141 Scattering Theory
A framework for collisions that is used to relate incoming free-particle states to outgoing amplitudes and cross sections, where a cross section is an effective area that measures the likelihood of a scattering event.
The incident-plus-scattered wave. An incident beam interacting with a short-range target produces an outgoing wave. In the far region the wavefunction is an incident plane wave plus a scattered spherical wave. This principle is used to define the scattering amplitude \(f\).
The asymptotic scattered wave is
\[ \psi(\mathbf{r}) \sim e^{ikz} + f(\theta,\phi)\dfrac{e^{ikr}}{r} \]
where
- \(f\) is the scattering amplitude.
- \(\theta\) and \(\phi\) are scattering angles.
- \(k\) is the wave number.
- \(r\) is the distance from the target.
The differential cross section. The differential cross section is the squared modulus of the scattering amplitude. This principle is used to convert \(f\) into a measured angular distribution.
The differential cross section is
\[ \dfrac{d\sigma}{d\Omega} = \lvert f(\theta,\phi)\rvert^{2} \]
where
- \(\sigma\) is the cross section.
- \(\Omega\) is solid angle.
- \(f\) is the scattering amplitude.
One-dimensional reflection and transmission. In one dimension the same problem is stated as reflection and transmission amplitudes. This principle is used to analyze barriers and wells on the line.
Note: Also called quantum scattering.
141.1 References
- Sakurai, J. J., & Napolitano, J. Modern Quantum Mechanics. Cambridge University Press, 2021. — incident plus scattered wave; amplitude \(f\).
- Hall, B. C. Quantum Theory for Mathematicians. Springer, 2013. — scattering states for short-range potentials.
- Shankar, R. Fundamentals of Physics II. Yale University Press, 2020. — \(\dfrac{d\sigma}{d\Omega}=|f|^{2}\).
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