Muon collider: potential, challenges and pathways forward
21 Jan 2025
No
- Kai Gregory

 

 

Development of a successor to LHC's successor is underway, with the muon collider emerging as a promising candidate. This article explores STFC's efforts to address this future facilities technincal limitations.

Yes

​​​​​​​​

 

Physicists are exploring post-HL-LHC collider options, with muon colliders emerging as promising candidates due to their discovery potential and lower projected cost. This article details the efforts of STFC to support the required technologies for this technically challenging facility 

The concept of colliding oppositely charged muon beams dates to the 1960s, with physicists envisioning a facility beyond their technical reach, though capable of key discoveries. Today, this vision may become a reality, motivated by a discovery potential far exceeding the original expectations. Physics communities are dedicated to addressing the many technical challenges they pose, hoping to position a muon collider as a potential successor to the High Luminosity Large Hadron Collider. However, they face stiff competition from more thoroughly developed proposals at more advanced stages of planning. 

 

Promise and pitfalls of muon collision 

Two critical performance metrics for a particle collider are centre of mass energy, the total energy of the colliding particles at the point of collision and luminosity; the number of particles colliding in each collision. Any collider design seeks to maximise both, subject to other constraints. 

Muons can achieve a higher centre of mass energy than electrons, for a given energy input. Muons are fundamental particles, 207 times heavier than an electron. Muons make ideal candidates for circular accelerators, with their greater mass suppressing synchrotron radiation, which causes large energy losses in electron – positron accelerators. Mitigation of this drawback allows muon colliders to reach equivalent energy scales with more compact designs and lower power consumption. 

They can also reach a very high effective centre of mass, relative to protons. Protons are made up of quarks, each carrying a random quantity of energy. Each proton-proton collision is then effectively a lower-energy collision between two proton constituents (quarks and gluons). As fundamental particles, muons collide cleanly and at their full collision energy.  

Muon colliders can achieve equivalent center-of-mass energy with a more compact design; for instance, a 10 km muon collider is expected to match the center-of-mass energy of the proposed 91 km Future Circular Collider electron-positron (FCC-ee). Muon colliders are favoured over other facilities due to their higher power efficiency, consuming less power per unit of luminosity when increasing in energy. These two factors are especially crucial as research within all fields seeks to reduce their energy use and abide by sustainability frameworks.  

These advantages are yet to be exploited however, as creating and controlling, an intense muon beam is fraught with difficulty. A pivotal issue is the short muon lifetime. Muons are very short lived, existing for less than 1 millionth of a second before decaying. This fleeting existence can be extended according to the theory of special relativity. At velocities approaching the speed of light, muons experience time dilation which prolongs their apparent lifetime in an accelerator. 

Additionally, muons are inherently challenging to produce and manipulate due to their complex creation. Unlike electrons or protons, muons are produced in the decay of other particles, leading to a less well-defined beam. To summarise: muons must be produced, corralled into an accelerator, accelerated to near the speed of light and focused into a coherent beam, all within a fraction of a second.  

These properties pose significant technical challenges, with groups around the world dedicating R&D efforts to solving these. The Internation Muon Collider Collaboration (IMCC), along with the US Muon Collider Collaboration are currently spearheading these efforts and using their findings to assess the feasibility of a muon collider concept. 

While they have made progress, a definitive design remains incomplete. The long-term goal of the collaborations is to create a feasible design, guided by insights gained from demonstrator experiments for individual components.  ​

Motivation for muons 

Muon colliders possess vast discovery potential, with their impressive precision and higher centre of mass energy. Physicists can test the standard model with greater accuracy and even uncover new physics at higher energy scales. 

Since its discovery in 2012, the Higgs boson has been the subject of intense study at the LHC and will be probed at the HL-LHC at higher sensitivity. The reach of muon colliders extends far beyond these facilities, with its multi-TeV (Tera Electron Volt) energy scale probing deep into the unknown Higgs sector. Proposed facilities such as the electron-positron FCC-ee would produce more Higgs bosons, but with less sensitivity to processes such as rare Higgs decays [3]. Performing measurements on these events could allow us to answer further questions about the Higgs, such as whether it is made up of other particles, and its behaviour in the early universe [4].  

Their versatility extends beyond Higgs physics, as a muon collider would conduct a broad physics programme. It would be sensitive to hypothetical particles in a variety of different theoretical models, including supersymmetry and extra dimensions, and could potentially detect dark matter particles. Also, muon colliders offer a unique opportunity to investigate muon specific physics, through precise measurements of rare muon decays [4]  

 

Misbehaving muons: Muon collider challenges 

IMCC draft.png

Muon collider conceptual design: Developed by the now defunct research collaboration Muon Accelerator Program and adopted by IMCC, depicts 5 stages of required from muon production through to collision. This article will cover the mechanism and most pressing challenges associated with each stage excluding the proton driver. Image credit: IMCC 

An alternative design has also been drafted, proposing a positron driven muon beam. This article will not cover this, though for more detail consult the link 


Maximising the number of collisions per second (the “instantaneous luminosity”) is the key to observing rare or new physics processes and recording a large dataset, to achieve the full machine potential. Physicists can maximise luminosity by generating many muons and squeezing them together to enhance the chances of collision. Achieving this requires an intense proton source directed at a target, along with precise focusing and handling of the resulting muon beam.  

