Unbound States A review on calculations for the potential step.

Slides:



Advertisements
Similar presentations
Tunneling Phenomena Potential Barriers.
Advertisements

A 14-kg mass, attached to a massless spring whose force constant is 3,100 N/m, has an amplitude of 5 cm. Assuming the energy is quantized, find the quantum.
1 Chapter 40 Quantum Mechanics April 6,8 Wave functions and Schrödinger equation 40.1 Wave functions and the one-dimensional Schrödinger equation Quantum.
Electron Tunneling and the Josephson Effect. Electron Tunneling through an Insulator.
Tunneling. Energy Barrier  Kinetic energy is used to overcome potential energy. More for motion past barrier Less creates turning point  Objects with.
LECTURE 19 BARRIER PENETRATION TUNNELING PHENOMENA PHYSICS 420 SPRING 2006 Dennis Papadopoulos.
We’ve learned about this situation: the finite potential well… …but what if we “turn it upside down”? This is a finite potential barrier. When we solved.
Wave mechanics in potentials Modern Ch.4, Physical Systems, 30.Jan.2003 EJZ Particle in a Box (Jason Russell), Prob.12 Overview of finite potentials Harmonic.
Modern Physics 6b Physical Systems, week 7, Thursday 22 Feb. 2007, EJZ Ch.6.4-5: Expectation values and operators Quantum harmonic oscillator → blackbody.
Lecture 4. Application to the Real World Particle in a “Finite” Box (Potential Well) Tunneling through a Finite Potential Barrier References Engel, Ch.
Chapter 41 Quantum Mechanics.
Chapter 41 Quantum Mechanics.
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.
Particles (matter) behave as waves and the Schrödinger Equation 1. Comments on quiz 9.11 and Topics in particles behave as waves:  The (most.
Physics 2170 – Spring Quantum tunneling: STM & electric shock Homework set 12 is due Wednesday. Clicker.
Lecture 16 Tunneling (c) So Hirata, Department of Chemistry, University of Illinois at Urbana-Champaign. This material has been developed and made available.
Quantum Tunneling Tyler Varin, Gereon Yee, & Sirage Siragealdin Dr. Younes Ataiiyan May 12, 2008.
Lecture VII Tunneling. Tunneling An electron of such an energy will never appear here! classically E kin = 1 eV 0 V-2 Vx.
Happyphysics.com Physics Lecture Resources Prof. Mineesh Gulati Head-Physics Wing Happy Model Hr. Sec. School, Udhampur, J&K Website: happyphysics.com.
Bound States 1. A quick review on the chapters 2 to Quiz Topics in Bound States:  The Schrödinger equation.  Stationary States.  Physical.
An Electron Trapped in A Potential Well Probability densities for an infinite well Solve Schrödinger equation outside the well.
1 of xx Klein Tunneling PHYS 503 Physics Colloquium Fall /11 Deepak Rajput Graduate Research Assistant Center for Laser Applications University of.
School of Mathematical and Physical Sciences PHYS August, PHYS1220 – Quantum Mechanics Lecture 6 August 29, 2002 Dr J. Quinton Office: PG.
Topic 5: Schrödinger Equation
Bound States Review of chapter 4. Comment on my errors in the lecture notes. Quiz Topics in Bound States: The Schrödinger equation. Stationary States.
Chapter 41 1D Wavefunctions. Topics: Schrödinger’s Equation: The Law of Psi Solving the Schrödinger Equation A Particle in a Rigid Box: Energies and Wave.
TUNNEL DIODE (Esaki Diode) It was introduced by Leo Esaki in Heavily-doped p-n junction –Impurity concentration is 1 part in 10^3 as compared to.
Hydrogen Atom and QM in 3-D 1. HW 8, problem 6.32 and A review of the hydrogen atom 2. Quiz Topics in this chapter:  The hydrogen atom  The.
Modern Physics (II) Chapter 9: Atomic Structure
Quantum Tunnelling Quantum Physics 2002 Recommended Reading: R.Harris, Chapter 5 Sections 1, 2 and 3.
Free particle in 1D (1) 1D Unbound States
Unbound States 1. A review on calculations for the potential step. 2. Quiz Topics in Unbound States:  The potential step.  Two steps: The potential.
Wednesday, Oct. 31, 2012PHYS , Fall 2012 Dr. Amir Farbin 1 PHYS 3313 – Section 001 Lecture #16 Wednesday, Oct. 31, 2012 Dr. Amir Farbin Reflection.
Introduction to Quantum Mechanics
Physics 2170 – Spring Quantum tunneling:  -decay Exam 2 is done. Please check to make sure I added your.
Nanoelectronics Part II Single-Electron and Few-Electron Phenomena and Devices Chapter 6 Tunnel Junctions and Applications of Tunneling
Wednesday, April 15, 2015 PHYS , Spring 2015 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture # 20 Wednesday, April 15, 2015 Dr. Jaehoon Yu Finite.
Superconductivity, Josephson Junctions, and squids
Lectures in Physics, summer 2008/09 1 Modern physics 4. Barriers and wells.
Application of photodiodes
Schrodinger’s Equation Solutions Finite Square Well
PHYS 3313 – Section 001 Lecture #16
CHAPTER 5 The Schrodinger Eqn.
Chapter 40 Quantum Mechanics
Lecture 16 Tunneling.
and Quantum Mechanical Tunneling
BCS THEORY BCS theory is the first microscopic theory of superconductivity since its discovery in It explains, The interaction of phonons and electrons.
CHAPTER 5 The Schrodinger Eqn.
Elements of Quantum Mechanics
Unbound States A review about the discussions we have had so far on the Schrödinger equation. Topics in Unbound States: The potential step. Two steps:
PHYS274 Quantum Mechanics VII
 Heisenberg’s Matrix Mechanics Schrödinger’s Wave Mechanics
Quantum Physics Schrödinger
CHAPTER 6 Quantum Mechanics II
CHAPTER 5 The Schrodinger Eqn.
Wave functions, Energy Levels and Particle in the Box
Elements of Quantum Mechanics
2. Solving Schrödinger’s Equation
PHYS 3313 – Section 001 Lecture #21
Chapter 40 Quantum Mechanics
Do all the reading assignments.
Free particle wavefunction
L ECE 4243/6243 Fall 2016 UConn F. Jain Notes Chapter L8 (page ).
6: Barrier Tunneling and Atomic Physics
Square Barrier Barrier with E>V0
The Schrödinger Equation
PHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101
CHAPTER 3 PROBLEMS IN ONE DIMENSION Particle in one dimensional box
Chapter 40 Quantum Mechanics
Last hour: Particles at step functions
Presentation transcript:

