Monitored neutrino beam

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

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Accelerator neutrinos

Accelerator neutrino beams are beams of neutrinos produced by particle accelerators. [1] [2] Since neutrinos are neutral particles that feebly interact with matter, monitoring the production rate of neutrinos at accelerators is a major experimental challenge. M. Schwartz and B. Pontecorvo proposed to exploit accelerators to produce neutrinos in 1960. [3] Their ideas brought to the first neutrino experiment where neutrinos were produced by an accelerator from the scattering of protons in a beryllium target. The scattering produces a wealth of particles and, in particular, pions, which decay producing muons and neutrinos. The experiment, first carried out by Lederman, Schwartz, Steinberger and collaborators demonstrated the existence of two neutrino flavors. [4] At that time, protons were not even steered outside the accelerator but the target was inserted close to the proton orbit. The protons in the AGS accelerator of the Brookhaven National Laboratory were brought to strike an internal Be target in a short straight session of the accelerator. Modern experiments steer the protons outside the accelerator and focus the particles produced after the target by magnetic horns or a static focusing system based on quadrupoles and dipoles. The focusing system increases the flux of pions pointing toward the neutrino detector and selects the charge and momentum of these pions. After focusing, pions propagate along a tunnel and decay by reactions like . All undecayed pions and all muons are stopped at the end of the tunnel while the neutrinos cross the wall of the tunnel because their interaction probability is very small. At large distances from the end of the tunnel, no particles are present except for an intense flux of neutrinos.

Diagnostics and flux determination

In early experiments, the flux of neutrinos was estimated by measuring the number of pions produced after the target and monitoring the muons produced at the end of the tunnel. After the discovery of neutrino oscillation, the need for high precision beams fostered the construction of sophisticated monitoring systems. They are based on dedicated experiments to measure the number of particles produced by proton interactions on solid-state targets (beryllium, graphite). The beamline comprises the proton beam, target, focusing system, and decay tunnel, and it is simulated by Monte Carlo methods. Variations of the flux are monitored in real-time by measuring the number of protons impinging on the target and the rate of muons. All these techniques are the basic toolkit of accelerator neutrino physicists and are inherited by beam diagnostics. [5]

Modern monitored neutrino beams

Monitored neutrino beams [6] are beams where diagnostic can directly measure the flux of neutrinos because the experimenters monitor the production of the lepton associated with the neutrino at the single-particle level. For instance, if a muon neutrino is produced by a decay, its appearance is signaled by the observation of the corresponding antimuon. This is a direct estimate because the number of antimuons produced by those decays is equal to the number of muon neutrinos. Similarly, an electron neutrino produced by a kaon decay -for instance - is signaled by the observation of a positron. Monitoring the production of leptons in the decay tunnel of an accelerator neutrino beam is a challenge because the number of leptons and background particles is huge. In the 1980s, monitored neutrino beams were built in the USSR in the framework of the "tagged neutrino beam facility". [7] This facility did not reach a flux sufficient to feed neutrino experiments and was later descoped to a tagged kaon beam facility. Current neutrino beams record muons but they have not reached single-particle sensitivity. Their precision on flux (15%) cannot beat conventional techniques, yet. [8] The most advanced monitored neutrino beam project is ENUBET, which aims at designing a monitored neutrino beam for high precision neutrino cross-section measurements.

Tagged neutrino beams

Monitored neutrino beams detect the charged leptons produced in the decay tunnel but the experimenters do not attempt to identify simultaneously the charged lepton and the neutrino produced by the decay of the parent particle. For example, a decay creates an antimuon that can be detected inside the tunnel by a particle detector. The vast majority of neutrinos cross the tunnel without interacting but a handful of them interacts in the neutrino detector, which is generally located far from the tunnel. If the time resolution of the particle detector in the tunnel and the neutrino detector outside the tunnel is very good (below 1 ns), the experimenters can associate unambiguously the neutrino observed in the detector with the charged lepton recorded in the tunnel. These facilities are called (time) tagged neutrino beams and were proposed by L.N. Hand and B. Pontecorvo in the 1960s. [9] To date, an intense and time-tagged neutrino facility has never been built.

Related Research Articles

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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; that is, it is a fundamental particle.

<span class="mw-page-title-main">Neutrino</span> Elementary particle with extremely low mass

A neutrino is a fermion that interacts only via the weak interaction and gravity. The neutrino is so named because it is electrically neutral and because its rest mass is so small (-ino) that it was long thought to be zero. The rest mass of the neutrino is much smaller than that of the other known elementary particles. The weak force has a very short range, the gravitational interaction is extremely weak due to the very small mass of the neutrino, and neutrinos do not participate in the electromagnetic interaction or the strong interaction. Thus, neutrinos typically pass through normal matter unimpeded and undetected.

<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, and neutral leptons. 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">ATLAS experiment</span> CERN LHC experiment

ATLAS is the largest general-purpose particle detector experiment at the Large Hadron Collider (LHC), a particle accelerator at CERN in Switzerland. The experiment is designed to take advantage of the unprecedented energy available at the LHC and observe phenomena that involve highly massive particles which were not observable using earlier lower-energy accelerators. ATLAS was one of the two LHC experiments involved in the discovery of the Higgs boson in July 2012. It was also designed to search for evidence of theories of particle physics beyond the Standard Model.

<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">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.

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

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

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

Hyper-Kamiokande is a neutrino observatory and experiment under construction, conducted in Japan by the collaboration of institutes from 21 countries from six continents. As a successor of the Super-Kamiokande (SK) 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

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<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.

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

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

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References

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