Lecture Description
With our aim of localizing the wave function, we use a Gaussian wave packet in the form of φ(k) for our Fourier Transform. The values of the function φ(k) will be used as the amplitudes of the solutions that when superimposed, interfere constructively in a finite region.
Course Index
- The Free Particle: Continuous States
- The Free Particle: Analyzing the Solutions
- The Free Particle: Are Continuous States Physical?
- The Free Particle: A Gaussian Wave Packet
- The Free Particle: Calculating Our Wave Packet
- Solving the Schrödinger Equation
- Description of Plane Waves
- Probability Current Density
- Calculating R and T
- Explaining Quantum Behavior
- Particle-like Gets Stopped
- The Strange Evanescent Wave
- Infinite Square Well: Deriving Discrete Energy Value
- Infinite Square Well: What is Zero-Point Energy?
- Infinite Square Well: Unusual Probability Densities
- The Scattering Problem
- Ratio Transmitted Particles
- Energy Values and Resonance
- Full Transmission of Part
- Tunneling: Setting the Situation
- Tunneling: Deciphering the Wave-like Particle
- Tunneling: Penetrating the Potential Barrier
- Tunneling: Further Analysis of T
- Tunneling: The WKB Approximation Method
- Introduction
- Unphysical Solutions
- Fourier Transform Revisit
- Outside the Well
- Anti/Symmetric Solutions
- Boundary Conditions
- A Graphical Solution
- Discrete Energy Specturm
Course Description
In this course, GMath Physics Instructor Donny Lee gives 32 video lessons on Quantum Mechanics and Physical Problems in One-Dimension.
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