Spin and the Exclusion Principle Modern Ch. 7, Physical Systems, 20

Slides:



Advertisements
Similar presentations
Cutnell/Johnson Physics 7 th edition Classroom Response System Questions Chapter 40 All about Atoms Reading Quiz Questions.
Advertisements

Start EM Ch.5: Magnetostatics finish Modern Physics Ch.7: J=L+S Methods of Math. Physics, Thus. 24 Feb. 2011, E.J. Zita Magnetostatics: Lorentz Force and.
© 2010 Pearson Education, Inc. PowerPoint ® Lectures for College Physics: A Strategic Approach, Second Edition Chapter 29 Atoms and Molecules.
Chap 12 Quantum Theory: techniques and applications Objectives: Solve the Schrödinger equation for: Translational motion (Particle in a box) Vibrational.
EXAM #3 HAS BEEN MOVED TO MONDAY, NOVEMBER 9 TH Bring a Periodic Table to class this week November 2, 2009.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
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.
Modern physics and Quantum Mechanics Physical Systems, 8 Mar.2007 EJZ More angular momentum and H atom Compare to Bohr atom Applications: Bohr magneton,
Spin Quantum Number and Spin Example: Electron, s = ½ (fermion) Implications? Spin angular momentum is INTRINSIC to a particle mass charge spin More 
1 8.1Atomic Structure and the Periodic Table 8.2Total Angular Momentum 8.3Anomalous Zeeman Effect Atomic Physics CHAPTER 8 Atomic Physics What distinguished.
Quantum Ch.4 - continued Physical Systems, 27.Feb.2003 EJZ Recall solution to Schrödinger eqn in spherical coordinates with Coulomb potential (H atom)
Lecture 2210/26/05. Moving between energy levels.
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
1AMQ P.H. Regan & W.N.Catford 1 1AMQ, Part III The Hydrogen Atom 5 Lectures n Spectral Series for the Hydrogen Atom. n Bohr’s theory of Hydrogen. n The.
Periodic Table. Quantum Numbers  The Bohr model of hydrogen provided a single quantum number n. Principal quantum numberPrincipal quantum number One-dimensional.
Spin-Orbit Effect In addition to its motion about the nucleus, an electron also has an intrinsic angular momentum called “spin” similar to the earth moving.
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.
Chapter 41 Atomic Structure.
Spectral Line Physics Atomic Structure and Energy Levels Atomic Transition Rates Molecular Structure and Transitions 1.
Lecture VI Many - electron atoms dr hab. Ewa Popko.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 31 Physics, 4 th Edition James S. Walker.
Chapter 41 Atomic Structure
1 Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Quantum Theory and the Electronic Structure of.
Quantum Physics Study Questions PHYS 252 Dr. Varriano.
Atomic Orbitals, Electron Configurations, and Atomic Spectra
PHY206: Atomic Spectra  Lecturer: Dr Stathes Paganis  Office: D29, Hicks Building  Phone: 
29 Atoms and Molecules Slide 29-2.
Vector coupling of angular momentum. Total Angular Momentum L, L z, S, S z J and J z are quantized Orbital angular momentumSpin angular momentum Total.
1 My Chapter 28 Lecture. 2 Chapter 28: Quantum Physics Wave-Particle Duality Matter Waves The Electron Microscope The Heisenberg Uncertainty Principle.
Spin and Atomic Physics 1. HW 8, problem Quiz Topics in this chapter:  The spin and the Stern-Gerlach experiment.  Fermion, Boson and.
ATOMIC PHYSICS Dr. Anilkumar R. Kopplkar Associate Professor
Phys 102 – Lecture 26 The quantum numbers and spin.
MULTIELECTRON ATOMS l ELECTRON SPIN: Electron has intrinsic angular momentum - “spin”; it behaves as if it were “spinning”, i.e. rotating around its axis.
Baby-Quiz 1.If all objects emit radiation, why don’t we see most of them in the dark? 2.Suppose you were a nineteenth-century scientist who had just discovered.
An Electron Trapped in A Potential Well Probability densities for an infinite well Solve Schrödinger equation outside the well.
Quantum Chemistry Chapter 6. Copyright © Houghton Mifflin Company. All rights reserved.6 | 2 Electromagnetic Radiation.
Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Electromagnetic Radiation Radiant energy that exhibits wavelength-like behavior and.
Chapter 10 Atomic Structure and Atomic Spectra. Spectra of complex atoms Energy levels not solely given by energies of orbitals Electrons interact and.
Quantum Theory and the Electronic Structure of Atoms Chapter 7.
Quantum Theory and the Electronic Structure of Atoms Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
The Bohr Model of the Atom. The behavior of electrons in atoms is revealed by the light given off when the electrons are “excited” (made to absorb energy).
Quantum Theory the modern atomic model. Bohr Model of the Atom a quantum model proposed by Niels Bohr in 1913 It helped to explain why the atomic emission.
Chapter 35 Quantum Mechanics of Atoms. S-equation for H atom 2 Schrödinger equation for hydrogen atom: Separate variables:
Ch4 Fine structure of atoms Magnetic moments Spin of the electron Stern-Gerlach experiment Spectrum of the alkali atoms Spin-orbit coupling (interaction)
Quantum Theory and the Electronic Structure of Atoms Chapter 6.
Atomic Structure and Periodicity. Atoms ProtonsNeutronsElectrons 1. Where are the electrons 2. Do they have different energies.
Chapter 28:Atomic Physics
Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2.
Quantum Theory and the Electronic Structure of Atoms Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Atomic Structure and Atomic Spectra
Unit 12: Part 2 Quantum Physics. Overview Quantization: Planck’s Hypothesis Quanta of Light: Photons and the Photoelectric Effect Quantum “Particles”:
Total Angular Momentum L, L z, S, S z J and J z are quantized Orbital angular momentumSpin angular momentum Total angular momentum.
Atomic Physics Quantum Physics 2002 Recommended Reading: Harris Chapter 7.
Physics 1202: Lecture 34 Today’s Agenda Announcements: Extra creditsExtra credits –Final-like problems –Team in class –Teams 5 & 6 HW 10 due FridayHW 10.
Chapter 40 All About Atoms In this chapter we continue with a primary goal of physics―discovering and understanding the properties of atoms. 100 years.
Absorption & Emission Spectra. Emission Spectrum Hot, glowing objects emit a continuous spectrum of light  temperature. Fill a tube a glass tube with.
Chapter 40 All About Atoms. 40.2: Some Properties of Atoms: Atoms are stable. Essentially all the atoms that form our tangible world have existed without.
Hydrogen atom energy levels deBroglie and Bohr: 1. Wavelength comes from speed: 2. Integer wavelengths fit in orbit of size r 3. F = ma:
Lecture Outline Chapter 31 Physics, 4th Edition James S. Walker
Chapter 41 Atomic Structure
Arrangement of Electrons in Atoms
Atomic Theory.
Hydrogen Revisited.
Spin PHY
Lasers and effects of magnetic field
Chapter 7 Atomic Physics.
Particles and Waves.
Quantum Mechanical View of Atoms
Chapter 41 Atomic Structure
Physics 3313 – Review 2 Wednesday May 5, 2010 Dr. Andrew Brandt
Presentation transcript:

