Summary of One-Dimensional Systems: Difference between revisions

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Significant Feature: No reflection at certain energies
Significant Feature: No reflection at certain energies


'''6. [[One-Dimensional Bound States#Finite Asymmetric Square Well|''Finite Square Well'' Potential]]'''
'''6. [[One-Dimensional Bound States#Infinite Square Well|''Infinite Square Well'' Potential]]'''
 
Physical Example: Neutron bound in nucleus
 
Significant Feature: Energy quantization
 
'''7. [[One-Dimensional Bound States#Infinite Square Well|''Infinite Square Well'' Potential]]'''


Physical Example: Molecule strictly confined to box
Physical Example: Molecule strictly confined to box
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Significant Feature: Approximation to finite square well
Significant Feature: Approximation to finite square well


'''8. ''Simple Harmonic Oscillator'' Potential'''
'''7. [[One-Dimensional Bound States#Finite Asymmetric Square Well|''Finite Square Well'' Potential]]'''


Physical Example: Atom of vibrating diatomic molecule
Physical Example: Neutron bound in nucleus


Significant Feature: Zero-point energy
Significant Feature: Energy quantization


'''9. [[Motion in a Periodic Potential|''Periodic'' Potential]]'''
'''8. [[Motion in a Periodic Potential|''Periodic'' Potential]]'''


Physical Example: Electron in lattice
Physical Example: Electron in lattice


Significant Feature: Energy band and energy gap
Significant Feature: Energy band and energy gap
== Problem ==
An electron is moving freely inside of a one-dimensional box with walls at <math>x=0\!</math> and <math>x=a.\!</math>  If the electron is initially in the ground state of the box and we suddenly increase the size of the box by moving the right-hand wall instantaneously from <math>x=a\!</math> to <math>x=4a,\!</math> then calculate the probability of finding the electron in
'''(a)''' the ground state of the new box, and
'''(b)''' the first excited state of the new box.
[[Phy5645/One dimensional problem|Solution]]

Latest revision as of 13:32, 8 August 2013

Quantum Mechanics A
SchrodEq.png
Schrödinger Equation
The most fundamental equation of quantum mechanics; given a Hamiltonian , it describes how a state evolves in time.
Basic Concepts and Theory of Motion
UV Catastrophe (Black-Body Radiation)
Photoelectric Effect
Stability of Matter
Double Slit Experiment
Stern-Gerlach Experiment
The Principle of Complementarity
The Correspondence Principle
The Philosophy of Quantum Theory
Brief Derivation of Schrödinger Equation
Relation Between the Wave Function and Probability Density
Stationary States
Heisenberg Uncertainty Principle
Some Consequences of the Uncertainty Principle
Linear Vector Spaces and Operators
Commutation Relations and Simultaneous Eigenvalues
The Schrödinger Equation in Dirac Notation
Transformations of Operators and Symmetry
Time Evolution of Expectation Values and Ehrenfest's Theorem
One-Dimensional Bound States
Oscillation Theorem
The Dirac Delta Function Potential
Scattering States, Transmission and Reflection
Motion in a Periodic Potential
Summary of One-Dimensional Systems
Harmonic Oscillator Spectrum and Eigenstates
Analytical Method for Solving the Simple Harmonic Oscillator
Coherent States
Charged Particles in an Electromagnetic Field
WKB Approximation
The Heisenberg Picture: Equations of Motion for Operators
The Interaction Picture
The Virial Theorem
Commutation Relations
Angular Momentum as a Generator of Rotations in 3D
Spherical Coordinates
Eigenvalue Quantization
Orbital Angular Momentum Eigenfunctions
General Formalism
Free Particle in Spherical Coordinates
Spherical Well
Isotropic Harmonic Oscillator
Hydrogen Atom
WKB in Spherical Coordinates
Feynman Path Integrals
The Free-Particle Propagator
Propagator for the Harmonic Oscillator
Differential Cross Section and the Green's Function Formulation of Scattering
Central Potential Scattering and Phase Shifts
Coulomb Potential Scattering

1. Zero Potential

Physical Example: Proton in beam from cyclotron

Significant Feature: Results used for other systems

2. Step Potential (energy below top)

Physical Example: Conduction electron near surface of metal

Significant Feature: Penetration of excluded region

3. Step Potential (energy above top)

Physical Example: Neutron trying to escape nucleus

Significant Feature: Partial reflection at potential discontinuity

4. Barrier Potential (energy below top)

Physical Example: particle trying to escape Coulomb barrier

Significant Feature: Tunneling

5. Barrier Potential (energy above top)

Physical Example: Electron scattering from negatively ionized atom

Significant Feature: No reflection at certain energies

6. Infinite Square Well Potential

Physical Example: Molecule strictly confined to box

Significant Feature: Approximation to finite square well

7. Finite Square Well Potential

Physical Example: Neutron bound in nucleus

Significant Feature: Energy quantization

8. Periodic Potential

Physical Example: Electron in lattice

Significant Feature: Energy band and energy gap