zhite Yu +1
    Science China Physics Mechanics and AstronomyPeer-reviewedLicence not statedFull text11 citedHigh-energy & particle physicsOpenAlex
  3. Electric Dipole Moments as Precision Probes of CP-Violating Top-Quark Interactions in SMEFT
    Subhajit Kala, Soumitra Nandi, Sonakshi Saha
    arXivPreprintCC BY 4.0Full textHigh-energy & particle physicsarXiv
  4. Electric Dipole Moments in the CP-violating Generational Three-Higgs-Doublet Model
    Hao-Ran Ma, Ti-Bin Hou, Jin-Lei Yang +1
    arXivPreprintCC BY 4.0Full textHigh-energy & particle physicsarXiv
  5. Bottom quark electroweak dipole moments at a high-energy μ−collider
    D. Barducci
    arXivPreprintarXiv licenceFull textHigh-energy & particle physicsarXiv
BibTeX
@misc{kosnik2026current,
  title = {{Current and future constraints on heavy New Physics from $τ$ weak dipole moments}},
  author = {Nejc Košnik and Zachary Polonsky and Aleks Smolkovič},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2606.07232},
  eprint = {2606.07232},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2606.07232},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Current and future constraints on heavy New Physics from τ weak dipole moments
AU  - Nejc Košnik
AU  - Zachary Polonsky
AU  - Aleks Smolkovič
PY  - 2026
DA  - 2026/09/15
PB  - arXiv
DO  - 10.48550/arxiv.2606.07232
UR  - https://arxiv.org/abs/2606.07232
AB  - We study the weak magnetic and electric dipole moments of the τ lepton as precision tests of the Standard Model (SM) and probes of heavy New Physics (NP). We present an updated SM prediction for the τ weak magnetic dipole moment at one loop, including a careful assessment of theoretical uncertainties from electroweak scheme dependence. Working within the SM Effective Field Theory, we derive comprehensive current constraints on the τ dipole operators from a combination of observables: the τ weak and electromagnetic dipole moments, high-mass Drell-Yan tails at the LHC, Z partial decay widths, and the electron electric dipole moment. Finally, we assess the prospects of measuring the SM value of the τ weak magnetic moment at the FCC-ee Tera-Z run, and project the sensitivities of the leading observables to heavy NP at FCC-ee and HL-LHC, incorporating informed assumptions about improvements of systematic uncertainties. We find that the τ weak dipole moments are already among the leading probes of the τ dipole operators, and will become increasingly dominant at future colliders.
ER  -