Spin and the Exclusion Principle Modern Ch. 7, Physical Systems, 20 Spin and the Exclusion Principle Modern Ch.7, Physical Systems, 20.Feb.2003 EJZ Review Hydrogen atom, orbital angular momentum L Electron spin s Total angular momentum J = S + L= Spin + orbit Applications: 21 cm line, Zeeman effect Good QN and allowed transitions Pauli exclusion principle Periodic Table Lasers

Hydrogen atom : Bohr model We found rn = n2 r1, En = E1/n2, where the “principle quantum number” n labels the allowed energy levels. Discrete orbits match observed energy spectrum

Hydrogen atom: Orbits are not discrete (notice different r scales)

Hydrogen atom: Schrödinger solutions depend on new angular momentum quantum numbers Quantization of angular momentum direction for l=2 Magnetic field splits l level in (2l+1) values of ml = 0, ±1, ± 2, … ± l

Hydrogen atom examples from Giancoli

Hydrogen atom plus L+S coupling: Hydrogen atom so far: 3D spherical solution to Schrödinger equation yields 3 new quantum numbers: l = orbital quantum number ml = magnetic quantum number = 0, ±1, ±2, …, ±l ms = spin = ±1/2 Next step toward refining the H-atom model: Spin with Total angular momentum J=L+s with j=l+s, l+s-1, …, |l-s|

Total angular momentum: Multi-electron atoms: J = S+L where S = vector sum of spins, L = vector sum of angular momenta Spectroscopic notation: L=0 1 2 3 S P D F Allowed transitions (emitting or absorbing a photon of spin 1) ΔJ = 0, ±1 (not J=0 to J=0) ΔL = 0, ±1 Δmj = 0, ±1 (not 0 to 0 if ΔJ=0) ΔS = 0 Δl = ±1

Discuss state labels and allowed transitions for sodium

Magnetic moment of electron Magnetic moment: Bohr magneton models e- as spinning ball (or loop) of charge We expect but Stern-Gerlach experiment shows that where g = 2.0023…=gyromagnetic ratio (electron is not quite a spinning ball of charge).

Application of Zeeman effect: 21-cm line Electron feels magnetic field due to proton magnetic moment (hyperfine splitting).

Pauli Exclusion principle Identical fermions have antisymmetric wavefunctions, so electrons cannot share the same energy state. Fill energy levels in up-down pairs: 1s 2s 2p 3s 3p 3d 4s 4p 4d 4f …

LASER = Light Amplification by Stimulated Emission of Radiation Pump electrons up into metastable excited state. One transition down stimulates cascade of emissions. Monochromatic: all photons have same wavelength Coherent: in phase, therefore intensity ~ N2