
The component of a particle's momentum perpendicular to the beam axis in a collider.Transverse momentum is the component of a particle's momentum that is perpendicular to the beam axis in a collider experiment. In particle physics, when two beams of particles collide head-on, the total momentum along the beam direction is conserved and is essentially zero before the collision. Any particle produced in the collision that has momentum perpendicular to the beam must be balanced by other particles with opposite transverse momentum, so the vector sum of all transverse momenta in an event is zero. This makes transverse momentum a powerful tool for identifying particles that escape detection, such as neutrinos, which carry away momentum without leaving a trace in the detector.
The concept of transverse momentum became central with the development of colliding beam experiments in the 1960s and 1970s, particularly at CERN and Fermilab, where it was used to analyze the products of high-energy collisions.
In a collider, the beam axis defines the z-direction. For each detected particle, its momentum vector is decomposed into a longitudinal component (along the beam) and a transverse component (in the plane perpendicular to the beam). The transverse momentum is calculated from the particle's energy and its angle relative to the beam. Because the initial transverse momentum is zero, any imbalance in the detected transverse momenta indicates the presence of invisible particles. This is the basis for many searches for new physics, such as dark matter candidates, which would appear as missing transverse momentum.
Transverse momentum is used in every particle collider experiment to measure the properties of known particles, discover new ones, and search for physics beyond the Standard Model, such as supersymmetry or extra dimensions.
The transverse momentum of particles in a jet can be used to infer the mass of the original quark or gluon that produced the jet, a technique that helped discover the Higgs boson.




