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| {{Infobox Particle
| | Hello from Denmark. I'm glad to came across you. My first name is Elane. <br>I live in a city called Kobenhavn V in nothern Denmark.<br>I was also born in Kobenhavn V 22 years ago. Married in May 2005. I'm working at the backery.<br><br>Feel free to visit my blog post; [http://tinyurl.com/l4wydqp nike free run] |
| | bgcolour =
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| | name = Muon
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| | image = [[Image:Moon's shadow in muons.gif|248px]]
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| | caption = The Moon's cosmic ray shadow, as seen in secondary muons generated by cosmic rays in the atmosphere, and detected 700 meters below ground, at the [[Soudan II]] detector
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| | num_types =
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| | composition = [[Elementary particle]]
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| | statistics = [[Fermionic]]
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| | group = [[Lepton]]
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| | generation = Second
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| | interaction = [[Gravity]], [[Electromagnetic interaction|Electromagnetic]], <br>[[Weak interaction|Weak]]
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| | antiparticle = Antimuon ({{SubatomicParticle|Antimuon}})
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| | theorized =
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| | discovered = [[Carl D. Anderson]] (1936)
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| | symbol = {{SubatomicParticle|muon-}}
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| | mass = {{val|105.6583715|(35)|ul=MeV/c2}}<ref name="PDG2012">
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| {{cite web
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| |author=J. Beringer ''et al.'' ([[Particle Data Group]])
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| |url=http://pdg.lbl.gov/2012/tables/rpp2012-sum-leptons.pdf
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| |title=PDGLive Particle Summary 'Leptons (e, mu, tau, ... neutrinos ...)'
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| |publisher=[[Particle Data Group]]
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| |year=2012
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| |accessdate=2013-01-12
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| }}</ref>
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| | mean_lifetime = {{val|2.1969811|(22)|e=-6|ul=s}}<ref name="PDG2012" />
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| | decay_particle =
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| | electric_charge = −1 [[Elementary charge|e]]
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| | color_charge = None
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| | spin = {{frac|1|2}}
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| | num_spin_states =
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| }}
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| The '''muon''' ({{IPAc-en|ˈ|m|juː|ɒ|n}}; from the [[Greek alphabet|Greek]] letter [[mu (letter)|mu]] (μ) used to represent it) is an [[elementary particle]] similar to the [[electron]], with unitary negative [[electric charge]] of roughly −1 and a [[spin-½|spin of {{frac|1|2}}]], but with much more mass ({{val|105.7|ul=MeV/c2}}). Together with the [[electron]] (mass {{val|0.511|ul=MeV/c2}}), the [[tau (particle)|tau]] (mass {{val|1777.8|ul=MeV/c2}}), ), and the three [[neutrino]]s, it is classified as a [[lepton]]. As is the case with other leptons, the muon is not believed to have any sub-structure at all (i.e., is not thought to be composed of any simpler particles), except possibly at the string scale.
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| The muon is an unstable [[subatomic particle]] with a [[mean lifetime]] of {{val|2.2|ul=µs}}. This comparatively long decay lifetime (the second longest known) is due to being mediated by the [[weak interaction]]. The only longer lifetime for an unstable subatomic particle is that for the free [[neutron]], a baryon particle composed of quarks, which also decays via the weak force. Muon decay produces at least three particles, and these must include an [[electron]] of the same charge as the muon, plus two [[neutrino]]s of different types.
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| Like all elementary particles, the muon has a corresponding [[antiparticle]] of opposite charge (+1) but equal [[mass]] and spin: the '''antimuon''' (also called a ''positive muon''). Muons are denoted by {{SubatomicParticle|Muon-}} and antimuons by {{SubatomicParticle|Muon+}}. Muons were previously called '''mu mesons''', but are not classified as [[meson]]s by modern particle physicists (see ''[[#History|History]]'').
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| Muons have a [[mass]] of {{val|105.7|ul=MeV/c2}}, which is about 200 times the mass of an electron. Since the muon's interactions are very similar to those of the electron, a muon can be thought of as a much heavier version of the electron. Due to their greater mass, muons are not as sharply accelerated when they encounter electromagnetic fields, and do not emit as much [[bremsstrahlung]] (deceleration radiation). This allows muons of a given energy to penetrate far more deeply into matter than electrons, since the deceleration of electrons and muons is primarily due to energy loss by the bremsstrahlung mechanism. As an example, so-called "secondary muons", generated by [[cosmic rays]] hitting the atmosphere, can penetrate to the Earth's surface, and even into deep mines.
