Muon
In the
Standard Model of
particle physics, a
muon is a semistable
fundamental particle with negative
electric charge and a
spin of 1/2. Together with the
electron, the
tauon and the
neutrinos, it is classified as part of the the
lepton family of
fermions. Like all fundamental particles, the muon has an
antimatter partner of opposite charge but equal
mass and spin: the
antimuon.
For historical reasons, muons are sometimes referred to as
mu mesons, even though they are not classified as
mesons by modern particle physicists (
see History). Muons have a mass that is 207 times greater than the electron (105.6
MeV). Because of this, a muon can be thought of as an extremely heavy electron. Muons are denoted by μ
- and antimuons by μ
+.
On earth, muons are created when a charged
pion decays. The pions are created in an upper atmosphere by
cosmic radiation and have a very short decay time--a few nanoseconds. The muons created when the pion decays are also short-lived: their decay time is 2.2 microseconds. However, muons in the atmosphere are moving at very high velocities, so that the
time dilation effect of
special relativity make them easily detectable at the earth's surface.
As with the case of the other charged leptons, there is a
muon-neutrino which is associated with the muon. Muon-neutrinos are denoted by ν
μ. Muons naturally decay into an electron, an electron neutrino, and a muon-antineutrino.
Muon atoms
\nThe muon was the first elementary particle discovered that does not appear in ordinary atoms. Muons can, however, form muon atoms by replacing the electrons in ordinary atoms. Muon atoms are much smaller than typical atoms because in order to conserve angular momentum, the more massive muon must be closer to the atomic nucleus than their less massive electron counterparts.
History
\nMuons were discovered by Carl D. Anderson in 1936 while he studied cosmic radiation. He had noticed particles that curved in a manner distinct from that of electrons and other known particles when passed through a magnetic field. In particular, these new particles curved to a smaller degree than electrons, but more sharply than protons. It was assumed that their electric charge was equal to that of the electron, and so to account for the difference in curvature, it was supposed that these particles were of intermediate mass (lying somewhere between that of an electron and that of a proton).
For this reason, Anderson initially called the new particle a mesotron, adopting the prefix meso- from the Greek word for "intermediate". Shortly thereafter, additional particles of intermediate mass were discovered, and the more general term meson was adopted to refer to any such particle. Faced with the need to differentiate between different types of mesons, the mesotron was renamed the mu meson (with the Greek letter mu used to approximate the sound of the English letter m).
However it was soon found that the mu meson significantly differed from other mesons (e.g. its breakdown products included a neutrino and an antineutrino, rather than one or the other as was observed in other mesons). Thus mu mesons were not mesons at all, and so the term mu meson was abandoned and replaced with the modern term muon.
Related topics
\n*Muonium\n*Muon-catalyzed fusion\n*List of particles
References
\n*Serway & Faughn, College Physics, Fourth Edition (Fort Worth TX: Saunders, 1995) page 841
Category:Leptons\n
