ENUBET

Last updated

The Enhanced NeUtrino BEams from kaon Tagging or ENUBET [1] is an ERC funded project [2] that aims at producing an artificial neutrino beam in which the flavor, flux and energy of the produced neutrinos are known with unprecedented precision.

Interest in these types of high precision neutrino beams has grown significantly in the last ten years, [3] especially after the start of the construction of the DUNE and Hyper-Kamiokande detectors. DUNE and Hyper-Kamiokande are aimed at discovering CP violation in neutrinos observing a small difference between the probability of a muon-neutrino to oscillate into an electron-neutrino and the probability of a muon-antineutrino to oscillate into an electron-antineutrino. This effect points toward a difference in the behavior of matter and antimatter. In quantum field theory, this effect is described by a violation of the CP symmetry in particle physics.

The experiments that will measure CP violation need a very precise knowledge of the neutrino cross-sections, i.e. the probability for a neutrino to interact in the detector. [4] This probability is measured counting the number of interacting neutrinos divided by the flux of incoming neutrinos. Current neutrino cross-section experiments are limited by large uncertainties in the neutrino flux. A new generation of cross-section experiment is therefore needed to overcome these limitations with new techniques or high precision beams, as ENUBET. [5] [6]

In ENUBET, neutrinos are produced by focusing mesons in a narrow band beam towards an instrumented decay tunnel, where charged leptons produced in association with neutrinos by mesons' decay can be monitored at the single particle level. Beams like ENUBET are called monitored neutrino beams.

Mesons (essentially pions and kaons) are produced in the interactions of accelerated protons with a Beryllium or Graphite target. The proposed facility is being studied taking into account the energies of currently available proton drivers: 400 GeV (CERN SPS), 120 GeV (FNAL Main Injector), 30 GeV (J-PARC Main Ring).

Kaons and pions are momentum and charge selected in a short transfer line by means of dipole and quadrupole magnets and are focused in a collimated beam into an instrumented decay tube. Large angle muons and positrons from kaon decays (, , ) are measured by detectors on the tunnel walls, while muons from pion decays () are monitored after the hadron dump at the end of the tunnel. The decay region is kept short (40 m) in order to reduce the neutrino contamination from muon decays ().

In this way, the neutrino flux is assessed in a direct way with a precision of 1%, without relying on complex simulations of the transfer line and on hadro-production data extrapolation that currently limits the knowledge of the flux to 5-10%. [7] The ENUBET facility can be used to perform precision studies of the neutrino cross section and of sterile neutrinos or Non-Standard Interaction models. This method can also be extended to detect other leptons in order to have a complete monitored neutrino beam. [8]

The ENUBET project started in 2016. As of 2024, it involves 17 European institutions in 5 European countries and brings together about 80 scientists. ENUBET studies all technical and physics challenges to demonstrate the feasibility of a monitored neutrino beam: [9] it has build a full-scale demonstrator of the instrumented decay tunnel (3 m length and partial azimuthal coverage) and assesses costs and physics reach of the proposed facility. The first end-to-end simulation of the ENUBET monitored neutrino beam was published in 2023. [10]

The ENUBET ERC project was completed in 2022. Since March 2019, ENUBET has been part of the CERN Neutrino Platform [11] (NP06/ENUBET) for the development of a new generation of neutrino detectors and facilities.

Related Research Articles

<span class="mw-page-title-main">Muon</span> Subatomic particle

A muon is an elementary particle similar to the electron, with an electric charge of −1 e and a spin of 1/2, but with a much greater mass. It is classified as a lepton. As with other leptons, the muon is not thought to be composed of any simpler particles.

<span class="mw-page-title-main">Pionium</span>

Pionium is a composite particle consisting of one
π+
and one
π
meson. It can be created, for instance, by interaction of a proton beam accelerated by a particle accelerator and a target nucleus. Pionium has a short lifetime, predicted by chiral perturbation theory to be 2.89×10−15 s. It decays mainly into two
π0
mesons, and to a smaller extent into two photons.

