For example, light particles are also bosons and are called photons, a combination of the words boson and photo (meaning light). In 1962, physicist Philip Anderson, an expert in condensed matter physics, observed that the breakdown of symmetry played a role in superconductivity and suggested that it could also be part of the answer to the problem of caliber invariance in particle physics. Particles, such as protons, made up of quarks obtain most of their mass from the bonding energy that holds their components together. Therefore, whatever gave mass to these particles did not have to break the invariance of the indicator as a basis for other parts of the theories where it worked well, and it didn't have to require or predict unexpected particles without mass or far-reaching forces that didn't really seem to exist in nature.
CERN estimates that, after the update each year, the accelerator will create 15 million of these particles. However, for this unification to work mathematically, force-carrying particles are required to have no mass. The relevant particle theory (in this case, the Standard Model) will determine the necessary types of collisions and detectors. This is because the spontaneous rupture of symmetry does not occur with photons as with their companion particles that carry force, the W and Z bosons.
In the extreme energies of these collisions, the desired esoteric particles are produced from time to time, which can be detected and studied; any absence or difference with respect to theoretical expectations can also be used to improve the theory. First, the publisher did not allow us to call it the Damned Particle, although that might be a more appropriate title, given its evil nature and the expenses it is causing. A boson is a force-carrying particle that comes into play when particles interact with each other, and a boson is exchanged during this interaction. The particle was detected both by the LHC ATLAS detector and by the Compact Muon Solenoid (CMS) detector.
The standard model includes a field of the type needed to break the electroweak symmetry and give the particles their correct mass. In the late 1950s and early 1960s, physicists still didn't know how to solve these problems or how to create an integral theory for particle physics. If caliber invariance was to be maintained, then these particles had to acquire their mass through some other mechanism or interaction. This involves accelerating large numbers of particles to extremely high energies and very close to the speed of light, and then allowing them to collide with each other.