The relativistic Breit–Wigner distribution (after the 1936 nuclear resonance formula^{[1]} of Gregory Breit and Eugene Wigner) is a continuous probability distribution with the following probability density function,^{[2]}
where k is a constant of proportionality, equal to
 with
(This equation is written using natural units, ħ = c = 1.)
It is most often used to model resonances (unstable particles) in highenergy physics. In this case, E is the centerofmass energy that produces the resonance, M is the mass of the resonance, and Γ is the resonance width (or decay width), related to its mean lifetime according to τ = 1/Γ. (With units included, the formula is τ = ħ/Γ.)
The probability of producing the resonance at a given energy E is proportional to f (E), so that a plot of the production rate of the unstable particle as a function of energy traces out the shape of the relativistic Breit–Wigner distribution. Note that for values of E off the maximum at M such that E^{2} − M^{2} = MΓ, (hence E − M = Γ/2 for M ≫ Γ), the distribution f has attenuated to half its maximum value, which justifies the name for Γ, width at halfmaximum.
In the limit of vanishing width, Γ → 0, the particle becomes stable as the Lorentzian distribution f sharpens infinitely to 2Mδ(E^{2} − M^{2}).
In general, Γ can also be a function of E; this dependence is typically only important when Γ is not small compared to M and the phase spacedependence of the width needs to be taken into account. (For example, in the decay of the rho meson into a pair of pions.) The factor of M^{2} that multiplies Γ^{2} should also be replaced with E^{2} (or E ^{4}/M^{2}, etc.) when the resonance is wide.^{[3]}
The form of the relativistic Breit–Wigner distribution arises from the propagator of an unstable particle,^{[4]} which has a denominator of the form p^{2} − M^{2} + iMΓ. (Here, p^{2} is the square of the fourmomentum carried by that particle in the tree Feynman diagram involved.) The propagator in its rest frame then is proportional to the quantummechanical amplitude for the decay utilized to reconstruct that resonance,
The resulting probability distribution is proportional to the absolute square of the amplitude, so then the above relativistic Breit–Wigner distribution for the probability density function.
The form of this distribution is similar to the amplitude of the solution to the classical equation of motion for a driven harmonic oscillator damped and driven by a sinusoidal external force. It has the standard resonance form of the Lorentz, or Cauchy distribution, but involves relativistic variables s = p^{2}, here = E^{2}. The distribution is the solution of the differential equation for the amplitude squared w.r.t. the energy energy (frequency), in such a classical forced oscillator,
with
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✪ BreitWigner Resonances ☆ Physics Lecture

✪ Mod07 Lec40 Fano parameterization of BreitWigner formula

✪ Mod06 Lec39 BreitWigner Resonances
Transcription
References
 ^ Breit, G.; Wigner, E. (1936). "Capture of Slow Neutrons". Physical Review. 49 (7): 519. Bibcode:1936PhRv...49..519B. doi:10.1103/PhysRev.49.519.
 ^ See Pythia 6.4 Physics and Manual (page 98 onwards) for a discussion of the widths of particles in the PYTHIA manual. Note that this distribution is usually represented as a function of the squared energy.
 ^ Bohm, A.; Sato, Y. (2005). "Relativistic resonances: Their masses, widths, lifetimes, superposition, and causal evolution". Physical Review D. 71 (8). arXiv:hepph/0412106. Bibcode:2005PhRvD..71h5018B. doi:10.1103/PhysRevD.71.085018.
 ^ Brown, L S (1994). Quantum Field Theory, Cambridge University press, ISBN 9780521469463 , Chapter 6.3.