The Optical Theorem (Total cross section?)

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SUMMARY

The discussion centers on the optical theorem as presented in Sakurai's work, specifically the equation σtotal = (4π/k)Im(f(0)), where f(0) represents the forward scattering amplitude. Participants clarify that the total cross section refers to the scattering of an incoming wave function integrated over all directions around a scatterer, confirming that it encompasses both elastic and inelastic scattering processes. The conversation also highlights the relationship between the optical theorem and fundamental principles such as S-matrix theory, causality, and unitarity.

PREREQUISITES
  • Understanding of the optical theorem in quantum mechanics
  • Familiarity with scattering amplitudes and cross sections
  • Knowledge of S-matrix theory and its implications
  • Basic concepts of elastic and inelastic scattering
NEXT STEPS
  • Study the derivation of the optical theorem in Sakurai's "Modern Quantum Mechanics"
  • Explore the relationship between scattering amplitudes and differential cross sections
  • Investigate the implications of causality and unitarity in quantum scattering
  • Learn about detailed balance in kinetic theory and its connection to the optical theorem
USEFUL FOR

Physicists, particularly those specializing in quantum mechanics, scattering theory, and theoretical physics, will benefit from this discussion. It is also relevant for students and researchers looking to deepen their understanding of the optical theorem and its applications.

Xyius
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I am going over the optical theorem (specifically from Sakurai) and I just have a simple couple of questions. The optical theorem says

\sigma_{total}=\frac{4\pi}{k}\text{Im}(f(0))

Where ##f(0)## is the scattering amplitude in the forward direction. (Which I am assuming means the direction parallel to the incident direction. Or does it mean in the direction back towards the source?)

I just want to verify what is meant by the total cross section. To me the total cross section means the amount the incoming wave function is scattered integrated in all directions over a sphere around the scatterer. Is this the correct way of thinking?
 
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Xyius said:
(Which I am assuming means the direction parallel to the incident direction. Or does it mean in the direction back towards the source?)
The parallel one, not the antiparallel.
Xyius said:
To me the total cross section means the amount the incoming wave function is scattered integrated in all directions over a sphere around the scatterer
Differential cross-section is defined as the fraction of the scattered probability current at certain direction, fraction means relative to the incoming probability current. The total cross section is the sum of differential cross section over all directions.
 
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Thank you! (Sorry for the late reply!)
 
It's worth mentioning that on the left-hand side stands the total cross section, including both elastic and inelastic channels, while on the right-hand side there's the elastic scattering amplitude.

The optical theorem can be generalized to more general scattering processes than just single-particle scattering on a potential. It reflects the very fundamental principles of S-matrix theory, causality and unitarity and is closely linked to detailed balance in kinetic theory.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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