Physics 451 Quantum mechanics I Fall 2012 Sep 12, 2012 Karine Chesnel.

Slides:



Advertisements
Similar presentations
The Infinite Square Well Now we are ready to solve the time independent Schrödinger equation (TISE) to get ψ(x) and E. (Recall Ψ(x,t) = ψ(x)e −i2  Et/h.
Advertisements

Physics 451 Quantum mechanics I Fall 2012 Dec 5, 2012 Karine Chesnel.
Quantum One: Lecture 3. Implications of Schrödinger's Wave Mechanics for Conservative Systems.
Review Three Pictures of Quantum Mechanics Simple Case: Hamiltonian is independent of time 1. Schrödinger Picture: Operators are independent of time; state.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Modern Physics 6a – Intro to Quantum Mechanics Physical Systems, Thursday 15 Feb. 2007, EJZ Plan for our last four weeks: week 6 (today), Ch.6.1-3: Schrödinger.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
LECTURE 16 THE SCHRÖDINGER EQUATION. GUESSING THE SE.
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.
Ch 9 pages ; Lecture 21 – Schrodinger’s equation.
Physics 451 Quantum mechanics I Fall 2012 Sep 10, 2012 Karine Chesnel.
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.
Bound States 1. A quick review on the chapters 2 to Quiz Topics in Bound States:  The Schrödinger equation.  Stationary States.  Physical.
Physics 451 Quantum mechanics I Fall 2012 Oct 17, 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Ch 9 pages Lecture 22 – Harmonic oscillator.
Physics 451 Quantum mechanics I Fall 2012 Nov 5, 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Wednesday, Oct. 30, 2013PHYS , Fall 2013 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #14 Wednesday, Oct. 30, 2013 Dr. Jaehoon Yu Infinite.
Physics 451 Quantum mechanics I Fall 2012 Nov 7, 2012 Karine Chesnel.
(1) Experimental evidence shows the particles of microscopic systems moves according to the laws of wave motion, and not according to the Newton laws of.
Wednesday, Oct. 17, 2012PHYS , Fall 2012 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #13 Wednesday, Oct. 17, 2012 Dr. Jaehoon Yu Properties.


Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 451 Quantum mechanics I Fall 2012 Karine Chesnel.
PHYS 3313 – Section 001 Lecture #18

Chapter 5: Quantum Mechanics
Physics 451 Quantum mechanics I Fall 2012 Oct 5, 2012 Karine Chesnel.
Monday, Nov. 4, 2013PHYS , Fall 2013 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #15 Monday, Nov. 4, 2013 Dr. Jaehoon Yu Finite Potential.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2011 Karine Chesnel.
2. Time Independent Schrodinger Equation

Physics 451 Quantum mechanics I Fall 2012 Sep 7, 2012 Karine Chesnel.
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.
量子力學導論 Chap 1 - The Wave Function Chap 2 - The Time-independent Schrödinger Equation Chap 3 - Formalism in Hilbert Space Chap 4 - 表象理論.

Principles of Quantum Mechanics P1) Energy is quantized The photoelectric effect Energy quanta E = h  where h = J-s.
Review for Exam 2 The Schrodinger Eqn.
Physics 451 Quantum mechanics I Fall 2012 Oct 12, 2012 Karine Chesnel.
CHAPTER 5 The Schrodinger Eqn.
Concept test 15.1 Suppose at time
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:
CHAPTER 5 The Schrodinger Eqn.
+2 or 3 more presentatios. +2 or 3 more presentatios.
Quantum mechanics I Fall 2012
CHAPTER 5 The Schrodinger Eqn.
CHAPTER 5 The Schrodinger Eqn.
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Quantum mechanics II Winter 2011
Concept test 15.1 Suppose at time
Quantum mechanics I Fall 2012
Quantum mechanics II Winter 2012
Quantum mechanics II Winter 2011
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Shrödinger Equation.
Concept test 14.1 Is the function graph d below a possible wavefunction for an electron in a 1-D infinite square well between
Quantum mechanics I Fall 2012
Other examples of one-dimensional motion
Source: D. Griffiths, Introduction to Quantum Mechanics (Prentice Hall, 2004) R. Scherrer, Quantum Mechanics An Accessible Introduction (Pearson Int’l.
Quantum mechanics I Fall 2012
PHYS 3313 – Section 001 Lecture #20
Presentation transcript:

Physics 451 Quantum mechanics I Fall 2012 Sep 12, 2012 Karine Chesnel

Homework remaining this week: Extended Friday Sep 14 by 7pm: HW # 5 Pb 2.4, 2.5, 2.7, 2.8 Announcements Quantum mechanics Note: Penalty on late homework: - 2pts per day Credit for group presentations: Homework 2: 20 points Quiz 5: 5 points

No student assigned to the following transmitters: Announcements Quantum mechanics Please register your i-clicker at the class website! 2214B68 17A E5C6E2C 1E71A9C6

Quantum mechanicsCh 2.1 Time-independent Schrödinger equation Solution  (x) depends on the potential function V(x). Space dependent part: Stationary state Associated to energy E

Quantum mechanicsCh 2.1 Stationary states Properties: Expectation values are not changing in time (“stationary”): with is independent of time The expectation value for the momentum is always zero In a stationary state! (Side note: does not mean that and are zero!)

Quantum mechanicsCh 2.1 Stationary states Properties: Hamiltonian operator - energy

Quantum mechanicsCh 2.1 Stationary states General solution where Associated expectation value for energy

Quiz 6a A. B. C. one of the values D. Quantum mechanics A particle, is in a combination of stationary states: What will we get if we measure its energy?

Quiz 6b A.0 B. C. D. E. Quantum mechanics A particle, is in a combination of stationary states: What is the probability of measuring the energy E n ?

Quantum mechanicsCh 2.2 Time-independent potential Expectation value for the energy:

Quantum mechanicsCh 2.2 Infinite square well x 0a The particle can only exist in this region V(x)=0 for 0<x<a V=∞ else Shape of the wave function?

Quantum mechanicsCh 2.2 Infinite square well Solutions to Schrödinger equation: Simple harmonic oscillator differential equation with

Quantum mechanicsCh 2.2 Infinite square well Solutions to Schrödinger equation: Boundary conditions: At x=0: At x=a: with

Quantum mechanicsCh 2.2 Infinite square well Possible states and energy values: Quantization of the energy Each state  n is associated to an energy E n

Quantum mechanicsCh 2.2 Infinite square well Properties of the wave functions  n : x 0a 1.They are alternatively even and odd around the center 2. Each successive state has one more node Ground state Excited states 3. They are orthonormal 4. Each state evolves in time with the factor

Quantum mechanicsCh 2.2 Infinite square well Pb 2.4 Particle in one stationary state Pb 2.5 Particle in a combination of two stationary states evolution in time? oscillates in time expressed in terms of E 1 and E 2

Quantum mechanicsCh 2.2 Infinite square well Expectation value for the energy: The probability that a measurement yields to the value E n is Normalization