Breit-Wigner Distribution: What is it & How is it Used?

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SUMMARY

The Breit-Wigner distribution function is essential in calculating scattering cross sections involving intermediate particles, particularly in resonance scenarios. It is mathematically defined as W(s_A) = (1/π)(m_AΓ)/((s_A - m_A²)² + m_A²Γ²), enhancing the cross section when s_A is near m_A². This distribution is notably applied in the study of exotic hadrons like X(3872), which appears as an intermediate particle in reactions such as p+p → X(3872) → D0 + antiD0*. For further understanding, the book "Field Theory in Particle Physics" by De Wit is recommended for its detailed discussion on decay rates and the Breit-Wigner function.

PREREQUISITES
  • Understanding of scattering theory and cross sections
  • Familiarity with resonance phenomena in particle physics
  • Knowledge of decay rates and their calculations
  • Basic grasp of quantum field theory concepts
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  • Study the mathematical derivation of the Breit-Wigner distribution
  • Explore resonance production mechanisms in high-energy physics
  • Learn about decay rates in particle physics using De Wit’s textbook
  • Investigate the properties and significance of exotic hadrons like X(3872)
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Particle physicists, researchers in high-energy physics, and students studying scattering theory and resonance phenomena will benefit from this discussion.

nakulphy
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what is breit wigner distribution function ?
it is used in resonance scan means it decides the no of events for any specific channel. i am also giving the link of the paper where i found this
http://pos.sissa.it/archive/conferences/160/018/Bormio2012_018.pdf

please help me out

thank you
 
Last edited by a moderator:
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The Breit-Wigner distribution is a particular factor appearing in the expression for the scattering cross section when this scattering happens via an intermediate particle. Consider for example the scattering a+b\to A\to X+Y. The expression for the cross section is given by:
$$
\frac{d\sigma(a+b\to X+Y)}{d\vec pd s_X}=\frac{d\Gamma(A\to X)}{\Gamma(A\to all)}\frac{d\sigma(a+b\to A+Y)}{d\vec pd s_A} W(s_A)\sqrt{\frac{\vec p^2+m_A^2}{\vec p^2+s_A}},
$$
where the Breit-Wigner distribution is given by:
$$
W(s_A)=\frac{1}{\pi}\frac{m_A\Gamma}{(s_A-m_A^2)^2+m_A^2\Gamma^2}.
$$
As you can see, such a distribution gives an enhancement of the cross section (i.e. of the number of particles produced) when s_A\simeq m_A^2, provided that the width \Gamma of the intermediate particle is not too large.
 
Last edited:
thank you very much
i will try to understand this and also try to correlate with the paper and will come back to you soon.

thank you
 
The paper itself is about the exotic hadron X(3872). It is a perfect example of resonance. Namely it doesn't appear as a final state of the reaction but as an intermediate particle. It is, for example, produced ad LHC via the reaction: p+p -> X(3872) -> D0 + antiD0*. As you can see this is exactly as the reaction I showed you before.
 
thank you very much.

can you please suggest me the reference book to study this ? actually I understood the things but still I want to understand in more detail.

thank you

Nakul Soni
 
Last edited:
Do you mean the X(3872) or resonances in general?
 
for the basic of Breit-Wigner and the distribution function.
 
One of the best books is De Wit - Field theory in particle physics. In particular the chapter on decay rates
 

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