 

 Muon production  

Perhaps the most developed area of muon collider research is into proton targets. Past and ongoing studies aim to find a robust target which can withstand the high radiation, temperatures and pressures applied by the powerful proton beam, ensuring a consistently high yield of muons. These studies also explore the intense solenoidal fields needed to focus collision products. Like the targets, the magnets generating these fields must also tolerate this punishing environment.  

 

The MERcury Intensive Target (MERIT) experiment, conducted in 2007, demonstrated a feasible target to produce intense muon beams. Proton beams from CERN’s proton synchrotron were directed at a liquid Mercury target, selected for its high atomic number and resistance to melting, unlike solid alternatives [6]. Despite its success in yielding muons, the liquid mercury target is hazardous to handle and susceptible to damage. 

Researchers at the University of Warwick and Rutherford Appleton Laboratory (RAL) are seeking preferable alternatives. The collaboration has designed and tested an innovative system which circulates a medium containing Tungsten Powder. Circulation of this dense material reduces damage, increasing durability of the target. Having conducted an initial beam experiment, they hope to optimise the system in preparation for beams of even higher power [7].  

Powder Rig Photo (2).jpg


Tungsten powder handling rig at RAL  

















Muon cooling 

After the proton beam strikes its target, the resulting muons must be concentrated into a beam and be accelerated for collision. This requires the initially diffuse cloud of muons to be focused into a narrow, pencil-shaped beam. This process of emittance reduction, also known as cooling, is constrained by the muon's short lifetime. Ionisation cooling can provide a rapid and effective solution.  

After the production and isolation of muons, the high intensity beam is focused onto a component called an absorber via superconducting solenoids. Prior to their entry, muons occupy a large space due to an average high momentum, perpendicular (transverse) and parallel (longitudinal) to the direction of travel.  

The absorber ‘absorbs’ this momentum, with the muons interacting with liquid within the absorber. By liberating electrons from their nuclei, the muons lose kinetic energy. Collision with nuclei has the opposite effect: this is minimised through the selection of less dense materials such as liquid hydrogen or lithium hydride. 

After passing through the absorber, momentum in both planes are reduced, shrinking the space they occupy. Whilst this focuses the beam, it lowers the longitudinal momentum and muons short lifetime necessitates rapid acceleration. Restoration of its longitudinal momentum occurs through the alternating electric fields of a Radiofrequency (RF) cavity. This cooling effect accumulates as the process is repeated, with the initially chaotic muon cloud reduced to dense bunches. Eventually, by passing through multiple absorbers and RF cavities, this tight bunch of muons can be efficiently accelerated. ​


Step IV_SS-FC-SS-PRY_PlanView_Normal (1).JPG

Rendering of single cooling cell and its surrounding steel shielding: Entering the cell, they travel through the tracker (cyan), tracing momentum and measuring momentum. Superconducting solenoids focus (presence indicated by orange and red) muons onto absorber (light blue component in the center). 

The Muon Ionisation Cooling Experiment (MICE) is an international research collaboration, using a muon beam at the RAL ISIS Neutron and Muon Source, that intended to demonstrate this effect. A muon beam was directed to an absorber without acceleration, measuring important parameters such as emittance and muon density. MICE was successful, serving as the first demonstration of ionisation cooling. The collaboration observed a reduction in transverse momentum and increase in muon density [8]  

2015-05-27 16.40.37 (1).jpg


MICE apparatus at the STFC ISIS Neutron and Muon Source. This is where the experiments demonstrating ionisation cooling took place from 2017 to 2019. Metal panels shield computing infrastructure from strong solenoidal fields. Image credit: STFC ISIS 








The IMCC aims to build on the achievements of the MICE collaboration by developing a future demonstrator experiment that more closely replicates the conditions required for a muon collider. This next step would involve demonstrating the reduction of both longitudinal and transverse momentum across multiple absorbers. Additionally, it would need to operate with a higher-intensity muon beam and accommodate a wider range of emittance values [9]. A successor to the MICE experiment, capable of cooling in both planes with multiple absorbers, first requires advancements to magnet engineering, RF cavities and cooling technology 


Muon acceleration  

Muons emerge from the cooling apparatus primed for acceleration, tightly bunched and strongly focused. IMCC envisages a low energy muon acceleration via a series of linear accelerators followed by injection of the beam into a synchrotron.  

Once injected, they will undergo further acceleration to relativistic velocity before collision. Conventional pulsed synchrotrons are a potential option for high energy acceleration though more efficient and cost-effective alternatives exist [9].  

Rapid Cycling synchrotrons and Fixed Field Alternating Gradients (FFAs) are both promising alternatives. FFAs are particularly appealing as they can rapidly accelerate particles from a broad range of initial energies. This feature makes them well suited to applications like muon colliders. The Electron Model for Many Applications experiment (EMMA) demonstrated the feasibility of a subset of FFAs at low energy. Commissioned in 2010 at STFC’s Daresbury laboratory, EMMA accelerated electron beams on a timescale compatible with muon lifetime. Significant adaptation is needed to scale this technology for use within high energy muon beams [10].  