<span class="mw-page-title-main">Lepton</span> Class of elementary particles

In particle physics, a lepton is an elementary particle of half-integer spin that does not undergo strong interactions. Two main classes of leptons exist: charged leptons, including the electron, muon, and tauon, and neutral leptons, better known as neutrinos. Charged leptons can combine with other particles to form various composite particles such as atoms and positronium, while neutrinos rarely interact with anything, and are consequently rarely observed. The best known of all leptons is the electron.

<span class="mw-page-title-main">Tau (particle)</span> Elementary subatomic particle with negative electric charge

The tau, also called the tau lepton, tau particle, tauon or tau electron, is an elementary particle similar to the electron, with negative electric charge and a spin of 1/2. Like the electron, the muon, and the three neutrinos, the tau is a lepton, and like all elementary particles with half-integer spin, the tau has a corresponding antiparticle of opposite charge but equal mass and spin. In the tau's case, this is the "antitau". Tau particles are denoted by the symbol
τ
and the antitaus by 
τ+
.

<span class="mw-page-title-main">Gargamelle</span> CERN Bubble chamber particle detector

Gargamelle was a heavy liquid bubble chamber detector in operation at CERN between 1970 and 1979. It was designed to detect neutrinos and antineutrinos, which were produced with a beam from the Proton Synchrotron (PS) between 1970 and 1976, before the detector was moved to the Super Proton Synchrotron (SPS). In 1979 an irreparable crack was discovered in the bubble chamber, and the detector was decommissioned. It is currently part of the "Microcosm" exhibition at CERN, open to the public.

<span class="mw-page-title-main">Jack Steinberger</span> German-American physicist, Nobel laureate (1921–2020)

Jack Steinberger was a German-born American physicist noted for his work with neutrinos, the subatomic particles considered to be elementary constituents of matter. He was a recipient of the 1988 Nobel Prize in Physics, along with Leon M. Lederman and Melvin Schwartz, for the discovery of the muon neutrino. Through his career as an experimental particle physicist, he held positions at the University of California, Berkeley, Columbia University (1950–68), and the CERN (1968–86). He was also a recipient of the United States National Medal of Science in 1988, and the Matteucci Medal from the Italian Academy of Sciences in 1990.

<span class="mw-page-title-main">LHCb experiment</span> Experiment at the Large Hadron Collider

The LHCb experiment is a particle physics detector experiment collecting data at the Large Hadron Collider at CERN. LHCb is a specialized b-physics experiment, designed primarily to measure the parameters of CP violation in the interactions of b-hadrons. Such studies can help to explain the matter-antimatter asymmetry of the Universe. The detector is also able to perform measurements of production cross sections, exotic hadron spectroscopy, charm physics and electroweak physics in the forward region. The LHCb collaborators, who built, operate and analyse data from the experiment, are composed of approximately 1650 people from 98 scientific institutes, representing 22 countries. Vincenzo Vagnoni succeeded on July 1, 2023 as spokesperson for the collaboration from Chris Parkes. The experiment is located at point 8 on the LHC tunnel close to Ferney-Voltaire, France just over the border from Geneva. The (small) MoEDAL experiment shares the same cavern.

<span class="mw-page-title-main">Neutrino oscillation</span> Phenomenon in which a neutrino changes lepton flavor as it travels

Neutrino oscillation is a quantum mechanical phenomenon in which a neutrino created with a specific lepton family number can later be measured to have a different lepton family number. The probability of measuring a particular flavor for a neutrino varies between three known states, as it propagates through space.

<span class="mw-page-title-main">Neutrinoless double beta decay</span> A nuclear physics process that has yet to observed

Neutrinoless double beta decay (0νββ) is a commonly proposed and experimentally pursued theoretical radioactive decay process that would prove a Majorana nature of the neutrino particle. To this day, it has not been found.

<span class="mw-page-title-main">Muon spin spectroscopy</span>

Muon spin spectroscopy, also known as µSR, is an experimental technique based on the implantation of spin-polarized muons in matter and on the detection of the influence of the atomic, molecular or crystalline surroundings on their spin motion. The motion of the muon spin is due to the magnetic field experienced by the particle and may provide information on its local environment in a very similar way to other magnetic resonance techniques, such as electron spin resonance and, more closely, nuclear magnetic resonance (NMR).

