Mu2e

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Mu2e project logo Mu2e-logo.jpg
Mu2e project logo
A prototype of the Mu2e Transport Solenoid module Mu2e-crew-600x400.jpg
A prototype of the Mu2e Transport Solenoid module

Mu2e, or the Muon-to-Electron Conversion Experiment, is a particle physics experiment at Fermilab in the US. [1] The goal of the experiment is to identify physics beyond the Standard Model, namely, the conversion of muons to electrons without the emission of neutrinos, which occurs in a number of theoretical models. [2] [3] Former project co-spokesperson Jim Miller likens this process to neutrino oscillation, but for charged leptons. [4] The rate for this process in the Standard Model of particle physics is unobservably small, so any observation of this process would constitute a major discovery and indicate new physics beyond the standard model. [2] The experiment will be 10,000 times more sensitive than previous muon to electron conversion experiments, and probe effective energy scales up to 10,000 TeV. [2]

Contents

Timeline

Prior work

Physicists have been searching for flavor violation since the 1940s. [2] Flavor violation among neutrinos was proven in 1998 at the Super-Kamiokande experiment in Japan. [5]

In 1989, Russian physicists Vladimir Lobashev and Rashid Djilkibaev proposed an experiment to search for lepton flavor violation. The experiment, called MELC, operated from 1992 to 1995 at the Moscow Meson Factory at the Institute for Nuclear Research in Russia, before being shut down due to the political and economic crises of the time. [6]

In 1997, American physicist William Molzon proposed a similar experiment at Brookhaven National Laboratory. Research and development on the MECO experiment began in 2001, but funding was pulled in 2005. [6]

Development

Mu2e is based on the MECO experiment proposed at Brookhaven, and the earlier MELC experiment at Russia's Institute for Nuclear Research. [7] Research and development for the Mu2e experiment began in 2009, with the conceptual design complete in mid-2011. [3] In July 2012, Mu2e received Critical Decision 1 approval (the second of five critical decision levels) from the Department of Energy, about one month after initial review. [8] Project Manager Ron Ray asserted, "I know of no other project that has received sign-off that quickly after review." [8] Funding of the Mu2e experiment was recommended by the Department of Energy's Particle Physics Project Prioritization Panel, in its 2014 report. [9]

Construction and operation

Groundbreaking on the detector hall took place on April 18, 2015. [10] Originally, commissioning was anticipated in 2019 and preliminary results were expected 2020; [1] however, the project was significantly delayed, and, in 2022, the experiment was projected to begin in 2026. [11] The delivery of two magnets from General Atomics was delayed, contributing to the shift in start-date. [12] The experiment is expected to run for three years. [7]

Later improvements to the detector may increase the sensitivity of the experiment by one to two orders of magnitude, allowing a more in-depth study of any charged lepton conversion that may be discovered in the initial run. [2]

As of February 2024, two Mu2E transport solenoids had been constructed and moved from Fermilab's Heavy Assembly Building to the detector hall, where final assembly will be completed.

Design

Stages of the Mu2e experiment Mu2e1-600x400.png
Stages of the Mu2e experiment

The Mu2e apparatus will be 92 feet (28 m) in length, and will consist of three sections. [10] The total cost of the experiment is $271 million. [13]

Muon production

Repurposed elements from the Tevatron collider will be used to generate and deliver an 8 GeV proton beam. The protons will be extracted from Fermilab's Delivery Ring through a non-linear third-integer resonance extraction process and sent in pulses to the tungsten target. These protons will then collide with the tungsten production target in the production solenoid, producing a cascade of particles including pions, which decay into muons. Mu2e will produce between 200 [7] and 500 quadrillion (2×1017 to 5×1017) muons per year. [6] For every 300 protons hitting the production target, about one muon will enter the transport solenoid. [7]

Transport

The 4.5-Tesla magnetic field of a production solenoid will direct some of the particles produced into an S-shaped 2-Tesla evacuated transport solenoid, consisting of 50 separate superconducting electromagnets, [14] which will select muons by charge and momentum, and carry the desired slow muons to the detector after some time delay. [3]

Detection

On entering the detector solenoid, the muons will hit (and stop within) an aluminum target that is about 0.2 mm thick, [6] [13] entering orbitals around nuclei within the target. [3] [10] Any muons which convert into electrons without emitting neutrinos will escape these orbitals and enter the detector with a characteristic energy of 104.97 MeV (which is the muon mass minus the binding energy of about 0.5 MeV and nuclear recoil energy of about 0.2 MeV). [6] [15]

The detector itself consists of two main components: a straw tracker to measure the momentum of outgoing particles; and an electromagnetic calorimeter to identify which particle interactions to record for further study, identify what type of particle passed through the tracker, and to confirm the measurements of the tracker. [15] An electron with energy of around 105 MeV will indicate that the electron originated in a neutrinoless muon conversion. [16]

