List of ISOLDE experimental setups | |
---|---|
COLLAPS, CRIS, EC-SLI, IDS, ISS, ISOLTRAP, LUCRECIA, Miniball, MIRACLS, SEC, VITO, WISArD | |
Other facilities | |
MEDICIS | Medical Isotopes Collected from ISOLDE |
508 | Solid State Physics Laboratory |
The Weak Interaction Studies with 32Ar Decay (WISArD) experiment is a permanent experimental setup located in the ISOLDE facility, at CERN. The purpose of the experiment is to investigate the weak interaction by looking for beta-delayed protons emitted from a nucleus. [1] In the absence of online isotope production during Long Shutdown 2, the experimental setup has also been used to measure the shape of the beta energy spectrum. [2] A goal of the experiment is to search for physics beyond the Standard Model (SM) by expanding the existing limits on currents in the weak interaction. [3]
The WISArD experimental setup reutilises the WITCH experiment's superconducting magnet and existing infrastructure. [4] [3]
The Standard Model describes three of the four fundamental interactions and classifies all known elementary particles. Whilst being essentially confirmed by the discovery of the Higgs boson, there are still many unanswered questions, specifically regarding the weak interaction. The Standard Model proposes a specific Vector – Axial Vector (V – A) formalism for the weak interaction, however other contributions are not excluded by theory. Measurements of well-selected beta decays, such as pure Fermi (F) or pure Gamow-Teller (GT) decays, may provide experimental evidence for these other contributions, as beta decays cause minimal disturbances from effects relating to nuclear structure and the pure transitions are independent of underlying nuclear interactions. [3] [5]
By determining the momentum of the beta particle and the neutrino, a correlation coefficient that quantifies the extent of non-SM contributions can be determined. [3] However, it is essentially impossible to observe and measure the neutrino in this kind of experiment. Its characteristics can be determined from three-body kinematics by measuring the beta particle and the recoil of the beta-decay daughter. In the WISArD experiment, the measurement of the recoil is replaced by the measurements of the characteristics of protons emitted by the recoiling nucleus. By comparing the energy of the protons emitted, in the same and in opposite hemispheres of the experimental setup with respect to the beta particle, a kinematical shift between the two cases can be measured. This kinematical shift carries the information needed to deduce the beta-neutrino correlation and thus provides access to physics beyond the Standard Model. [6] [7] [3]
Alternatively, the non-SM contributions can be studied by performing a very precise measurement of the shape of the continuous beta energy spectrum. In a detector, beta particles undergo large-angle deflections along their tracks and a particle that entered a detector may undergo sufficient deflection to re-emerge from the same surface. This is known as backscattering, and is an intrinsic limitation in conventional spectrum shape measurements. In WISArD this problem is mitigated by installing two detectors face-to-face in a high magnetic field, effectively guiding the backscattered beta particle towards the opposing detector. [2]
A radioactive ion beam (RIB) of the argon isotope 32Ar is produced at the ISOLDE facility in a spallation reaction (target bombarded by high-energy particles), followed by the heat diffusion of argon atoms from the target. [3] The beam is extracted and accelerated before being mass separated by the High Resolution Separator (HRS) or General Purpose Separator (GPS). [6] [3] This beam is then sent to the WISArD experimental setup via beamlines. [6]
The WISArD beam transport system consists of ion-source (IBL), horizontal (HBL), vertical (VBL) and solenoid magnet (SBL) beamlines. The IBL provides a stable ion beam and consists of an ionising unit, a conical graphite cylinder, an extraction electrode and an extraction lens. The HBL transports the RIBs to subsequent sections formed from two kicker-bender assemblies and a high-voltage Einzel lens. The VBL uses cylindrically shaped electrodes to focus and inject the beam into the SBL region, with the penultimate electrode used as an Einzel lens. [3] [8] The superconducting magnet section produces fields up to 9 T using the former WITCH magnet and surrounds a vacuum tube. [9]
The detection setup (DSet2018) consists of four aluminium rods to both support the detectors and constrain the assembly. Additionally, there is a scintillation detector used for beta particle detection, silicon detectors to detect beta-delayed protons, a catcher foil for implanting the radioactive argon beam on, and a 208Po alpha source. [3] The catcher foil is placed in the centre of the magnetic field, with four silicon detectors positioned above and four below. [10] Positrons are guided to the scintillation detector by the magnetic field. [6]
Following the initial run of WISArD in 2018, several upgrades were made to the setup. [3]
