
One of the three types (flavors) of neutrinos, associated with the muon in weak interactions.The muon neutrino is one of the three flavors of neutrinos, elementary particles that interact only via the weak nuclear force and gravity. It is produced in processes involving muons, such as the decay of pions in cosmic-ray showers, or in particle accelerators. Muon neutrinos are famously elusive: billions pass through your body every second without leaving a trace. Their study has revealed that neutrinos can oscillate — change flavor — which implies they have tiny masses, a discovery that earned the 2015 Nobel Prize in Physics.
The muon neutrino was first detected in 1962 by Leon Lederman, Melvin Schwartz, and Jack Steinberger at Brookhaven National Laboratory, using a beam of neutrinos produced by pion decay. They showed that these neutrinos produced muons, not electrons, confirming the existence of a distinct flavor.
Muon neutrinos are created when a muon decays or when a pion decays into a muon and a neutrino. They are detected indirectly: when a muon neutrino interacts with a nucleus, it typically produces a muon, which leaves a long, straight track in a detector like Super-Kamiokande or IceCube. By counting the number of muon neutrinos arriving from a given source (e.g., the Sun or the atmosphere) and comparing it to the expected number, physicists can measure oscillation probabilities. The flavor change occurs because the three neutrino mass states are superpositions of flavor states, and they acquire different phases as they travel.
Muon neutrinos are used in long-baseline experiments (like NOvA and T2K) to study neutrino oscillations and CP violation, which may explain the matter-antimatter asymmetry of the universe. They also serve as a probe of the Earth's interior via neutrino tomography.
The muon neutrino was the first particle discovered using a particle accelerator, and its discovery required a 10-ton spark chamber detector placed in a neutrino beam at Brookhaven.