In order to disturb the path of the electrons as little as possible, the tracker uses as little material as possible. The wire chamber tracker consists of panels of 15-micron-thick straws of metalized mylar filled with argon and carbon dioxide, the thinnest such straws ever used in a particle physics experiment. Electronics at each end of the straws will record the signal produced when electrons interact with the gas in the straw, allowing the trajectory of the electrons to be reconstructed. [16]

Sensitivity

The rate of neutrinoless conversion of muons to electrons was previously constrained by the MEG experiment to less than 2.4×10−12, and further constrained to 7×10−13 by the SINDRUM II experiment at the Paul Scherrer Institute in Switzerland. [5] Mu2e has an expected sensitivity of 5×10−17, four orders of magnitude beyond SINDRUM II, meaning that it will see a signal if as few as one in 100 quadrillion muons transforms into an electron. [5] [6]

Collaboration

As of October 2018, the Mu2e collaboration included 240 people from 40 institutions in six countries. [17] The collaboration is led by co-spokespersons Bob Bernstein (Fermilab) and Stefano Miscetti (INFN Frascati). The project manager for Mu2e is Julie Whitmore; the deputy project managers are Karen Byrum and Paul Derwent.

See also

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 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.

<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.

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<span class="mw-page-title-main">Fermilab</span> High-energy particle physics laboratory in Illinois, US

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<span class="mw-page-title-main">Collider Detector at Fermilab</span> American experimental physics device (1985–2011)

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COMET is a nuclear physics experiment in J-PARC, Tokai, Japan. In contrast to the usual muon decay to an electron and neutrino, COMET seeks to look for neutrinoless muon to electron conversion, where the electron flies away with an energy of 104.8 MeV. Muon to electron conversion is not forbidden in the Standard Model but the branching ratio is about considering neutrino oscillations. In beyond the Standard Model approaches the muon to electron conversion process can be as high as e.g. via the supersymmetric .

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]

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References

  1. 1 2 "Mu2e: muon-to-electron-conversion experiment". Fermilab. April 21, 2015. Retrieved 30 April 2015.
  2. 1 2 3 4 5 "Research Goals". Fermilab. March 17, 2015. Retrieved 1 May 2015.
  3. 1 2 3 4 Glenzinski, Doug (February 2011). "The Mu2e Experiment at Fermilab" (PDF). University of Pennsylvania. Retrieved 1 May 2015.
  4. ↑ Piergrossi, Joseph (January 10, 2013). "Midwest muon experiments carry on East Coast legacy". Symmetry Magazine. Retrieved 4 May 2015.
  5. 1 2 3 Dorigo, Tommaso (December 3, 2012). "Mu2E: Exploring Lepton Flavour Violation At Fermilab". Science 2.0. Retrieved 4 May 2015.
  6. 1 2 3 4 5 6 Mustain, Andrea (June 2010). "The muon guys: On the hunt for new physics". Symmetry Magazine. Retrieved 4 May 2015.
  7. 1 2 3 4 "How does it work?". Fermilab. March 17, 2015. Retrieved 30 April 2015.
  8. 1 2 Piergrossi, Joseph (July 20, 2012). "Department of Energy advances Fermilab's Mu2e experiment". Symmetry Magazine. Retrieved 4 May 2015.
  9. ↑ Jepsen, Kathryn (May 22, 2014). "Proposed plan for the future of US particle physics: The Particle Physics Project Prioritization Panel's report recommends a strategic path forward for US particle physics" . Retrieved 4 May 2015.
  10. 1 2 3 Kwon, Diana (April 21, 2015). "Mu2e breaks ground on experiment seeking new physics". Fermilab Today.
  11. ↑ Bernstein, Maxwell (March 24, 2022). "Straws, crystals and the quest for new subatomic physics". Fermilab News.
  12. ↑ "HEP Project Status, Mike Procario" (PDF). High Energy Physics Advisory Panel November 1–2, 2021 Agenda.
  13. 1 2 "Mu2e-doc-4299-v15: Mu2e Technical Design Report (TDR)". mu2e-docdb.fnal.gov. Retrieved 2017-01-18.
  14. ↑ Salles, Andre (December 16, 2013). "Mu2e attracts magnet experts". Symmetry Magazine. Retrieved 4 May 2015.
  15. 1 2 "Mu2e-doc-8084-v1: The Mu2e Experiment at Fermilab". mu2e-docdb.fnal.gov. Retrieved 2017-01-18.
  16. 1 2 "How to Detect a Rare Particle Decay with a Detector Made of (Almost) Nothing". Newswise. March 3, 2015. Retrieved 4 May 2015.
  17. ↑ "Collaboration". Fermilab. 26 October 2018. Retrieved 7 December 2018.
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