The total transport efficiency of the ion-beam system was improved from 12% to close to 90% from Nov2018 to Upg2021. [7] This was done by optimising the electrostatic elements of the beamline, and reducing the effect of the fringe fields (outer magnetic fields) by focusing the beam prior to it entering the fringe field region. [3]
New silicon detectors were tailor-made for the experiment, improving the solid angle coverage and energy resolution. Additionally, a modification of the plastic scintillation detector was made to lower the detection threshold and therefore limit the effect of backscattering. [7] [3] Furthermore, a better compact microchannel plate (MCP) was designed to measure the position and the extension of the argon beam, information needed for reaching a desired precision level for the correlation coefficient. [3]
The results from the first beta-neutrino correlation campaign with 32Ar in November 2018 showed the proof-of-principle by successfully measuring the proton kinematic energy shift and testing the system. [6] The new test run in 2021 showed that all components of the new setup work and improvements with respect to the first campaign could be achieved. [3] It is foreseen that the full scale experiment with 32Ar will run in the first half of 2024.
In November and December 2020, a first beta spectrum shape measurement was performed with 114In. This yielded the first experimental determination of the weak magnetism form factor, which contains the major part of the effect of the strong interaction on the weak interaction-driven beta decay, for such a heavy nucleus. [2] The result is in agreement with that of a twin-experiment using instead a multi-wire drift chamber based beta spectrometer. [11]
A muon is an elementary particle similar to the electron, with an electric charge of −1 e and spin-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.
A neutrino is an elementary particle that interacts 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.
In particle physics, the W and Z bosons are vector bosons that are together known as the weak bosons or more generally as the intermediate vector bosons. These elementary particles mediate the weak interaction; the respective symbols are
W+
,
W−
, and
Z0
. The
W±
bosons have either a positive or negative electric charge of 1 elementary charge and are each other's antiparticles. The
Z0
boson is electrically neutral and is its own antiparticle. The three particles each have a spin of 1. The
W±
bosons have a magnetic moment, but the
Z0
has none. All three of these particles are very short-lived, with a half-life of about 3×10−25 s. Their experimental discovery was pivotal in establishing what is now called the Standard Model of particle physics.
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.
The Cowan–Reines neutrino experiment was conducted by physicists Clyde Cowan and Frederick Reines in 1956. The experiment confirmed the existence of neutrinos. Neutrinos, subatomic particles with no electric charge and very small mass, had been conjectured to be an essential particle in beta decay processes in the 1930s. With neither mass nor charge, such particles appeared to be impossible to detect. The experiment exploited a huge flux of electron antineutrinos emanating from a nearby nuclear reactor and a detector consisting of large tanks of water. Neutrino interactions with the protons of the water were observed, verifying the existence and basic properties of this particle for the first time.
In nuclear physics, double beta decay is a type of radioactive decay in which two neutrons are simultaneously transformed into two protons, or vice versa, inside an atomic nucleus. As in single beta decay, this process allows the atom to move closer to the optimal ratio of protons and neutrons. As a result of this transformation, the nucleus emits two detectable beta particles, which are electrons or positrons.
The ISOLDE Radioactive Ion Beam Facility, is an on-line isotope separator facility located at the centre of the CERN accelerator complex on the Franco-Swiss border. Created in 1964, the ISOLDE facility started delivering radioactive ion beams (RIBs) to users in 1967. Originally located at the Synchro-Cyclotron (SC) accelerator, the facility has been upgraded several times most notably in 1992 when the whole facility was moved to be connected to CERN's ProtonSynchroton Booster (PSB). ISOLDE is currently the longest-running facility in operation at CERN, with continuous developments of the facility and its experiments keeping ISOLDE at the forefront of science with RIBs. ISOLDE benefits a wide range of physics communities with applications covering nuclear, atomic, molecular and solid-state physics, but also biophysics and astrophysics, as well as high-precision experiments looking for physics beyond the Standard Model. The facility is operated by the ISOLDE Collaboration, comprising CERN and sixteen (mostly) European countries. As of 2019, close to 1,000 experimentalists around the world are coming to ISOLDE to perform typically 50 different experiments per year.