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| Because muons have a very large mass and energy compared with the [[decay energy]] of radioactivity, they are never produced by [[radioactive decay]]. They are, however, produced in copious amounts in high-energy interactions in normal matter, during certain [[particle accelerator]] experiments with [[hadron]]s, or naturally in [[cosmic ray]] interactions with matter. These interactions usually produce [[pi meson]]s initially, which most often decay to muons.
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| As with the case of the other charged leptons, the muon has an associated [[muon neutrino]], which is not the same particle as the [[electron neutrino]], and does not participate in the same nuclear reactions. Muon neutrinos are denoted by {{SubatomicParticle|Muon neutrino}}.
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| ==History==
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| Muons were discovered by [[Carl D. Anderson]] and [[Seth Neddermeyer]] at Caltech in 1936, while studying [[cosmic radiation]]. Anderson had noticed particles that curved differently from electrons and other known particles when passed through a [[magnetic field]]. They were negatively charged but curved less sharply than electrons, but more sharply than [[proton]]s, for particles of the same velocity. It was assumed that the magnitude of their negative electric charge was equal to that of the electron, and so to account for the difference in curvature, it was supposed that their mass was greater than an electron but smaller than a proton. Thus Anderson initially called the new particle a ''mesotron'', adopting the prefix ''meso-'' from the Greek word for "mid-". The existence of the muon was confirmed in 1937 by J. C. Street and E. C. Stevenson's cloud chamber experiment.<ref>New Evidence for the Existence of a Particle Intermediate Between the Proton and Electron", Phys. Rev. 52, 1003 (1937).</ref>
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| A particle with a mass in the meson range had been predicted before the discovery of any mesons, by theorist [[Hideki Yukawa]]:<ref>Yukaya Hideka, On the Interaction of Elementary Particles 1, Proceedings of the Physico-Mathematical Society of Japan (3) 17, 48, pp 139–148 (1935). (Read 17 November 1934)</ref>
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| <blockquote>
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| "It seems natural to modify the theory of Heisenberg and Fermi in the following way. The transition of a heavy particle from neutron state to proton state is not always accompanied by the emission of light particles. The transition is sometimes taken up by another heavy particle."
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| </blockquote>
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| Because of its mass, the mu meson was initially thought to be Yukawa's particle, but it later proved to have the wrong properties. Yukawa's predicted particle, the pi meson, was finally identified in 1947 (again from cosmic ray interactions), and shown to differ from the earlier-discovered mu meson by having the correct properties to be a particle which mediated the [[nuclear force]].
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| With two particles now known with the intermediate mass, the more general term ''[[meson]]'' was adopted to refer to any such particle within the correct mass range between electrons and nucleons. Further, in order to differentiate between the two different types of mesons after the second meson was discovered, the initial mesotron particle was renamed the ''mu meson'' (the Greek letter ''μ'' (''mu'') corresponds to ''m''), and the new 1947 meson (Yukawa's particle) was named the [[pi meson]].
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| As more types of mesons were discovered in accelerator experiments later, it was eventually found that the mu meson significantly differed not only from the pi meson (of about the same mass), but also from all other types of mesons. The difference, in part, was that mu mesons did not interact with the [[nuclear force]], as pi mesons did (and were required to do, in Yukawa's theory). Newer mesons also showed evidence of behaving like the pi meson in nuclear interactions, but not like the mu meson. Also, the mu meson's decay products included both a [[neutrino]] and an [[antineutrino]], rather than just one or the other, as was observed in the decay of other charged mesons.
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| In the eventual [[Standard Model]] of particle physics codified in the 1970s, all mesons other than the mu meson were finally understood to be [[hadrons]]—that is, particles made of [[quarks]]—and thus subject to the [[nuclear force]]. In the quark model, a ''meson'' was no longer defined by mass (for some had been discovered that were very massive—more than [[nucleon]]s), but instead were particles composed of exactly two quarks (a quark and antiquark), unlike the [[baryon]]s, which are defined as particles composed of three quarks (protons and neutrons were the lightest baryons). Mu mesons, however, had shown themselves to be fundamental particles (leptons) like electrons, with no quark structure. Thus, mu mesons were not [[meson]]s at all, in the new sense and use of the term ''meson'' used with the quark model of particle structure.