The-EMMA-proof-of-principle-accelerator-at-the-Daresbury-Laboratory (1).png




Image credit: EMMA experiment at Daresbury Laboratory. World’s first non-scaling FFA accelerator   The EUROnu Project (2013) DOI: Link. Figure 13









Muon decay: Detection issues and damage to components  

Entering the collider ring, the two opposing muon beams are set to collide at the TeV energy scale. Despite experiencing time dilation, muon survival wanes, with estimates of 10% loss by this stage. Many muons decay to produce electrons, positrons and neutrinos. These electrons and positrons will deposit their energy into the surrounding collider components, leading to radiation damage. IMCC is exploring technology that would tolerate / protect against the energy deposited [11] 

Research on mitigating muon decay products is also relevant to particle detectors. These complex systems must be able to isolate the collision products from the signatures produced from muon decay known as Beam Induced Background (BIB). Detectors must be able to sift through vast swathes of BIB without compromising the desired events [11] 

Preliminary designs for the detector have been produced and used to create simulations accurate for muon collision at 1.5 TeV. These simulations shed light onto challenges that BIB poses to muon colliders and offer feasible solutions to BIB mitigation. IMCC will first ensure these encouraging results are replicated at higher energies, up to 10 TeV, before finalising detector design.  


Balancing Ambition with Reality: The future of Muon colliders 

Several different colliders have been proposed for the future, with a variety of different technology choices and at many different locations. At the time of writing none of these has been approved for construction, and there will be an interesting few years ahead as the decision process across laboratories, review panels and national funding agencies continues.  

Muon colliders are an appealing candidate, boasting an impressive precision and high Center of Mass energy The creation of a bright muon beam has applications for neutrino physics and muon spectroscopy, development towards muon colliders will stand to benefit these synergistic fields. A muon collider would have lower space and power requirements than an electron or proton collider of comparable physics reach, but, as discussed here, requires the development of several novel technologies. Conversely, competing facilities are at more advanced stages of planning, while muon colliders are yet to settle on a single design or select a construction site [12]  

The IMCC is working to overcome the many technical barriers to present a convincing case for the next European Strategy for Particle Physics Update in 2026 [12]. If successful, the IMCC proposal outlines continuation of their comprehensive R&D program, followed by integration of these technologies in large scale demonstrator experiments, ready for possible construction to begin in 2045 [12].  

 

 

References 

[1] Long, K.R., Lucchesi, D., Palmer, M.A. et al. Muon colliders to expand frontiers of particle physics. Nat. Phys. 17, 289–292 (2021). https://doi.org/10.1038/s41567-020-01130-x 

[2] IMCC collaboration - Towards a Muon Collider (2023) Link 

[3] Roman Pöschl Future colliders – Linear and circular colliders (2018) Proceedings of ALPS2018    

[4] Murayama, Hitoshi, Asai, Shoji, Heeger. et al Exploring the Quantum Universe: Pathways to Innovation and Discovery in Particle Physics. (2023) doi:10.2172/2368847. Sections 5.1.4 - 5.1.5 then Section 4.1 

[5] Kyberg et al nuSTORM Neutrinos from STORed Muons. Letter of Intent to the Fermilab Physics Advisory Committee (2012) Link 

[6] I, Efthymiopoulos, MERIT collaboration, MERIT - The high intensity liquid mercury target experiment at the CERN PS 2008 IEEE Nuclear Science Symposium, Medical Imaging Conference and 16th Room Temperature Semiconductor Detector Workshop pp 3302 – 3305      DOI: 10.1109/NSSMIC.2008.4775051 

[7] Chris Densham Potential of a Circulating Fluidised Bed (CFB) as a Muon Collider target Indico Link  

[8] MICE collaboration Demonstration of cooling by the Muon Ionization Cooling Experiment (2020) Nature, 578, 53 – 59    

[9] Daniel Schulte, Muon collider DOI: Indico. Youtube Link 

[10] J. Scott Berg FFAs for Acceleration in a Muon Collider (2024) Indico Presentation: Link 

[11] Dr Karol Krizka Building the case for a muon collider (2024) Link 

[12] Accettura. et al. (Vol 2) Interim report for International Muon Collaboration (2024) https://doi.org/10.23731/CYRM-2024-002 

​General References 

  • Daniel Schulte Muon Collider (2024) Link  

Great presentation: Establishes potential IMCC strategy and objectives. 

  • ​Muon collider Snowmass White Papers (2022) - Link  

Used for 3 TeV feasibility study and promising technologies. 

  • ​​IMCC website (CERN) - Link  

Basic overview. Navigate Structure / Resources for more detailed studies 

  • ​​​F Collamati, C Curatolo, D Lucchesi, A Mereghetti, N Mokhov, M Palmer, P Sala Advanced assessment of Beam Induced Background at a Muon Collider (2021)  Link     

Interesting paper about BIB strategies in detectors in 1.5 TeV simulations. 

 ​

 

 ​











Contact: Gregory, Kai (STFC,RAL,PPD)