PROFILPELAJAR.COM

The International Muon Ionization Cooling Experiment (or MICE) is a high-energy physics experiment at the Rutherford Appleton Laboratory. The experiment is a recognized CERN experiment (RE11).^[1]^[2] MICE is designed to demonstrate ionization cooling of muons.^[3] This is a process whereby the emittance of a beam is reduced in order to reduce the beam size, so that more muons can be accelerated in smaller-aperture accelerators and with fewer focussing magnets. This might enable the construction of high-intensity muon accelerators, which can be used in, for example, a neutrino factory or muon collider.

MICE will reduce the transverse emittance of a muon beam over a single 7-meter cooling cell and measure that reduction. The original MICE design was based on a scheme outlined in Feasibility Study II.^[4] It was revised significantly in 2014.^[3] Pions will be produced from a target in the ISIS neutron source and transported along a beamline where most will decay to muons before entering MICE. Cooling is tested with lithium hydride (LiH) crystals or liquid hydrogen (LH₂) cells; magnets are used to focus and analyze the muon beam. MICE will measure cooling performance over a range of beam momenta between about 150 and 250 MeV/c.

Beamline

The MICE muon beamline provides a low-intensity muon beam for MICE. Pions will be transported from a target dipping into the fringe of the ISIS proton beam, through a pion decay channel, into a muon transport line, and then into MICE. For efficient use of muons, it is desirable to have a reasonably good match between the transport beamline and the cooling channel, with selection performed in analysis. Also, the beamline must suppress non-muon events from entering the cooling channel. A beam rate of a few hundred muons per second is expected.

Experiment setup

MICE combines systems to identify, track, steer, and cool muons.^[3]

To reject background from pions and electrons, Cerenkov detectors and time-of-flight detectors are the outermost components of the experiment. A calorimeter at the end distinguishes electrons from muons.^[5]

The muon emittance is measured with scintillating-fibre tracking detectors in a 4-Tesla magnetic field both before and after the main cooling cell. A diffuser can be placed in front of the first tracking detector to study the cooling of muon beams with larger emittance.

The main cooling cell consists of a secondary LiH absorber, a radio frequency cavity (RF cavity), coils to focus the beam onto the central main absorber (LiH or LH₂), magnet coils to focus the beam leaving the main absorber, a second RF cavity, and another secondary LiH absorber.

While the secondary absorbers contribute to cooling, their main purpose is to stop electrons released in the RF cavities. The RF cavities are designed to accelerate the muons. As they cannot be synchronized with the incoming muons, some muons will be accelerated while others will be decelerated. The time of flight measurements allow a calculation of the electric field that the muons experienced in the cavities.

The baseline main absorber is a LiH disk 65 mm (2.6 in) thick. Alternatively, a 350-millimetre-long (14 in) liquid hydrogen vessel can be used.

Detectors

Muons pass through the cooling channel one-by-one. The muons' phase space coordinates will be measured by time-of-flight scintillators and scintillating fibre tracking detectors upstream and downstream of the cooling channel. Muons will be distinguished from other particles in the beam using a combination of the spectrometers and the so-called Particle Identification (PID) detectors, three time-of-flight scintillators, a Cerenkov detector, and a calorimeter.

Status

As of 2017, MICE is taking data, and upgrades to a longer cooling cell are considered.^[6]

References

^ "Recognized Experiments at CERN". The CERN Scientific Committees. CERN. Archived from the original on 13 June 2019. Retrieved 20 January 2020.
^ "RE11/MICE : Muon Ionization Cooling Experiment". The CERN Experimental Programme. CERN. Retrieved 20 January 2020.
^ ^a ^b ^c Bogomilov, M.; et al. (MICE collaboration) (2017). "Design and expected performance of the MICE demonstration of ionization cooling". Physical Review Special Topics: Accelerators and Beams. 20 (6): 063501. arXiv:1701.06403. Bibcode:2017PhRvS..20f3501B. doi:10.1103/PhysRevAccelBeams.20.063501. S2CID 54956640.
^ The BNL Advanced Accelerator Group (ed.) S. Ozaki, R. Palmer, M. Zisman, and J. Gallardo, Feasibility Study-II of a Muon-Based Neutrino Source, BNL-52623, (2001) [RETRIEVED: 2007-11-16]
^ Adams, D.; et al. (2015). "Electron-Muon Ranger: Performance in the MICE Muon Beam". Journal of Instrumentation. 10 (12): P12012. arXiv:1510.08306. Bibcode:2015JInst..10P2012A. doi:10.1088/1748-0221/10/12/P12012. S2CID 26941784.
^ Presentation by Kenneth Richard Long at the 47th Muon Ionization Cooling Experiment (MICE) Collaboration Meeting (pdf)