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| With this change in definition, the term ''mu meson'' was abandoned, and replaced whenever possible with the modern term ''muon'', making the term mu meson only historical. In the new quark model, other types of mesons sometimes continued to be referred to in shorter terminology (e.g., ''pion'' for pi meson), but in the case of the muon, it retained the shorter name and was never again properly referred to by older "mu meson" terminology.
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| The eventual recognition of the "mu meson" muon as a simple "heavy electron" with no role at all in the nuclear interaction, seemed so incongruous and surprising at the time, that Nobel laureate [[I. I. Rabi]] famously quipped, "Who ordered that?"
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| In the [[Time dilation of moving particles|Rossi–Hall experiment]] (1941), muons were used to observe the [[time dilation]] (or alternately, [[length contraction]]) predicted by [[special relativity]], for the first time.
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| ==Muon sources==
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| Since the production of muons requires an available [[center of momentum frame]] energy of 105.7 MeV, neither ordinary [[radioactive decay]] events nor nuclear fission and fusion events (such as those occurring in [[nuclear reactors]] and [[nuclear weapons]]) are energetic enough to produce muons. Only nuclear fission produces single-nuclear-event energies in this range, but does not produce muons as the production of a single muon is possible only through the [[weak interaction]], which does not take part in a nuclear fission.
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| On Earth, most naturally occurring muons are created by [[cosmic rays]], which consist mostly of protons, many arriving from deep space at very high energy<ref>S. Carroll (2004). Spacetime and Geometry: An Introduction to General Relativity. Addison Wesly. p. 204</ref>
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| {{Quote|About 10,000 muons reach every square meter of the earth's surface a minute; these charged particles form as by-products of cosmic rays colliding with molecules in the upper atmosphere. Traveling at relativistic speeds, muons can penetrate tens of meters into rocks and other matter before attenuating as a result of absorption or deflection by other atoms.<ref>
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| {{Cite journal
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| |author=Mark Wolverton
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| |date=September 2007
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| |title=Muons for Peace: New Way to Spot Hidden Nukes Gets Ready to Debut
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| |url=http://www.sciam.com/article.cfm?id=muons-for-peace
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| |journal=[[Scientific American]]
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| |volume=297 |issue=3 |pages=26–28
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| |doi=10.1038/scientificamerican0907-26
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| }}</ref>}}
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| When a cosmic ray proton impacts atomic nuclei in the upper atmosphere, [[pions]] are created. These decay within a relatively short distance (meters) into muons (their preferred decay product), and [[muon neutrino]]s. The muons from these high energy cosmic rays generally continue in about the same direction as the original proton, at a velocity near the speed of light. Although their lifetime ''without'' relativistic effects would allow a half-survival distance of only about 0.66 km (660 meters) at most (as seen from Earth) the [[time dilation]] effect of [[special relativity]] (from the viewpoint of the Earth) allows cosmic ray secondary muons to survive the flight to the Earth's surface, since in the Earth frame, the muons have a longer half life due to their velocity. From the viewpoint ([[inertial frame]]) of the muon, on the other hand, it is the [[Fitzgerald contraction|length contraction]] effect of special relativity which allows this penetration, since in the muon frame, its lifetime is unaffected, but the length contraction causes distances through the atmosphere and Earth to be far shorter than these distances in the Earth rest-frame. Both effects are equally valid ways of explaining the fast muon's unusual survival over distances.
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| Since muons are unusually penetrative of ordinary matter, like neutrinos, they are also detectable deep underground (700 meters at the [[Soudan II]] detector) and underwater, where they form a major part of the natural background ionizing radiation. Like cosmic rays, as noted, this secondary muon radiation is also directional.
