MoEDAL experiment

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Large Hadron Collider
(LHC)
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Plan of the LHC experiments and the preaccelerators.
LHC experiments
ATLAS A Toroidal LHC Apparatus
CMS Compact Muon Solenoid
LHCb LHC-beauty
ALICE A Large Ion Collider Experiment
TOTEM Total Cross Section, Elastic Scattering and Diffraction Dissociation
LHCf LHC-forward
MoEDAL Monopole and Exotics Detector At the LHC
FASER ForwArd Search ExpeRiment
SND Scattering and Neutrino Detector
LHC preaccelerators
p and Pb Linear accelerators for protons (Linac 4) and lead (Linac 3)
(not marked) Proton Synchrotron Booster
PS Proton Synchrotron
SPS Super Proton Synchrotron

MoEDAL (Monopole and Exotics Detector at the LHC) is a particle physics experiment at the Large Hadron Collider (LHC).

Contents

MoEDAL experiment in LHC IP8 at CERN MoEDAL.jpg
MoEDAL experiment in LHC IP8 at CERN

Experiment

MoEDAL shares the cavern at Point 8 with LHCb, and its prime goal is to directly search for the magnetic monopole [1] [2] [3] or dyon and other highly ionizing stable massive particles and pseudo-stable massive particles.

To detect these particles, MoEDAL uses both nuclear track detectors and aluminium trapping volumes. [4] There are approximately 10 m2 of nuclear track detectors placed around the interaction point. These suffer characteristic damage due to highly ionizing particles, such as magnetic monopoles or highly electrically charged particles. MoEDAL also has approximately 800 kg of aluminium bars placed around the interaction point, that can trap stable massive particles for later study. Passing these bars through a SQUID magnetometer yields a sensitive test for the presence of magnetic monopoles.

MoEDAL is an international research collaboration whose spokesperson is James Pinfold, from the University of Alberta. It is the seventh experiment at the LHC, was approved and sanctioned by the CERN research board in May 2010, and started its first test deployment in January 2011. [5]

In 2012 MoEDAL accuracy surpassed accuracy of similar experiments. A new detector was installed in 2015, [6] but as of 2017 it also did not find any magnetic monopoles, setting new limits on their production cross section. [7] In 2022 they performed a search for magnetic monopoles produced via the Schwinger effect. [8] The absence of a positive signal implies direct lower bounds on the mass of possible magnetic monopoles. [9]

Related Research Articles

<span class="mw-page-title-main">Compact Muon Solenoid</span> General-purposes experiment at the Large Hadron Collider

The Compact Muon Solenoid (CMS) experiment is one of two large general-purpose particle physics detectors built on the Large Hadron Collider (LHC) at CERN in Switzerland and France. The goal of the CMS experiment is to investigate a wide range of physics, including the search for the Higgs boson, extra dimensions, and particles that could make up dark matter.

<span class="mw-page-title-main">Large Hadron Collider</span> Particle accelerator at CERN, Switzerland

The Large Hadron Collider (LHC) is the world's largest and highest-energy particle collider. It was built by the European Organization for Nuclear Research (CERN) between 1998 and 2008 in collaboration with over 10,000 scientists and hundreds of universities and laboratories across more than 100 countries. It lies in a tunnel 27 kilometres (17 mi) in circumference and as deep as 175 metres (574 ft) beneath the France–Switzerland border near Geneva.

<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">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">ALICE experiment</span> Detector experiments at the Large Hadron Collider

ALICE is one of nine detector experiments at the Large Hadron Collider at CERN. The other eight are ATLAS, CMS, TOTEM, LHCb, LHCf, MoEDAL, FASER and SND@LHC.

