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Interaction Cross-Section

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Interaction Cross-Section
Concept and Application in Nuclear Physics

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Definition
The interaction cross-section is the probability of interaction of ionizing particles with one atom,
an electron, the nucleus of an atom, or all the atoms (electrons, nuclei) located in a given volume
of matter..

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Historical Context
Rutherford Experiment (1909): α-particle scattering on gold nuclei
Rutherford Formula: description of elastic Coulomb scattering
Concept Introduction: cross-section as measure of process probability
Theory Development: quantum mechanics and nuclear physics

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Physical Meaning
Geometric Interpretation
If a particle were a solid sphere, σ would equal the cross-sectional area of that sphere
Probabilistic Interpretation
The larger σ, the higher the probability of interaction upon particle collision

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Main Formula
σ = N / (n × Φ)
N — number of particles interacting with the target
n — number of target nuclei per unit area
Φ — incident particle flux density

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Types of Cross-Sections
Total (σ_total): sum of all processes
Elastic Scattering: without particle energy change
Inelastic Scattering: with internal state change
Absorption/Capture: particle is absorbed by the nucleus

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Units of Measurement
Primary unit: barn (b)
1 barn = 10⁻²⁴ cm² = 10⁻²⁸ m²
Order of magnitude comparable to nuclear cross-sectional area
Name derived from the phrase "big as a barn"

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Energy Dependence
Neutron Capture: σ ∝ 1/v (inversely proportional to velocity)
Scattering: depends on type of interaction
Threshold Effects: emergence of new channels above certain energy
Resonances: significant σ increase at specific energies

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Practical Applications
Nuclear Energy
Chain reaction control in reactors
Radiation Protection
Shielding and safety calculations
Experimental Physics
Analysis of particle collision results

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Key Takeaways
Interaction cross-section is a fundamental characteristic of collision probability in particle physics
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