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  2. Scattering and Neutrino Detector - Wikipedia

    en.wikipedia.org/wiki/Scattering_and_Neutrino...

    The Scattering and Neutrino Detector (SND) at the Large Hadron Collider (LHC), CERN, is an experiment built for the detection of the collider neutrinos. The primary goal of SND is to measure the p+p --> +X process and search for the feebly interacting particles. It will be operational from 2022, during the LHC-Run 3 (2022-2024).

  3. MINERνA - Wikipedia

    en.wikipedia.org/wiki/MINERνA

    Main Injector Experiment for ν-A, or MINERνA, is a neutrino scattering experiment which uses the NuMI beamline at Fermilab.MINERνA seeks to measure low energy neutrino interactions both in support of neutrino oscillation experiments and also to study the strong dynamics of the nucleon and nucleus that affect these interactions.

  4. Neutrino detector - Wikipedia

    en.wikipedia.org/wiki/Neutrino_detector

    A neutrino detector is a physics apparatus which is designed to study neutrinos. Because neutrinos only weakly interact with other particles of matter, neutrino detectors must be very large to detect a significant number of neutrinos. Neutrino detectors are often built underground, to isolate the detector from cosmic rays and other background ...

  5. CONUS-Experiment - Wikipedia

    en.wikipedia.org/wiki/CONUS-Experiment

    CONUS (COherent Neutrino nUcleus Scattering) Experiment is a research project at the commercial nuclear power plant in Brokdorf, Germany (see Figure 1). The CONUS project is sponsored by the Max-Planck-Institut für Kernphysik and Preussen Elektra GmbH .

  6. Neutron spectroscopy - Wikipedia

    en.wikipedia.org/wiki/Neutron_spectroscopy

    This allows the total spin of the unpaired electrons and neutron to be probed. The magnetic scattering length from one electron is b m = 𝛾r 0 = 1.348 fm which is on the same order of magnitude as the nuclear scattering length. Because of the dipole-dipole character of the interaction, the scattering is considered to be anisotropic. [7]

  7. List of neutrino experiments - Wikipedia

    en.wikipedia.org/wiki/List_of_neutrino_experiments

    Coherent Elastic Neutrino Nucleus Scattering (CEvNS) few keV nuclear recoil energy Spallation Neutron Source at Oak Ridge National Laboratory: Nov 2016- CONUS / CONUS+: COherent Neutrino nUcleus Scattering R ν e: ν e + nucleus → ν e + nucleus ES (NC) HPGe Coherent Elastic Neutrino Nucleus Scattering (CEvNS) 4 detectors: 160eV, 170eV, 180eV ...

  8. Time projection chamber - Wikipedia

    en.wikipedia.org/wiki/Time_projection_chamber

    [5] [6] Chen's initial goals with such a detector were to study neutrino-elecron scattering, but the goals evolved to measure solar or cosmic neutrinos or proton decay. [5] [7] [8] In 1977, Carlo Rubbia independently, and nearly simultaneously, proposed to construct an LArTPC at CERN for rare event particle physics experiments. [9] [7]

  9. FASER experiment - Wikipedia

    en.wikipedia.org/wiki/FASER_experiment

    Layout of the FASER detector. Located at the front end of FASER is the FASERν neutrino detector. It consists of many layers of emulsion films interleaved with tungsten plates as target material for neutrino interactions. Behind FASERν and at the entrance to the main detector is a charged particle veto consisting of plastic scintillators.