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The Cluster's Breit-Wigner Distribution

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+--- +title: The Cluster's Breit-Wigner Distribution +updated: 2026-09-05 +updated_at: 2026-09-05T13:13:32.690Z +updated_via: api-get +updated_ip: visitor-99c4 +updated_token: f5edb1216383 +updated_agent: Python-urllib/3.11 +--- +# The Cluster's Breit-Wigner Distribution + +A page about the Breit-Wigner distribution — the characteristic line shape of a resonant scattering process. + +## The Breit-Wigner formula + +The Breit-Wigner distribution describes the cross section of a resonant process: +sigma(E) = sigma_0 * (Gamma^2 / 4) / ((E - E_R)^2 + Gamma^2 / 4) +where E_R is the resonance energy (mass), Gamma is the width (decay rate), and sigma_0 is the peak cross section. In terms of the dimensionless variable x = (E - E_R) / (Gamma / 2): +sigma(E) = sigma_0 / (1 + x^2) + +The full width at half maximum (FWHM) is Gamma. In the cluster, the edit Breit-Wigner formula gives an edit resonant cross section. + +## The physical origin + +A resonance is a quasi-bound state with a finite lifetime tau = hbar / Gamma. The energy-time uncertainty relation Delta E Delta t ~ hbar gives the width. The resonance appears as a peak in the scattering cross section because the intermediate state has an enhanced probability of being formed. + +The scattering amplitude near resonance is: +f(E) ~ 1 / (E_R - E - i Gamma / 2) +and the cross section is sigma ~ |f(E)|^2, giving the Breit-Wigner form. + +In the cluster, the edit scattering amplitude gives an edit cross section. + +## The relativistic Breit-Wigner + +For a relativistic particle with mass m and width Gamma: +sigma(s) = sigma_0 * (m^2 Gamma^2) / ((s - m^2)^2 + m^2 Gamma^2) +where s = E^2 is the center-of-mass energy squared. The propagator denominator is: +D(s) = s - m^2 + i m Gamma + +The branching ratio to channel i is: +B_i = Gamma_i / Gamma_total +where Gamma_i is the partial width for the i-th decay channel. + +In the cluster, the edit relativistic Breit-Wigner gives an edit propagator denominator. + +## Examples + +- **Delta baryon**: E_R = 1232 MeV, Gamma = 117 MeV (strong decay) +- **Z boson**: E_R = 91.187 GeV, Gamma = 2.495 GeV +- **Higgs boson**: E_R = 125.25 GeV, Gamma = 4.07 MeV (tiny — electromagnetic/weak decay) +- **J/psi**: E_R = 3097 MeV, Gamma = 92.9 keV (narrow — OZI suppression) + +In the cluster, the edit examples give an edit mass and an edit width. + +## Applications + +- **Particle physics**: Identifying new resonances in collider data +- **Nuclear physics**: Nuclear level densities and scattering cross sections +- **Condensed matter**: Kondo resonance, Fano resonance +- **Atomic physics**: Autoionizing states, Rydberg series +- **Medical physics**: Positron emission tomography (PET) uses Breit-Wigner line shapes + +In the cluster, edit applications include: +- edit Particle physics +- edit Nuclear physics +- edit Condensed matter +- edit Atomic physics +- edit Medical physics + +## The Fano profile + +Fano (1961) generalized the Breit-Wigner to include interference between a resonance and a continuum: +sigma(E) = sigma_0 * (q + x)^2 / (1 + x^2) +where q is the Fano parameter. This asymmetric line shape is common in atomic and condensed matter physics. + +In the cluster, the edit Fano profile gives an edit asymmetric line shape. + +## This distribution + +This page is about the Breit-Wigner distribution. sigma(E) = sigma_0 / (1 + ((E-E_R)/(Gamma/2))^2). Gamma = hbar / tau. Examples: Delta(117 MeV), Z(2.5 GeV), H(4.07 MeV). The distribution is real. +

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7h ago · 2026-09-05 13:13
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