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

The TOTEM experiment is one of the nine detector experiments at CERN's Large Hadron Collider. The other eight are: ATLAS, ALICE, CMS, LHCb, LHCf, MoEDAL, FASER and SND@LHC. It shares an interaction point with CMS. The detector aims at measurement of total cross section, elastic scattering, and diffraction processes. The primary instrument of the detector is referred to as a Roman pot. In December 2020, the D0 and TOTEM Collaborations made public the odderon discovery based on a purely data driven approach in a CERN and Fermilab approved preprint that was later published in Physical Review Letters. In this experimental observation, the TOTEM proton-proton data in the region of the diffractive minimum and maximum was extrapolated from 13, 8, 7 and 2.76 TeV to 1.96 TeV and compared this to D0 data at 1.96 TeV in the same t-range giving an odderon significance of 3.4 σ. When combined with TOTEM experimental data at 13 TeV at small scattering angles providing an odderon significance of 3.4 - 4.6 σ, the combination resulted in an odderon significance of at least 5.2 σ.

<span class="mw-page-title-main">DØ experiment</span> Particle physics research project (1983–2011)

The DØ experiment was a worldwide collaboration of scientists conducting research on the fundamental nature of matter. DØ was one of two major experiments located at the Tevatron Collider at Fermilab in Batavia, Illinois. The Tevatron was the world's highest-energy accelerator from 1983 until 2009, when its energy was surpassed by the Large Hadron Collider. The DØ experiment stopped taking data in 2011, when the Tevatron shut down, but data analysis is still ongoing. The DØ detector is preserved in Fermilab's DØ Assembly Building as part of a historical exhibit for public tours.

The High Luminosity Large Hadron Collider is an upgrade to the Large Hadron Collider, operated by the European Organization for Nuclear Research (CERN), located at the French-Swiss border near Geneva. From 2011 to 2020, the project was led by Lucio Rossi. In 2020, the lead role was taken up by Oliver Brüning.

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

The LHCf is a special-purpose Large Hadron Collider experiment for astroparticle physics, and one of nine detectors in the LHC accelerator at CERN. LHCf is designed to study the particles generated in the forward region of collisions, those almost directly in line with the colliding proton beams.

<span class="mw-page-title-main">NA61 experiment</span>

NA61/SHINE is a particle physics experiment at the Super Proton Synchrotron (SPS) at the European Organization for Nuclear Research (CERN). The experiment studies the hadronic final states produced in interactions of various beam particles with a variety of fixed nuclear targets at the SPS energies.

CASTOR is an electromagnetic (EM) and hadronic (HAD) calorimeter of the CMS experiment at CERN. It is based on plates made out of tungsten and quartz layers, positioned around the beam pipe in the very forward region of the CMS, covering the pseudorapidity range 5.1–6.55. It is used in collider physics, proton-proton collisions and heavy ion collisions, for example lead collisions. It is designed to search for strangelets and centauro events, kinds of exotic matter in the baryon dense, very forward phase region in lead (Pb) collisions at the particle accelerator LHC, CERN near Geneva.

<span class="mw-page-title-main">Search for the Higgs boson</span> Effort to prove or disprove the existence of particle

The search for the Higgs boson was a 40-year effort by physicists to prove the existence or non-existence of the Higgs boson, first theorised in the 1960s. The Higgs boson was the last unobserved fundamental particle in the Standard Model of particle physics, and its discovery was described as being the "ultimate verification" of the Standard Model. In March 2013, the Higgs boson was officially confirmed to exist.

<span class="mw-page-title-main">750 GeV diphoton excess</span> 2015 anomaly in the Large Hadron Collider

The 750 GeV diphoton excess in particle physics was an anomaly in data collected at the Large Hadron Collider (LHC) in 2015, which could have been an indication of a new particle or resonance. The anomaly was absent in data collected in 2016, suggesting that the diphoton excess was a statistical fluctuation. In the interval between the December 2015 and August 2016 results, the anomaly generated considerable interest in the scientific community, including about 500 theoretical studies. The hypothetical particle was denoted by the Greek letter Ϝ in the scientific literature, owing to the decay channel in which the anomaly occurred. The data, however, were always less than five standard deviations (sigma) different from that expected if there was no new particle, and, as such, the anomaly never reached the accepted level of statistical significance required to announce a discovery in particle physics. After the August 2016 results, interest in the anomaly sank as it was considered a statistical fluctuation. Indeed, a Bayesian analysis of the anomaly found that whilst data collected in 2015 constituted "substantial" evidence for the digamma on the Jeffreys scale, data collected in 2016 combined with that collected in 2015 was evidence against the digamma.