Unbound States A review on calculations for the potential step. 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

The potential step: solve the equation Initial condition: free particles moving from left to right. The Schrödinger Equation: When When When Solution: Inc. Refl. Trans. Apply normalization and wave function smoothness

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

The potential step: transmission and reflection When When Reflection probability: Reflection probability: Transmission probability: Transmission probability: Penetration depth:

Examples An electron of kinetic energy 5 eV encounters a 2 eV potential step. What is the probability that it will be reflected? This is the case when Straightforward, right? How about this: An electron of kinetic energy 5 eV encounters a 2 eV potential step down. What is the probability that it will be reflected? Not 0!

Two steps: The potential barrier and tunneling. Initial condition: free particles moving from left to right. When When  Tunneling Solution: Solution: Inc. Refl. Inc. Refl. Trans. Trans. Apply normalization and wave function smoothness

Two steps: The potential barrier and tunneling. When When  Tunneling Results: Results: Resonant transmission. Thin film optics analogy.

Tunneling through a wide barrier Transmission probability is very sensitive to barrier width L and the energy E. This leads to some wonderful applications of QM. How sensitive? An electron encounters a barrier of 5.0 eV with a width of 1.6 nm. What is the transmission probability when the electron is (a) 2.0 eV and (b) 3.0 eV? When E = 2.0 eV When E = 3.0 eV 50% energy increase leads to 150 times more transmission!

Real-life examples: Alpha decay and other applications. Who took my cheese? Who took the energy from my alphas?

The Tunnel Diode Invented in 1957 by Leo Esaki (Nobel prize in 1973) et al., a tunnel diode is also called an Esaki diode. First manufactured by Sony in 1957, tunnel diodes are still produced in small volume today and used in frequency converters and detectors, and sometimes in oscillators and amplifiers as well. A tunnel diode is made by highly doped p and n areas that form a very thin (~10 nm) depletion region. The thickness of the depletion region is controlled by external voltage, hence the probability of electrons tunneling through this barrier is also controlled. For more reading materials about this device please check: http://www.ee.sc.edu/personal/faculty/simin/ELCT563/08%20Tunnel%20Diodes.pdf http://www.jhuapl.edu/techdigest/views/pdfs/V04_N5_1965/V4_N5_1965_Munsterman.pdf I-V curve of a tunnel diode with a negative resistance region

SQUID, Field Emission and STM A SQUID, superconducting quantum interference device, is a very sensitive magnetometer based on superconducting loops that contain Josephson (1973 Nobel prize) Junctions, the tunneling of the Cooper pairs. Field electron emission is emission of electrons induced by an electrostatic field, through the tunnel effect. Scanning Tunneling Microscope. Please research on these quantum effects and their applications in sciences and technologies. They provide good topics for semester end presentations.

Self study: Section 6.4 Particle-wave propagation. Study section 6.4 and write a one page summary. We will compare the summaries in next class.

Review questions Please review the solutions to the Schrödinger equation with the step and two steps condition and make sure that you feel comfortable with the results.

Preview for the next class Text to be read: Please skim from 7.1 to 7.8. If you have difficulty in understanding the materials, see the slides by next Monday. Questions: What is the fundamental change to move the Schrödinger equation from 1-D to 3-D? What is the quantization condition for the z component of angular momentum? According to QM, can you have a visual presentation for the electron’s whereabouts in a hydrogen atom?

Homework ch6-2, due by 3/31 Problem 21 on page 224.