Quantum mechanics I Fall 2012

Slides:



Advertisements
Similar presentations
Physical Chemistry 2nd Edition
Advertisements

Quantum One: Lecture 5a. Normalization Conditions for Free Particle Eigenstates.
Physics 451 Quantum mechanics I Fall 2012 Dec 5, 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Chapter 3 Formalism. Hilbert Space Two kinds of mathematical constructs - wavefunctions (representing the system) - operators (representing observables)
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Quantum Mechanics(14/2)Taehwang Son Functions as vectors  In order to deal with in more complex problems, we need to introduce linear algebra. Wave function.
Physics 3 for Electrical Engineering
Physics 451 Quantum mechanics I Fall 2012 Sep 10, 2012 Karine Chesnel.
Chap 3. Formalism Hilbert Space Observables
Physics 451 Quantum mechanics I Fall 2012 Nov 12, 2012 Karine Chesnel.
Physics 451 Quantum mechanics I Fall 2012 Oct 17, 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 451 Quantum mechanics I Fall 2012 Oct 8, 2012 Karine Chesnel.
Formalism of Quantum Mechanics 2006 Quantum MechanicsProf. Y. F. Chen Formalism of Quantum Mechanics.

Physics 451 Quantum mechanics I Fall 2012 Sep 12, 2012 Karine Chesnel.
1 The Mathematics of Quantum Mechanics 3. State vector, Orthogonality, and Scalar Product.

5. Quantum Theory 5.0. Wave Mechanics

Mathematical Tools of Quantum Mechanics
Chapter 5: Quantum Mechanics
Physics 451 Quantum mechanics I Fall 2012 Oct 5, 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
2. Time Independent Schrodinger Equation
Physics 451 Quantum mechanics I Fall 2012 Oct 8, 2012 Karine Chesnel.

Physics 451 Quantum mechanics I Fall 2012 Oct 12, 2012 Karine Chesnel.
Lecture from Quantum Mechanics. "The most beautiful experience we can have is the mysterious. It is the fundamental emotion which stands at the cradle.
Quantum Two 1. 2 Angular Momentum and Rotations 3.
Q. M. Particle Superposition of Momentum Eigenstates Partially localized Wave Packet Photon – Electron Photon wave packet description of light same.
PHY 741 Quantum Mechanics 12-12:50 PM MWF Olin 103 Plan for Lecture 1:
Formalism Chapter 3.
Concept test 15.1 Suppose at time
Quantum mechanics I Fall 2012
Warm Up.
Quantum mechanics I Fall 2012
Quantum One.
Schrodinger Equation The equation describing the evolution of Ψ(x,t) is the Schrodinger equation Given suitable initial conditions (Ψ(x,0)) Schrodinger’s.
4. The Postulates of Quantum Mechanics 4A. Revisiting Representations
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Quantum One.
Quantum mechanics I Fall 2012
Quantum mechanics II Winter 2011
Concept test 15.1 Suppose at time
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Molecular Structure & Energy Levels
Quantum mechanics II Winter 2012
Quantum mechanics II Winter 2011
Quantum mechanics I Fall 2012
Lecture 7 SMES2201 Semester 1 (2009/2010)
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Quantum mechanics I Fall 2012
Last hour: If every element of state space can be expanded in one (and only one) way in terms of a set of countable, orthonormal functions uj , we call.
Quantum mechanics II Winter 2012
Quantum mechanics I Fall 2012
Shrödinger Equation.
PHY 741 Quantum Mechanics 12-12:50 PM MWF Olin 103
Homework Week of January 7th UNIT TEST TODAY! Monday Tuesday Wednesday
Quantum mechanics I Fall 2012
Linear Vector Space and Matrix Mechanics
Other examples of one-dimensional motion
Warm-ups Week of October 7-11, 2013.
Quantum mechanics I Fall 2012
Presentation transcript:

Quantum mechanics I Fall 2012 Physics 451 Quantum mechanics I Fall 2012 Oct 15, 2012 Karine Chesnel

Practice test: Monday Oct 22 Quantum mechanics Announcements Homework this week: HW # 13 due Tuesday Oct 16 Pb 3.3, 3.5, A18, A19, A23, A25 HW #14 due Thursday Oct 18 Pb 3.7, 3.9, 3.10, 3.11, A26 Review: Friday Oct 19 Practice test: Monday Oct 22 Test 2 preparation

Eigenvalues of an Hermitian operator Quantum mechanics Eigenvalues of an Hermitian operator Finite space Generalization of Determinate state: operator eigenstate eigenvalue Hermitian operator: 1. The eigenvalues are real 2. The eigenvectors corresponding to distinct eigenvalues are orthogonal 3. The eigenvectors span the space

Eigenvalues of a Hermitian operator Quantum mechanics Eigenvalues of a Hermitian operator Infinite space Two cases Discrete spectrum of eigenvalues: Eigenfunctions in Hilbert space Continuous spectrum of eigenvalues: Eigenfunctions NOT in Hilbert space

In which categories fall the following potentials? Quantum mechanics Quiz 17 In which categories fall the following potentials? 1. Harmonic oscillator Discrete spectrum Continuous spectrum Could have both 2. Free particle 3. Infinite square well 4. Finite square well

Discrete spectra of eigenvalues Quantum mechanics Discrete spectra of eigenvalues Theorem 1: the eigenvalues are real Theorem 2: the eigenfunctions of distinct eigenvalues are orthogonal Axiom 3: the eigenvectors of a Hermitian operator are complete

Orthogonalization procedure Quantum mechanics Degenerate states More than one eigenstate for the same eigenvalue Gram-Schmidt Orthogonalization procedure See problem A4

Continuous spectra of eigenvalues Quantum mechanics Continuous spectra of eigenvalues No proof of theorem 1 and 2… but intuition for: Eigenvalues being real Orthogonality between eigenstates Compliteness of the eigenstates

Continuous spectra of eigenvalues Quantum mechanics Continuous spectra of eigenvalues Momentum operator: For real eigenvalue p: Dirac orthonormality Eigenfunctions are complete Wave length – momentum: de Broglie formulae

Continuous spectra of eigenvalues Quantum mechanics Continuous spectra of eigenvalues Position operator: - Eigenvalue must be real Dirac orthonormality Eigenfunctions are complete