Anapole moment of neutrinos and radioactive sources near liquid xenon detectors
arXiv:2408.11904 · doi:10.1103/PhysRevD.111.073008
Abstract
We show that placing a radioactive source such as Cr near a liquid xenon detector may allow to detect the contribution induced by the anapole moment to neutrino-electron scattering in the Standard Model at the 1-2 level. Although the anapole moment of neutrinos induces a scattering rate with the same spectral shape as the neutral and charged current contributions, exposures of 60 tonne source run at XENONnT or XLZD may be enough to accumulate sufficient statistics for a detection. We also discuss a simple model where the anapole moment of neutrinos is enhanced or decreased with respect to the SM expectation, further demonstrating how a potential measurement of the anapole moment of neutrinos would allow to constrain new physics.
arXiv commentMatches version published in PRD
References in corpus (42)
- First Dark Matter Search Results from the LUX-ZEPLIN (LZ) Experiment
- Dark Matter Search Results from the PandaX-4T Commissioning Run
- Updated Bounds on Milli-Charged Particles
- First Dark Matter Search with Nuclear Recoils from the XENONnT Experiment
- Measurement of the response of a Ga solar neutrino experiment to neutrinos from an 37Ar source
- Search for New Physics in Electronic Recoil Data from XENONnT
- Measurement of Neutrino-Electron Scattering Cross-Section with a CsI(Tl) Scintillating Crystal Array at the Kuo-Sheng Nuclear Power Reactor
- Dark Radiation constraints on minicharged particles in models with a hidden photon
- Results from the Baksan Experiment on Sterile Transitions (BEST)
- Grand Unified Neutrino Spectrum at Earth: Sources and Spectral Components
- A Next-Generation Liquid Xenon Observatory for Dark Matter and Neutrino Physics
- Neutrino Charge Radii from COHERENT Elastic Neutrino-Nucleus Scattering
- On the charge radius of the neutrino
- The XENONnT Dark Matter Experiment
- Constraints on millicharged neutrinos via analysis of data from atomic ionizations with germanium detectors at sub-keV sensitivities
- Updating neutrino magnetic moment constraints
- On the observability of the neutrino charge radius
- Impact of the Dresden-II and COHERENT neutrino scattering data on neutrino electromagnetic properties and electroweak physics
- Implications of first LZ and XENONnT results: A comparative study of neutrino properties and light mediators
- Can Nonstandard Neutrino Interactions explain the XENON1T spectral excess?
- Bounds on the tau and muon neutrino vector and axial vector charge radius
- New constraint on neutrino magnetic moment and neutrino millicharge from LUX-ZEPLIN dark matter search results
- Light new physics and neutrino electromagnetic interactions in XENONnT
- Revisiting Large Neutrino Magnetic Moments
- Stellar probes of dark sector-photon interactions
- Probing Active to Sterile Neutrino Oscillations in the LENS Detector
- Consequences of the Dresden-II reactor data for the weak mixing angle and new physics
- Effects of neutrino oscillations and neutrino magnetic moments on elastic neutrino-electron scattering
- On a Neutrino Electroweak Radius
- Discovery potential of multi-ton xenon detectors in neutrino electromagnetic properties
- A neutrino floor for the Migdal effect
- Combining dark matter detectors and electron-capture sources to hunt for new physics in the neutrino sector
- Neutrino millicharge and other electromagnetic interactions with COHERENT-2021 data
- The weak mixing angle from low energy neutrino measurements: a global update
- New bounds on neutrino electric millicharge from limits on neutrino magnetic moment
- Neutrino Electromagnetic Properties and the Weak Mixing Angle at the LHC Forward Physics Facility
- Anapole Moment of Majorana Fermions and Implications for Direct Detection of Neutralino Dark Matter
- Testing the Gallium Anomaly
- Dirac Neutrino Anapole Moment
- Neutrino masses and mixing from milli-charged dark matter
- Inverse Tritium Beta Decay with Relic Neutrinos, Solar Neutrinos, and a 51Cr Source
- Production of the artificial 51Cr neutrino source in the BEST project