Main injector neutrino oscillation search (MINOS) was a particle physics experiment designed to study the phenomena of neutrino oscillations, first discovered by a Super-Kamiokande (Super-K) experiment in 1998. Neutrinos produced by the NuMI beamline at Fermilab near Chicago are observed at two detectors, one very close to where the beam is produced, and another much larger detector 735 km away in northern Minnesota.
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.
The Kamioka Observatory, Institute for Cosmic Ray Research, University of Tokyo is a neutrino and gravitational waves laboratory located underground in the Mozumi mine of the Kamioka Mining and Smelting Co. near the Kamioka section of the city of Hida in Gifu Prefecture, Japan. A set of groundbreaking neutrino experiments have taken place at the observatory over the past two decades. All of the experiments have been very large and have contributed substantially to the advancement of particle physics, in particular to the study of neutrino astronomy and neutrino oscillation.
WITCH, or experiment IS433, was a double Penning trap experiment to measure the recoil energy of decaying nuclei. A spectrometer in combination with a position-sensitive microchannel plate detector (MCP) was used to count ions while scanning their energy. The experiment was located at the ISOLDE Radioactive Ion Beam Facility in CERN. The beam from ISOLDE was bunched by REXTRAP after which it was transferred to the WITCH set-up.
Borexino is a deep underground particle physics experiment to study low energy (sub-MeV) solar neutrinos. The detector is the world's most radio-pure liquid scintillator calorimeter and is protected by 3,800 meters of water-equivalent depth. The scintillator is pseudocumene and PPO which is held in place by a thin nylon sphere. It is placed within a stainless steel sphere which holds the photomultiplier tubes (PMTs) used as signal detectors and is shielded by a water tank to protect it against external radiation. Outward pointing PMT's look for any outward facing light flashes to tag incoming cosmic muons that manage to penetrate the overburden of the mountain above. Neutrino energy can be determined through the number of photoelectrons measured in the PMT's. While the position can be determined by extrapolating the difference in arrival times of photons at PMT's throughout the chamber.
Ettore Fiorini was an Italian experimental particle physicist. He studied the physics of the weak interaction and was a pioneer in the field of double beta decay. He served as a professor of nuclear and subnuclear physics at the University of Milano-Bicocca.
]
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.
Monitored neutrino beams are facilities for the production of neutrinos with unprecedented control of the flux of particles created inside and outside the facility.
In particle physics, the coincidence method is an experimental design through which particle detectors register two or more simultaneous measurements of a particular event through different interaction channels. Detection can be made by sensing the primary particle and/or through the detection of secondary reaction products. Such a method is used to increase the sensitivity of an experiment to a specific particle interaction, reducing conflation with background interactions by creating more degrees of freedom by which the particle in question may interact. The first notable use of the coincidence method was conducted in 1924 by the Bothe–Geiger coincidence experiment.
The ISOLDE Decay Station (IDS) is a permanent experiment located in the ISOLDE facility at CERN. The purpose of the experiment is to measure decay properties of radioactive isotopes using spectroscopy techniques for a variety of applications, including nuclear engineering and astrophysics. The experimental setup has been operational since 2014.
The high-precision mass spectrometer ISOLTRAP experiment is a permanent experimental setup located at the ISOLDE facility at CERN. The purpose of the experiment is to make precision mass measurements using the time-of-flight (ToF) detection technique. Studying nuclides and probing nuclear structure gives insight into various areas of physics, including astrophysics.
The Versatile Ion polarisation Technique Online (VITO) experiment is a permanent experimental setup located in the ISOLDE facility at CERN, in the form of a beamline. The purpose of the beamline is to perform a wide range of studies using spin-polarised short-lived atomic nuclei. VITO uses circularly-polarised laser light to obtain polarised radioactive beams of different isotopes delivered by ISOLDE. These have already been used for weak-interaction studies, biological investigations, and more recently nuclear structure research. The beamline is located at the site of the former Ultra High Vacuum (UHV) beamline hosting ASPIC.