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| The same nuclear reaction described above (i.e. hadron-hadron impacts to produce pion beams, which then quickly decay to muon beams over short distances) is used by particle physicists to produce muon beams, such as the beam used for the muon [[G-factor (physics)|''g'' − 2 experiment]].<ref>
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| {{cite press
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| |publisher=[[Brookhaven National Laboratory]]
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| |date=30 July 2002
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| |title=Physicists Announce Latest Muon g-2 Measurement
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| |url=http://www.bnl.gov/bnlweb/pubaf/pr/2002/bnlpr073002.htm
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| |accessdate=2009-11-14
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| }}</ref>
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| ==Muon decay==
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| {{See also|Michel parameters}}
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| [[Image:Muon Decay.svg|right|thumb|The most common decay of the muon]]
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| Muons are unstable elementary particles and are heavier than electrons and neutrinos but lighter than all other matter particles. They decay via the [[weak interaction]]. Because [[lepton number]]s must be conserved, one of the product neutrinos of muon decay must be a muon-type neutrino and the other an electron-type antineutrino (antimuon decay produces the corresponding antiparticles, as detailed below). Because charge must be conserved, one of the products of muon decay is always an electron of the same charge as the muon (a positron if it is a positive muon). Thus all muons decay to at least an electron, and two neutrinos. Sometimes, besides these necessary products, additional other particles that have no net charge and spin of zero (e.g., a pair of photons, or an electron-positron pair), are produced.
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| The dominant muon decay mode (sometimes called the Michel decay after [[Louis Michel (physicist)|Louis Michel]]) is the simplest possible: the muon decays to an electron, an electron antineutrino, and a muon neutrino. Antimuons, in mirror fashion, most often decay to the corresponding antiparticles: a [[positron]], an electron neutrino, and a muon antineutrino. In formulaic terms, these two decays are:
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| <!-- anybody who will make this from <math> will be cursed --> | |
| : {{subatomic particle|muon}} → {{subatomic particle|electron}} + {{subatomic particle|electron antineutrino|link=yes}} + {{subatomic particle|muon neutrino}} , {{subatomic particle|antimuon}} → {{subatomic particle|positron|link=yes}} + {{subatomic particle|electron neutrino}} + {{subatomic particle|muon antineutrino}} .
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| The mean lifetime of the (positive) muon is {{val|2.1969811|0.0000022|u=µs}}.<ref name="PDG2012" /> The equality of the muon and antimuon lifetimes has been established to better than one part in 10<sup>4</sup>.
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| The muon [[decay width]] is, from [[Fermi's golden rule]]:
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| :<math>\Gamma=\frac{G_F^2 m_\mu^5}{192\pi^3}I\left(\frac{m_e^2}{m_\mu^2}\right),</math>
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| where <math>I(x)=1-8x-12x^2\ln x+8x^3-x^4</math> and <math>G_F </math> is the [[Fermi constant|Fermi coupling constant]], <math> x=2E_e/{m_\mu}c^2 </math>
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| The decay distributions of the electron in muon decays have been parameterised using the so-called [[Michel parameters]]. The values of these four parameters are predicted unambiguously in the [[Standard Model]] of [[particle physics]], thus muon decays represent a good test of the space-time structure of the [[weak interaction]]. No deviation from the Standard Model predictions has yet been found.
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| For the decay of the muon, the expected decay distribution for the [[Standard Model]] values of Michel parameters is
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| :<math>\frac{d^2\Gamma}{dx\,d\cos\theta} \sim x^2[(3-2x) + P_{\mu}\cos\theta(1-2x)].</math>
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| Integration of this expression over electron energy gives the angular distribution of the daughter electrons:
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| :<math>\frac{d\Gamma}{d\cos\theta} \sim 1 - \frac{1}{3}P_{\mu}\cos\theta.</math>
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| The electron energy distribution integrated over the polar angle is
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| :<math>\frac{d\Gamma}{dx} \sim (3x^2-2x^3).</math>
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| Due to the muons decaying by the weak interaction, [[Parity (physics)|parity]] conservation is violated. Replacing the <math>\cos\theta</math> term in the expected decay values of the Michel Parameters with a <math>\cos\omega t</math> term, where {{mvar|ω}} is the Larmor frequency from [[Larmor precession]] of the muon in a uniform magnetic field, given by:
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| <math>\omega = \frac{egB}{2m}</math>
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| where {{mvar|m}} is mass of the muon, {{mvar|e}} is charge, {{mvar|g}} is the muon [[g-factor (physics)|g-factor]] and {{mvar|B}} is applied field.
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| A change in the electron distribution computed using the standard, unprecessional, Michel Parameters can be seen displaying a periodicity of π [[radian]]s. This can be shown to physically correspond to a phase change of π, introduced in the electron distribution as the angular momentum is changed by the action of the [[charge conjugation|charge conjugation operator]], which is conserved by the weak interaction.