T2K is a particle physics experiment studying the oscillations of the accelerator neutrinos. The experiment is conducted in Japan by the international cooperation of about 500 physicists and engineers with over 60 research institutions from several countries from Europe, Asia and North America and it is a recognized CERN experiment (RE13). T2K collected data within its first phase of operation from 2010 till 2021. The second phase of data taking is expected to start in 2023 and last until commencement of the successor of T2K – the Hyper-Kamiokande experiment in 2027.

<span class="mw-page-title-main">Hyper-Kamiokande</span> Neutrino observatory in Japan

Hyper-Kamiokande is a neutrino observatory and experiment under construction in Hida, Gifu and in Tokai, Ibaraki in Japan. It is conducted by the University of Tokyo and the High Energy Accelerator Research Organization (KEK), in collaboration with institutes from over 20 countries across six continents. As a successor of the Super-Kamiokande and T2K experiments, it is designed to search for proton decay and detect neutrinos from natural sources such as the Earth, the atmosphere, the Sun and the cosmos, as well as to study neutrino oscillations of the man-made accelerator neutrino beam. The beginning of data-taking is planned for 2027.

<span class="mw-page-title-main">NOvA</span> Observatory

The NOνA experiment is a particle physics experiment designed to detect neutrinos in Fermilab's NuMI beam. Intended to be the successor to MINOS, NOνA consists of two detectors, one at Fermilab, and one in northern Minnesota. Neutrinos from NuMI pass through 810 km of Earth to reach the far detector. NOνA's main goal is to observe the oscillation of muon neutrinos to electron neutrinos. The primary physics goals of NOvA are:

<span class="mw-page-title-main">NA62 experiment</span>

The NA62 experiment is a fixed-target particle physics experiment in the North Area of the SPS accelerator at CERN. The experiment was approved in February 2007. Data taking began in 2015, and the experiment is expected to become the first in the world to probe the decays of the charged kaon with probabilities down to 10−12. The experiment's spokesperson is Cristina Lazzeroni. The collaboration involves 333 individuals from 30 institutions and 13 countries around the world.

The K2K experiment was a neutrino experiment that ran from June 1999 to November 2004. It used muon neutrinos from a well-controlled and well-understood beam to verify the oscillations previously observed by Super-Kamiokande using atmospheric neutrinos. This was the first positive measurement of neutrino oscillations in which both the source and detector were fully under experimenters' control. Previous experiments relied on neutrinos from the Sun or from cosmic sources. The experiment found oscillation parameters which were consistent with those measured by Super-Kamiokande.

MINOS+ was a continuation of the MINOS experiment to measure neutrino oscillation with improved electronics. It started taking data in 2013 and ran for 3 years. The experiment has ended and a 6-month dismantling project began in early October 2016.

<span class="mw-page-title-main">Accelerator Neutrino Neutron Interaction Experiment</span> Water Cherenkov detector experiment

The Accelerator Neutrino Neutron Interaction Experiment (ANNIE) is a proposed water Cherenkov detector experiment designed to examine the nature of neutrino interactions. This experiment will study phenomena like proton decay, and neutrino oscillations, by analyzing neutrino interactions in gadolinium-loaded water and measuring their neutron yield. Neutron Tagging plays an important role in background rejection from atmospheric neutrinos. By implementing early prototypes of LAPPDs, high precision timing is possible. The suggested location for ANNIE is the SciBooNE hall on the Booster Neutrino Beam associated with the MiniBooNE experiment. The neutrino beam originates in Fermilab where The Booster delivers 8 GeV protons to a beryllium target producing secondary pions and kaons. These secondary mesons decay to produce a neutrino beam with an average energy of around 800 MeV. ANNIE will begin installation in the summer of 2015. Phase I of ANNIE, mapping the neutron background, completed in 2017. The detector is being upgraded for full science operation which is expected to begin late 2018.

