Unbound States 1. A review about the discussions we have had so far on the Schrödinger equation. 2. Quiz Topics in Unbound States:  The potential step.  Two steps: The potential barrier and tunneling.  Real-life examples: Alpha decay and other applications.  A summary: Particle-wave propagation. today Thurs.

Review: The Schrödinger equation The free particle Schrödinger Equation: From  The Schrödinger Equation The plane wave solution And this leads to the equation that adds an external potential Solve for with the knowledge of, for problems in QM. The momentum of this particle: completely defined. The location of this particle: and We understand this equation as energy accounting undefined.

Review: the time independent Schrödinger equation and the two conditions for the wave function When the wave function can be expressed as and the time independent Schrödinger Equation: We have found The solution of this equation is the stationary states because The probability of finding a particle does not depend on time: Normalization : The wave function be smooth  the continuity of the wave function and its first order derivative. Two conditions 

Review: Solving the Schrödinger equation. Case 1: The infinite potential well Equation and Solution: Energy and probability 1.Standing wave. 2.The QM ground- state. A bound state particle cannot be stationary, although its wave function is stationary. 3.Energy ratio at each level: n 2. 4.With very large n, QM  CM.

Solving the Schrödinger equation. Case 2: The finite potential well The change  Equations:

Review: Solving the Schrödinger equation. Case 2: The finite potential well Solutions: Energy quantization: Penetration depth:

Review: Solving the Schrödinger equation. Case 3: The simple harmonic oscillator This model is a good approximation of particles oscillate about an equilibrium position, like the bond between two atoms in a di-atomic molecule. Solve for wave function and energy level

Review Solving the Schrödinger equation. Case 3: The simple harmonic oscillator Energy are equally spaced, characteristic of an oscillator Wave function at each energy level Gaussian

Compare Case 1, Case 2 and 3: Energy levels: Wave function: Penetration depth: Wave function: Energy levels:

New cases, unbound states: the potential step From potential well to a one-side well, or a step: Free particle with energy E. Standing waves do not form and energy is no quantized. We discussed about free particle wave function before. Which is: Re-write it in the form Right moving. Why? Right moving (along positive x - axis) wave of free particle: Left moving wave of free particle:

The potential step: solve the equation Initial condition: free particles moving from left to right. When The Schrödinger Equation: When Solution: Inc. Refl. Trans. Why no reflection here? Ans: no 2 nd potential step on the right. Are we done? What do we learn here? Any other conditions to apply to the solutions? Normalization and wave function smoothness When

The potential step: apply conditions Smoothness requires:   Transmission probability: Reflection probability: Express B and C in terms of A :

The potential step: transmission and reflection Now using the definitions of k and k’ : n air Reference: for normal incidence, light transmission probability: Reflection probability: Transmission probability: Reflection probability:  

The potential step: solve the equation Initial condition: free particles moving from left to right. The Schrödinger Equation: When Solution: Inc. Refl. When

The potential step: apply conditions Smoothness requires:   Transmission probability: Reflection probability: Express B in terms of A : Penetration depth: One can prove:

Review questions The plane wave solution of a free particle Schrödinger Equation is The plane wave solution of a free particle Schrödinger Equation is Can you normalize this wave function? Try to solve for the wave function and discuss about transmission and reflection for this situation: Try to solve for the wave function and discuss about transmission and reflection for this situation:

Preview for the next class (10/23) Text to be read: Text to be read: In chapter 6: In chapter 6: Section 6.2 Section 6.2 Section 6.3 Section 6.3 Section 6.4 Section 6.4 Questions: Questions: How much do you know about radioactive decays of isotopes? Have you heard of alpha decay, beta decay and gamma sources? How much do you know about radioactive decays of isotopes? Have you heard of alpha decay, beta decay and gamma sources? Have you heard of the “tunneling effect” in the EE department (only for EE students)? Have you heard of the “tunneling effect” in the EE department (only for EE students)? What is a wave phase velocity? What is a wave group velocity? What is a wave phase velocity? What is a wave group velocity?

Homework 8, due by 10/28 1. Problem 25 on page Problem 34 on page Problem 15 on page Problem 18 on page 224.