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| The observation of Parity violation in muon decay can be compared to the concept of violation of parity in weak interactions in general as an extension of [[The Wu Experiment]], as well as the change of angular momentum introduced by a phase change of π corresponding to the charge-parity operator being invariant in this interaction. This fact is true for all [[lepton]] interactions in The Standard Model.
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| Certain neutrino-less decay modes are kinematically allowed but forbidden in the Standard Model. Examples forbidden by lepton flavour conservation are:
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| :{{subatomic particle|muon}} → {{subatomic particle|electron}} + {{subatomic particle|photon}} and
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| :{{subatomic particle|muon}} → {{subatomic particle|electron}} + {{subatomic particle|positron}} + {{subatomic particle|electron}} .
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| Observation of such decay modes would constitute clear evidence for theories [[beyond the Standard Model]]. Upper limits for the branching fractions of such decay modes were measured in many experiments starting more than 50 years ago. The current upper limit for the {{subatomic particle|antimuon}} → {{subatomic particle|positron}} + {{subatomic particle|photon}} branching fraction was measured 2013 in the [[Mu to E Gamma|MEG]] experiment and is 5.7 × 10<sup>−13</sup>.<ref>{{cite journal|author=J. Adam (MEG Collaboration)|title=New Constraint on the Existence of the mu+ -> e+ gamma Decay|journal=Physical Review Letters|volume=110|issue=20|year=2013|pages=201801 |doi = 10.1103/PhysRevLett.110.201801|arxiv=1303.0754 |bibcode = 2013PhRvL.110t1801A |author-separator=,|displayauthors=1|display-authors=29|last2=Bai|last3=Baldini|last4=Baracchini|last5=Bemporad|last6=Boca|last7=Cattaneo|last8=Cavoto|last9=Cei|last10=Cerri|last11=De Bari|last12=De Gerone|last13=Doke|last14=Dussoni|last15=Egger|last16=Fujii|last17=Galli|last18=Gatti|last19=Golden|last20=Grassi|last21=Graziosi|last22=Grigoriev|last23=Haruyama|last24=Hildebrandt|last25=Hisamatsu|last26=Ignatov|last27=Iwamoto|last28=Kaneko|last29=Kettle|last30=Khazin}}</ref>
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| ==Muonic atoms==
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| The muon was the first [[elementary particle]] discovered that does not appear in ordinary [[atom]]s. Negative muons can, however, form muonic atoms (also called [[exotic atom|mu-mesic atoms]]), by replacing an electron in ordinary atoms. Muonic hydrogen atoms are much smaller than typical hydrogen atoms because the much larger mass of the muon gives it a much more localized [[ground state|ground-state]] [[wavefunction]] than is observed for the electron. In multi-electron atoms, when only one of the electrons is replaced by a muon, the size of the atom continues to be determined by the other electrons, and the atomic size is nearly unchanged. However, in such cases the orbital of the muon continues to be smaller and far closer to the nucleus than the [[atomic orbital]]s of the electrons.
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| Muonic [[helium]] is created by substituting a muon for one of the electrons in helium-4. The muon orbits much closer to the nucleus, so muonic helium can therefore be regarded like an isotope of hydrogen whose nucleus consists of two neutrons, two protons and a muon, with a single electron outside. Colloquially, it could be called "hydrogen 4.1", since the mass of the muon is roughly 0.1 [[atomic mass unit|au]]. Chemically, muonic helium, possessing an unpaired [[valence electron]], can [[chemical bond|bond]] with other atoms, and behaves more like a hydrogen atom than an inert helium atom.<ref>{{Cite journal
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| | title = Kinetic Isotope Effects for the Reactions of Muonic Helium and Muonium with H2
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| | journal = Science
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| | volume = 331
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| | issue = 6016
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| | pages = 448–450
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| | date = 28 Jan 2011
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| | url = http://www.sciencemag.org/content/331/6016/448.short
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| | doi = 10.1126/science.1199421
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| | accessdate =
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| | last1 = Fleming
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| | first1 = D. G.
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| | last2 = Arseneau
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| | first2 = D. J.
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| | last3 = Sukhorukov
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| | first3 = O.
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| | last4 = Brewer
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| | first4 = J. H.
