Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.

Slides:



Advertisements
Similar presentations
Optically polarized atoms
Advertisements

PY3P05 Lectures 7-8: Fine and hyperfine structure of hydrogen oFine structure oSpin-orbit interaction. oRelativistic kinetic energy correction oHyperfine.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 451 Quantum mechanics I Fall 2012 Dec 5, 2012 Karine Chesnel.
Quantum Mechanics Zhiguo Wang Spring, 2014.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
P460 - real H atom1 The Real Hydrogen Atom Solve SE and in first order get (independent of L): can use perturbation theory to determine: magnetic effects.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
Physics 452 Quantum mechanics II Winter 2011 Instructor: Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2011 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2011 Karine Chesnel.
QM in 3D Quantum Ch.4, Physical Systems, 24.Feb.2003 EJZ Schrödinger eqn in spherical coordinates Separation of variables (Prob.4.2 p.124) Angular equation.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
P460 - spin-orbit1 Energy Levels in Hydrogen Solve SE and in first order get (independent of L): can use perturbation theory to determine: magnetic effects.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Will the orbital energies for multielectron atoms depend on their angular momentum quantum number ℓ? (A) In the H atom, the orbital energies depend on.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2011 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
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.
Postulates Postulate 1: A physical state is represented by a wavefunction. The probablility to find the particle at within is. Postulate 2: Physical quantities.
Physics 451 Quantum mechanics I Fall 2012 Nov 5, 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 451 Quantum mechanics I Fall 2012 Nov 7, 2012 Karine Chesnel.

Monday, March 23, 2015PHYS , Spring 2014 Dr. Jaehoon Yu 1 PHYS 3313 – Section 001 Lecture #13 Monday, March 23, 2015 Dr. Jaehoon Yu Bohr Radius.
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.
Physics 361 Principles of Modern Physics Lecture 22.
Physics 451 Quantum mechanics I Fall 2012 Nov 20, 2012 Karine Chesnel.
Germano Maioli Penello Chapter 7 Magnetism in the localised electron model Presentation based on the book Magnetism: Fundamentals, Damien Gignoux & Michel.
13. Applications of Approximation Methods
Lecture 22 Spin-orbit coupling. Spin-orbit coupling Spin makes an electron act like a small magnet. An electron orbiting around the nucleus also makes.
Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel.
Physics 452 Quantum mechanics II Winter 2011 Karine Chesnel.
Quantum II (PHYS 4410) Lecture 17 Dipole-dipole hyperfine structure HWK 6 is due Wednesday at 6PM.
Chapter 4 Two-Level Systems, Spin. Two-level systems Let us start with the simplest non-trivial state space, with only two dimensions Despite its simplicity,
Postulates Postulate 1: A physical state is represented by a wavefunction. The probablility to find the particle at within is. Postulate 2: Physical quantities.

Group theory and intrinsic spin; specifically, s=1/2
Perturbation Theory Lecture 2 Books Recommended:
Stationary Perturbation Theory And Its Applications
Perturbation Theory Lecture 2 continue Books Recommended:
Spin and Magnetic Moments
Quantum mechanics I Fall 2012
Quantum mechanics II Winter 2011
QM2 Concept Test 2.1 Which one of the following pictures represents the surface of constant
Hydrogen relativistic effects II
The Real Hydrogen Atom Solve SE and in first order get (independent of L): can use perturbation theory to determine: magnetic effects (spin-orbit and hyperfine.
Quantum mechanics II Winter 2012
Quantum mechanics I Fall 2012
Chapter 4 Two-Level Systems.
Quantum mechanics II Winter 2012
Quantum mechanics II Winter 2012
QM1 Concept test 1.1 Consider an ensemble of hydrogen atoms all in the ground state. Choose all of the following statements that are correct. If you make.
Last hour: Orbit magnetism
 .
LECTURE 15.
Group theory and intrinsic spin; specifically, s=1/2
QM2 Concept Test 11.1 In a 3D Hilbert space,
“Addition” of angular momenta – Chap. 15
QM2 Concept Test 10.1 Consider the Hamiltonian
Quantum mechanics II Winter 2012
Presentation transcript:

Physics 452 Quantum mechanics II Winter 2012 Karine Chesnel

Homework Phys 452 Tuesday Jan 24: Homework # 5 Pb: 6.12, 6.13, 6.14 & 6.33 Thursday Jan 26: Homework # 6

Degenerate perturbation theory Phys 452 General method Start with an ortho-normal basis of the unperturbed states If the state is degenerate: build Diagonalize W : the eigenvalues are If the state is non-degenerate:

Phys 452 Application: The fine structure of hydrogen Motion of the electron Coulomb interaction between e - and nucleus Bohr’s energies where Bohr radius

Phys 452 The fine structure of hydrogen Spherical harmonics

Phys 452 The fine structure of hydrogen Fine structure + Lamb shift + Sources of perturbation: Hyperfine splitting + +… Bohr’s energy E = where fine structure constant

Phys 452 Quiz 6a How small is the fine structure correction compared to the Bohr’s energies ? A. Same order of magnitude B. Factorsmaller C. Factorsmaller D. Factorsmaller E. Factorsmaller

Phys 452 The fine structure of hydrogen Bohr’s energy Fine structure Lamb shift Hyperfine splitting Relativistic correction Spin- orbit coupling

Phys 452 The fine structure of hydrogen Relativistic correction What is the relativistic correction to the Hamiltonian? Momentum Kinetic energy

Phys 452 The fine structure of hydrogen Relativistic correction The first-order correction to the Bohr’s energy will be: Developing H’ in terms of p Pb 6.14 Application to harmonic oscillator

Phys 452 The fine structure of hydrogen Relativistic correction The first order correction to the Bohr’s energy is:

Phys 452 The fine structure of hydrogen Relativistic correction Expectation values Pb 6.12Pb 6.33 Pb 6.13 For example (1s) Introducing the azimuthal quantum number

Phys 452 Quiz 6b Give an estimate of the relativistic correction for the ground level of hydrogen ? A. B. C. D. E.

Phys 452 Quiz 6c Does the relativistic correction lift the degeneracy of the atomic levels ? A. Not at all B.Yes, partially C.Yes, completely D. It depends on the speed of the electron E. It depends on external fields

Phys 452 Quiz 6d What is the relativistic correction for the band (3d)? A. B. C. D. E.