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Resonance (particle physics)

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Concept in scattering theory

Inparticle physics, aresonance is the peak located around a certain energy found indifferential cross sections ofscattering experiments. These peaks are associated withsubatomic particles, which include a variety ofbosons,quarks andhadrons (such asnucleons,delta baryons orupsilon mesons) and theirexcitations. In common usage, "resonance" only describes particles with very shortlifetimes, mostly high-energy hadrons existing for10−23 seconds or less. It is also used to describe particles in intermediate steps of a decay, so-calledvirtual particles.[1]

Thewidth of the resonance (Γ) is related to themean lifetime (τ) of the particle (or its excited state) by the relation

Γ=τ{\displaystyle \Gamma ={\frac {\hbar }{\tau }}}

where=h2π{\displaystyle {\hbar }={\frac {h}{2\pi }}} andh is thePlanck constant.

Thus, the lifetime of a particle is the directinverse of the particle's resonance width. For example, the chargedpion has the second-longest lifetime of any meson, at2.6033×10−8 s.[2] Therefore, its resonance width is very small, about2.528×10−8 eV or about 6.11MHz. Pions are generally not considered as "resonances". The chargedrho meson has a very short lifetime, about4.41×10−24 s. Correspondingly, its resonance width is very large, at 149.1MeV or about 36ZHz. This amounts to nearly one-fifth of the particle'srest mass.[3]

See also

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References

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  1. ^Dudley, Chris."What is a Resonance Particle?".phy.duke.edu. Retrieved24 April 2017.
  2. ^K.A. Oliveet al. (Particle Data Group) (2016):Particle listings –π±
  3. ^K.A. Oliveet al. (Particle Data Group) (2016):Particle listings –ρ
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