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| | last5 = Mielke
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| | first5 = S. L.
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| | last6 = Schatz
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| | first6 = G. C.
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| | last7 = Garrett
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| | first7 = B. C.
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| | last8 = Peterson
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| | first8 = K. A.
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| | last9 = Truhlar
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| | first9 = D. G.
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| | pmid = 21273484 |bibcode = 2011Sci...331..448F | display-authors = 9
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| }}</ref>
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| A positive muon, when stopped in ordinary matter, can also bind an electron and form an exotic atom known as [[muonium]] (Mu) atom, in which the muon acts as the nucleus. The positive muon, in this context, can be considered a pseudo-isotope of hydrogen with one ninth of the mass of the proton. Because the [[reduced mass]] of muonium, and hence its [[Bohr radius]], is very close to that of [[hydrogen]], this short-lived "atom" behaves chemically — to a first approximation — like [[hydrogen]], [[deuterium]] and [[tritium]].
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| ==Use in measurement of the proton charge radius==
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| The recent culmination of a twelve year experiment at investigating the proton's charge radius involved the use of [[muonic hydrogen]]. This form of hydrogen is composed of a muon orbiting a proton.<ref>TRIUMF Muonic Hydrogen collaboration. "A brief description of Muonic Hydrogen research". Retrieved 2010-11-7</ref> The [[Lamb shift]] in muonic hydrogen was measured by driving the muon from its 2s state up to an excited 2[[azimuthal quantum number|p]] state using a laser. The frequency of the photon required to induce this transition was revealed to be 50 terahertz which, according to present theories of [[quantum electrodynamics]], yields a value of 0.84184 ± 0.00067 [[femtometre]]s for the charge radius of the proton.<ref>Pohl, Randolf et al. "''The Size of the Proton''" ''Nature'' 466, 213–216 (8 July 2010)</ref>
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| ==Anomalous magnetic dipole moment==
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| The [[anomalous magnetic dipole moment]] is the difference between the experimentally observed value of the magnetic dipole moment and the theoretical value predicted by the [[Dirac equation]]. The measurement and prediction of this value is very important in the [[precision tests of QED]] ([[quantum electrodynamics]]). The E821 experiment<ref>{{cite web|url=http://www.g-2.bnl.gov/ |title=The Muon g-2 Experiment Home Page |publisher=G-2.bnl.gov |date=2004-01-08 |accessdate=2012-01-06}}</ref> at [[Brookhaven National Laboratory]] (BNL) studied the precession of muon and anti-muon in a constant external magnetic field as they circulated in a confining storage ring. The E821 Experiment reported the following average value <ref>{{cite web|url=http://pdg.lbl.gov/2007/reviews/g-2_s004219.pdf |title=(from the July 2007 review by Particle Data Group) |format=PDF |date= |accessdate=2012-01-06}}</ref>
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| :<math>a = \frac{g-2}{2} = 0.00116592080(54)(33)</math>
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| where the first errors are statistical and the second systematic.
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| The prediction for the value of the muon anomalous magnetic moment includes three parts:
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| : α<sub>μ</sub><sup>SM</sup> = α<sub>μ</sub><sup>QED</sup> + α<sub>μ</sub><sup>EW</sup> + α<sub>μ</sub><sup>had</sup>.
