Related Experiment Video
Updated: Sep 27, 2025

07:46
Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
8.7K
The muon Smasher's guide
Hind Al Ali1, Nima Arkani-Hamed2, Ian Banta1
1Department of Physics, University of California, Santa Barbara, CA 93106, United States of America.
Summary
A future high-energy muon collider offers unique advantages for discovering new physics. This research details its physics case, highlighting its potential for exploring electroweak symmetry breaking, dark matter, and beyond.
Area of Science:
- Particle Physics
- High-Energy Physics
- Collider Physics
Background:
- Current particle colliders face limitations in energy and precision.
- The search for new physics beyond the Standard Model requires advanced experimental capabilities.
Purpose of the Study:
- To present a comprehensive physics case for a future high-energy muon collider.
- To explore collision energies from 1 to 100 TeV and various luminosities.
- To highlight the advantages of a muon collider over alternative proposals.
Main Methods:
- Leveraging the point-like nature of muons.
- Utilizing the electroweak radiation cloud surrounding the muon beam.
- Analyzing electroweak symmetry breaking, dark matter, and weak scale naturalness.
- Connecting with complementary experiments (electric dipole moments, flavor violation, gravitational waves).
Main Results:
- Muon colliders can blur the energy-precision dichotomy in new physics searches.
- Demonstrated applications to fundamental physics questions.
- Provided cross-section predictions for simplified models across center-of-mass energies.
Conclusions:
- A high-energy muon collider is a compelling next step for particle physics research.
- It offers a unique and powerful platform for exploring fundamental questions.
- Synergies with other experimental approaches will enhance discovery potential.
More Related Videos
Related Concept Videos
Nuclear Transmutation
19.0K
Nuclear transmutation is the conversion of one nuclide into another. It can occur by the radioactive decay of a nucleus, or the reaction of a nucleus with another particle. The first manmade nucleus was produced in Ernest Rutherford’s laboratory in 1919 by a transmutation reaction, the bombardment of one type of nuclei with other nuclei or with neutrons. Rutherford bombarded nitrogen-14 atoms with high-speed α particles from a natural radioactive isotope of radium and observed...
19.0K
Collisions in Multiple Dimensions: Introduction
5.7K
It is far more common for collisions to occur in two dimensions; that is, the initial velocity vectors are neither parallel nor antiparallel to each other. Let's see what complications arise from this. The first idea is that momentum is a vector. Like all vectors, it can be expressed as a sum of perpendicular components (usually, though not always, an x-component and a y-component, and a z-component if necessary). Thus, when the statement of conservation of momentum is written for a...
5.7K
Subatomic Particles
103.2K
Dalton was only partially correct about the particles that make up matter. All matter is composed of atoms, and atoms are composed of three smaller subatomic particles: protons, neutrons, and electrons. These three particles account for the mass and the charge of an atom.
103.2K
Nuclear Fusion
32.0K
The process of converting very light nuclei into heavier nuclei is also accompanied by the conversion of mass into large amounts of energy, a process called fusion. The principal source of energy in the sun is a net fusion reaction in which four hydrogen nuclei fuse and ultimately produce one helium nucleus and two positrons.
A helium nucleus has a mass that is 0.7% less than that of four hydrogen nuclei; this lost mass is converted into energy during the fusion. This reaction produces about...
A helium nucleus has a mass that is 0.7% less than that of four hydrogen nuclei; this lost mass is converted into energy during the fusion. This reaction produces about...
32.0K
Thomson's e/m Experiment
4.9K
In a beam of charged particles created by a heated cathode, the particles move at different speeds. However, many applications need a beam with uniform particle speeds. An arrangement known as a velocity selector uses electric and magnetic fields to pick particles with a particular speed from the beam.
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The...
A particle with charge q, speed v, and mass m enters an area from the top, where the magnetic and electric fields are perpendicular both to the particle's motion and to one another. The...
4.9K

