TwoDimensional Scattering Across a TopHat Potential - PowerPoint PPT Presentation

1 / 23
About This Presentation
Title:

TwoDimensional Scattering Across a TopHat Potential

Description:

For example what happens when two protons collide? ... The wave function DOES contain information about the probability a particle will ... – PowerPoint PPT presentation

Number of Views:21
Avg rating:3.0/5.0
Slides: 24
Provided by: jennifere3
Category:

less

Transcript and Presenter's Notes

Title: TwoDimensional Scattering Across a TopHat Potential


1
Two-Dimensional Scattering Across a Top-Hat
Potential
  • Jennifer L. Ellsworth
  • Wells College
  • May 3, 2000

2
Overview
  • Define scattering
  • Classical examples of scattering
  • Scattering in the quantum realm
  • Importance of scattering problems
  • Top-hat potential
  • Future directions

3
Scattering Definition
  • In general, scattering means to bring about a
    less orderly arrangement, either in position or
    direction.
  • More specifically, the term denotes the change
    in direction of particles owing to collisions
    with other particles or systems.
  • The system for this project was the top-hat
    potential.

4
Transmission
  • If a kangaroo jumps into a pool of water, he will
    be transmitted through the surface of the water
    into the pool.

5
Scattering
  • If the same kangaroo then tries to jump through
    concrete, he will bounce right back off again at
    some angle. This is scattering.

Concrete
6
Quantum Effects
  • Small particles like microscopic baseballs,
    protons, and electrons can behave differently.
    There is a positive probability that they will
    pass through barriers that classically are
    impenetrable.

7
Tunneling
  • This would be like our kangaroo jumping through a
    block of concrete.

Concrete
8
Why is scattering important?
  • Electricity and magnetism predict behavior of
    electromagnetic waves incident on charged
    particles.
  • Particle physics predict interaction between
    microscopic particles. For example what happens
    when two protons collide?
  • Nanoelectronics predict behavior of very, very
    small electronic components such as single
    electron transistors.

9
Goal
  • Predict the behavior of particles incident on a
    top-hat potential, when motion is constrained to
    two dimensions.

10
Potential
  • Potential is available energy, rather than active
    energy.
  • A potential barrier is a region including a
    maximum of potential which hinders a low energy
    particle on one side of the region from passing
    to the other side.
  • Example electrical repulsion of positively
    charged particles from the nucleus of an atom.

11
Top-Hat Potential
  • Top-hat potential energy curve of height V0 and
    radius a.
  • The potential can be split into two regionsa
    region where there is zero potential and a region
    where there is potential V0.

a
V0
Zero potential
12
Schrödingers Equation
  • A particle can be described by a wave function.
  • The wave function does NOT describe the physical
    path of the particle.
  • The wave function DOES contain information about
    the probability a particle will be found in any
    given region of space.
  • The wave function of a particle is an
    eigenfunction of Schrödingers equation.

13
General Scattering Problem
Incident waves (red) and scattered waves (blue)
are shown relative to a scattering center or top
hat portion of the potential (yellow).
14
Wave Functions
  • The wave function is denoted by the symbol ?.
  • Wave functions were found for the incident wave
    (shown in red in the last slide), and the general
    scattered wave (shown in blue in the last slide).

15
Bessel Functions
16
Cross Section and Phase Shift
  • A measure of the probability of scattering a
    particle out of a beam.
  • An angle that gives the relationship between the
    phase of the incident wave and the phase of the
    scattered wave.
  • Value must be between -? and ?.

17
Approach
  • Approximate the ?inc at large r.
  • Approximate the ?scatt at large r.
  • Approximate the total wave function ?tot at large
    r.
  • Set ?inc ?scatt ?tot then solve for cross
    section in terms of the phase shift.
  • Evaluate results based on estimations of phase
    shift for long and short wavelengths.

18
Asymptotic Wave Functions
19
Details
  • Set ?inc ?scatt ?tot
  • Sines and cosines are linearly independent so the
    coefficients of each of these terms must be
    independently equal.
  • This gives us two equations and two unknowns.
  • Solve for Dl in terms of the phase angle.
  • Solve for f(?) in terms of phase angle.
  • Determine cross section in terms of phase angle.

20
Result
  • The total scattering cross section is

21
Future Work
  • Predict cross section in the limit of small and
    large wavelengths.
  • How does the total cross section depend on the
    ratio E/V?
  • Determine if there are any exact solutions to the
    problem.
  • How does the total cross section change with time?

22
Acknowledgements
  • Dr. Steve Rae
  • Dr. Carol Shilepsky
  • Dr. Tom Stiadle
  • Joan Poore

23
Any Questions?
Write a Comment
User Comments (0)
About PowerShow.com