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| The difference between the [[g-factor (physics)|g-factors]] of the muon and the electron is due to their difference in mass. Because of the muon's larger mass, contributions to the theoretical calculation of its anomalous magnetic dipole moment from [[Standard Model]] [[weak interaction]]s and from contributions involving [[hadron]]s are important at the current level of precision, whereas these effects are not important for the electron. The muon's anomalous magnetic dipole moment is also sensitive to contributions from new physics [[beyond the Standard Model]], such as [[supersymmetry]]. For this reason, the muon's anomalous magnetic moment is normally used as a probe for new physics beyond the Standard Model rather than as a test of QED.<ref>{{cite journal |doi=10.1016/j.physletb.2007.04.012 |last1=Hagiwara |first1=K |last2=Martin |first2=A |last3=Nomura |first3=D |last4=Teubner |first4=T |title=Improved predictions for g−2g−2 of the muon and αQED(MZ2) |journal=Physics Letters B |volume=649 |issue=2–3 |page=173 |arxiv=hep-ph/0611102 |year=2007|bibcode = 2007PhLB..649..173H }}</ref>
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| ==See also==
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| * [[Exotic_atom#Muonic_atoms|Muonic atoms]]
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| * [[Muon spin spectroscopy]]
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| * [[Muon-catalyzed fusion]]
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| * [[Muon Tomography]]
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| * [[List of particles]]
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| ==References==
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| {{Reflist}}
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| {{Refbegin}}
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| * {{Cite journal
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| |author=S.H. Neddermeyer, C.D. Anderson
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| |year=1937
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| |title=Note on the Nature of Cosmic-Ray Particles
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| |journal=[[Physical Review]]
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| |volume=51
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| |issue=10 |pages=884–886
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| |doi=10.1103/PhysRev.51.884
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| |bibcode = 1937PhRv...51..884N |last2=Anderson
| |
| }}
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| * {{Cite journal
| |
| |author=J.C. Street, E.C. Stevenson
| |
| |year=1937
| |
| |title=New Evidence for the Existence of a Particle of Mass Intermediate Between the Proton and Electron
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| |journal=[[Physical Review]]
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| |volume=52
| |
| |issue=9 |pages=1003–1004
| |
| |doi=10.1103/PhysRev.52.1003
| |
| |bibcode = 1937PhRv...52.1003S |last2=Stevenson
| |
| }}
| |
| * {{Cite journal
| |
| |author=G. Feinberg, S. Weinberg
| |
| |year=1961
| |
| |title=Law of Conservation of Muons
| |
| |journal=[[Physical Review Letters]]
| |
| |volume=6
| |
| |issue=7 |pages=381–383
| |
| |doi=10.1103/PhysRevLett.6.381
| |
| |bibcode = 1961PhRvL...6..381F |last2=Weinberg
| |
| }}
| |
| * {{Cite book
| |
| |author=Serway & Faughn
| |
| |year=1995
| |
| |title=College Physics
| |
| |page=841 |edition=4th
| |
| |publisher=[[Saunders]]
| |
| |isbn=
| |
| }}
| |
| * {{Cite book
| |
| |author=M. Knecht
| |
| |year=2003
| |
| |chapter=The Anomalous Magnetic Moments of the Electron and the Muon
| |
| |url=http://books.google.com/?id=me6ftonVM_EC&pg=PA265&lpg=PA265&dq=%22The+Anomalous+Magnetic+Moments+of+the+Electron+and+the+Muon%22&q=%22The%20Anomalous%20Magnetic%20Moments%20of%20the%20Electron%20and%20the%20Muon%22
| |
| |editor=B. Duplantier, V. Rivasseau
| |
| |title=[[Poincaré Seminar]] 2002: Vacuum Energy – Renormalization
| |
| |series=[[Progress in Mathematical Physics]]
| |
| |volume=30 |page=265
| |
| |publisher=[[Birkhäuser Verlag]]
| |
| |isbn=3-7643-0579-7
| |
| }}
| |
| * {{Cite book
| |
| |author=E. Derman
| |
| |year=2004
| |
| |title=My Life As A Quant
| |
| |publisher=[[John Wiley & Sons|Wiley]]
| |
| |pages=58–62
| |
| |isbn=
| |
| }}
| |
| {{Refend}}
| |
| | |
| ==External links==
| |
| * [http://antwrp.gsfc.nasa.gov/apod/ap050828.html Muon anomalous magnetic moment and supersymmetry]
| |
| * [http://www.g-2.bnl.gov/ g-2 (muon anomalous magnetic moment) experiment]
| |
| * [http://www.npl.uiuc.edu/exp/mulan/ muLan (Measurement of the Positive Muon Lifetime) experiment]
| |
| * [http://pdg.lbl.gov/ The Review of Particle Physics]
| |
| * [http://twist.triumf.ca/ The TRIUMF Weak Interaction Symmetry Test]
| |
| * [http://meg.psi.ch/ The MEG Experiment (Search for the decay Muon → Positron + Gamma)]
| |
| * {{cite web|last=King|first=Philip|title=Making Muons|url=http://www.backstagescience.com/videos/ISIS_muons.html|work=Backstage Science|publisher=[[Brady Haran]]}}
| |
| | |
| {{Particles}}
| |
| {{Use dmy dates|date=September 2010}}
| |
| | |
| [[Category:Leptons]]
| |