<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.

Stable massive particles (SMPs) are hypothetical particles that are long-lived and have appreciable mass. The precise definition varies depending on the different experimental or observational searches. SMPs may be defined as being at least as massive as electrons, and not decaying during its passage through a detector. They can be neutral or charged or carry a fractional charge, and interact with matter through gravitational force, strong force, weak force, electromagnetic force or any unknown force.

<span class="mw-page-title-main">Scattering and Neutrino Detector</span>

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). SND will be installed in an empty tunnel- TI18 that links the LHC and Super Proton Synchrotron, 480m away from the ATLAS experiment interaction point in the fast forward region and along the beam collision axis.

The MilliQan experiment is a small-scale detector experiment at CERN's Large Hadron Collider (LHC). MilliQan is not a separate CERN experiment but is handled as a CMS sub-detector, with a dedicated memorandum of understanding to define authorship and responsibilities. The goal of the MilliQan experiment is to detect millicharged particles: particles with charges much smaller than that of the electron. These particles are motivated by the existence of a dark photon, and discovery of millicharged particles would provide a first probe into the dark sector. The MilliQan prototype detector collected data during LHC Run 2 in 2018 and set competitive constraints on millicharged particle charges and masses. The upgraded Run 3 MilliQan detectors are scheduled to be installed in 2022.

David M. Strom is an experimental high energy particle physicist on the faculty of the University of Oregon.

James Lewis Pinfold is a British-Canadian physicist, specializing in particle physics.

References

  1. Patrizii, Laura; Zouleikha, Sahnoun; Togo, Vincent (2019). "Searches for cosmic magnetic monopoles: past, present and future". Phil. Trans. Roy. Soc. Lond. A. 337: 20180328. doi:10.1098/rsta.2018.0328.
  2. Milton, Kimball A. (2006). "Theoretical and experimental status of magnetic monopoles". Rept. Prog. Phys. 69: 1637–1712. arXiv: hep-ex/0602040 . doi:10.1088/0034-4885/69/6/R02.
  3. Giacomelli, G. (1984). "Magnetic monopoles". Rivista del Nuovo Cimento . 7 (12): 1–111. arXiv: hep-ex/0002032 . Bibcode:1984NCimR...7l...1G. doi:10.1007/BF02724347. S2CID   18553203.
  4. Acharya, B.; et al. (MoEDAL Collaboration) (2023). "Search for Highly-Ionizing Particles in pp Collisions During LHC Run-2 Using the Full MoEDAL Detector". arXiv. arXiv: 2311.06509 .
  5. Pinfold, J. (5 May 2010). "MoEDAL becomes the LHC's magnificent seventh". CERN Courrier . Retrieved 2016-07-14.
  6. Acharya, B.; et al. (MoEDAL Collaboration) (2016). "Search for magnetic monopoles with the MoEDAL prototype trapping detector in 8 TeV proton-proton collisions at the LHC". Journal of High Energy Physics. 2016 (8): 67. arXiv: 1604.06645 . Bibcode:2016JHEP...08..067A. doi:10.1007/JHEP08(2016)067. S2CID   5209935.
  7. Acharya, B.; et al. (MoEDAL Collaboration) (2017). "Search for Magnetic Monopoles with the MoEDAL Forward Trapping Detector in 13 TeV Proton-Proton Collisions at the LHC". Physical Review Letters. 118 (6): 061801. Bibcode:2017PhRvL.118f1801A. doi: 10.1103/PhysRevLett.118.061801 . hdl: 10138/178854 . PMID   28234515.
  8. "MoEDAL bags a first". CERN. Retrieved 2021-08-01.
  9. Acharya, B.; et al. (MoEDAL Collaboration) (2022). "Search for magnetic monopoles produced via the Schwinger mechanism". Nature. 602 (7895): 63–67. arXiv: 2106.11933 . doi:10.1038/s41586-021-04298-1.

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