Classical scattering off a paraboloid

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SUMMARY

The discussion centers on classical scattering of particles from a paraboloid defined by the equation z = a((y²+x²)/R² - 1), where a and R are constants. It establishes that a minimum scattering angle exists, defined by the equation tan(θ_min/2) = R/2a. The restriction x² + y² ≤ R² is crucial as it limits the impact parameter s, ensuring that s cannot exceed R. The conversation also touches on the relationship between the scattering angle and Rutherford scattering, specifically regarding the sin⁻⁴(θ/4) dependence.

PREREQUISITES
  • Understanding of classical mechanics and scattering theory
  • Familiarity with mathematical concepts such as trigonometry and geometry
  • Knowledge of paraboloid shapes and their equations
  • Basic principles of particle physics
NEXT STEPS
  • Study the derivation of scattering angles in classical mechanics
  • Explore the implications of the impact parameter in scattering experiments
  • Investigate the relationship between classical scattering and quantum mechanics
  • Learn about Rutherford scattering and its mathematical formulations
USEFUL FOR

Students and researchers in physics, particularly those focusing on classical mechanics, scattering theory, and particle physics. This discussion is beneficial for anyone looking to deepen their understanding of scattering phenomena involving geometric shapes.

ehrenfest
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Homework Statement


Particles are scattered (classically) from a paraboloid shape. The surface is given by the relation:

[tex]z = a \left(\frac{y^2+x^2}{R^2}-1 \right)[/tex]
for x^2 +y^2 leq R^2 where a and R are constants. The particle is incident from z = -infinity with impact parameter s.
Show that there a minimum angle below which there is no scattering occurs given by

[tex]tan(\theta_{min}/2) = R/2a[/tex]

where theta is the scattering angle.

Homework Equations


The Attempt at a Solution



I found [itex]\tan(\theta/2) = R^2/2sa[/itex]. The problem implies that s cannot be greater than 1, which I fail to understand.

I am not sure why the restriction "x^2 +y^2 leq R^2" was included. Maybe that has something to do with this...

EDIT: I got it! x^2 +y^2 leq R^2 effectively cuts off the paraboloid at the x-y plane. The cross-section of the paraboloid on the x-y plane is the circle x^2+y^2 = R^2. Therefore the impact parameter cannnot be greater than R, which implies that [itex]\tan(\theta/2) \geq R/2a[/itex] as desired.
 
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The last part of this problem asks: Does the [itex]\sin^{-4}(\theta/4)[/itex] dependence have anything to do with Rutherford scattering?

Anyone have any ideas?
 

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