<span class="mw-page-title-main">FASER experiment</span> 2022 particle physics experiment at the Large Hadron Collider at CERN

FASER is one of the nine particle physics experiments in 2022 at the Large Hadron Collider at CERN. It is designed to both search for new light and weakly coupled elementary particles, and to detect and study the interactions of high-energy collider neutrinos. In 2023, FASER and SND@LHC reported the first observation of collider neutrinos.

An accelerator neutrino is a human-generated neutrino or antineutrino obtained using particle accelerators, in which beam of protons is accelerated and collided with a fixed target, producing mesons which then decay into neutrinos. Depending on the energy of the accelerated protons and whether mesons decay in flight or at rest it is possible to generate neutrinos of a different flavour, energy and angular distribution. Accelerator neutrinos are used to study neutrino interactions and neutrino oscillations taking advantage of high intensity of neutrino beams, as well as a possibility to control and understand their type and kinematic properties to a much greater extent than for neutrinos from other sources.

Monitored neutrino beams are facilities for the production of neutrinos with unprecedented control of the flux of particles created inside and outside the facility.

References

  1. "ENUBET - Enhanced NeUtrino BEams from kaon Tagging". enubet.pd.infn.it. Retrieved 2019-12-07.
  2. "ERC grant agreement ID: 681647".
  3. Katori, T. (2018). "Neutrino–nucleus cross sections for oscillation experiments". J. Phys. G. 45 (1): 013001. arXiv: 1611.07770 . Bibcode:2018JPhG...45a3001K. doi:10.1088/1361-6471/aa8bf7. S2CID   119468689.
  4. Ankowski, A. M.; Mariani, C. (2017). "Systematic uncertainties in long-baseline neutrino-oscillation experiments". J. Phys. G. 44 (5): 054001. arXiv: 1609.00258 . Bibcode:2017JPhG...44e4001A. doi:10.1088/1361-6471/aa61b2. S2CID   59414695.
  5. Mezzetto, M (2018). "Other future accelerator experiments". doi:10.5281/zenodo.1286826.{{cite journal}}: Cite journal requires |journal= (help)
  6. Dell'Acqua, Andrea; Aduszkiewicz, Antoni; Ahlers, Markus; Aihara, Hiroaki; Alion, Tyler; Saul Alonso Monsalve; Luis Alvarez Ruso; Antonelli, Vito; Babicz, Marta; Anastasia Maria Barbano; Pasquale di Bari; Baussan, Eric; Bellini, Vincenzo; Berardi, Vincenzo; Blondel, Alain; Bonesini, Maurizio; Booth, Alexander; Bordoni, Stefania; Boyarsky, Alexey; Boyd, Steven; Bross, Alan D.; Brunner, Juergen; Carlile, Colin; Catanesi, Maria-Gabriella; Christodoulou, Georgios; Coan, Thomas; Cussans, David; Patrick Decowski, M.; Albert De Roeck; et al. (2018). "Future Opportunities in Accelerator-based Neutrino Physics". arXiv: 1812.06739 [hep-ex].
  7. Soplin, Leonidas Aliaga (2016-01-01). "Neutrino Flux Prediction for the NuMI Beamline". doi:10.2172/1254643.{{cite journal}}: Cite journal requires |journal= (help)
  8. Longhin, A.; Ludovici, L.; Terranova, F. (2015). "A novel technique for the measurement of the electron neutrino cross section". Eur. Phys. J. C. 75 (4): 155. arXiv: 1412.5987 . Bibcode:2015EPJC...75..155L. doi:10.1140/epjc/s10052-015-3378-9. S2CID   52245662.
  9. Acerbi, F.; et al. (26 October 2023). "Design and performance of the ENUBET monitored neutrino beam". The European Physical Journal C. 83 (10): 964. arXiv: 2308.09402 . Bibcode:2023EPJC...83..964A. doi: 10.1140/epjc/s10052-023-12116-3 . hdl: 11379/588907 .
  10. Acerbi, F. (26 October 2023). "Design and performance of the ENUBET monitored neutrino beam". The European Physical Journal C. 83 (10): 964. Bibcode:2023EPJC...83..964A. doi:10.1140/epjc/s10052-023-12116-3.
  11. "CERN Neutrino Platform | CERN". home.cern. Retrieved 2019-12-07.