PHY 741 Quantum Mechanics 12-12:50 AM MWF Olin 103

Slides:



Advertisements
Similar presentations
PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
Advertisements

PHYS Quantum Mechanics PHYS Quantum Mechanics Dr Jon Billowes Nuclear Physics Group (Schuster Building, room 4.10)
Physics 451 Quantum mechanics I Fall 2012 Nov 12, 2012 Karine Chesnel.
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.
Phys 102 – Lecture 26 The quantum numbers and spin.
1. ALL POSSIBLE BASIC PARTICLES 2 Vector Electron and Positron 3.
MULTIELECTRON ATOMS l ELECTRON SPIN: Electron has intrinsic angular momentum - “spin”; it behaves as if it were “spinning”, i.e. rotating around its axis.
Germano Maioli Penello Chapter 7 Magnetism in the localised electron model Presentation based on the book Magnetism: Fundamentals, Damien Gignoux & Michel.
Atomic Orbitals And Quantum Numbers. Quantum Numbers A series of 4 numbers (and/or letters) that specify the properties of an electron in its orbit The.
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.
8/28/2015PHY 711 Fall Lecture 21 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 2: 1. Brief comment.
02/13/2015PHY 712 Spring Lecture 131 PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 13: Continue reading Chapter 5 1.Hyperfine.
PHY 711 Classical Mechanics and Mathematical Methods
PHL424: Nuclear angular momentum
Group properties of atomic orbitals and crystals
Group theory and intrinsic spin; specifically, s=1/2
PHY 711 Classical Mechanics and Mathematical Methods
PHY 741 Quantum Mechanics 12-12:50 PM MWF Olin 103 Plan for Lecture 1:
7. Quantum-Mechanical View of Atoms
Magnetic Dipoles and Angular Momenta
PHY 711 Classical Mechanics and Mathematical Methods
PHY 752 Solid State Physics
PHY 711 Classical Mechanics and Mathematical Methods
PHY 711 Classical Mechanics and Mathematical Methods
Zeeman effect HFS and isotope shift
Quantum mechanics I Fall 2012
Spin PHY
Last Time… 3-dimensional quantum states and wave functions
Chapter 7 Atomic Physics.
PHY 712 Electrodynamics 11-11:50 AM MWF Olin 107 Plan for Lecture 14:
Time reversal symmetry and
More on Magnetic Moments
Electron Orbitals Heisenberg 1. The ____________ ______________ principle states that it is impossible to determine simultaneously both the position and.
Consider the He atom. The Hamiltonian is
Bound Systems and Spectra
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 25:
Welcome back from fall break Comments on mid-term exam
Chap. 20 in Shankar: The Dirac equation
PHY 752 Solid State Physics Electron Gas in Magnetic Fields
PHY 741 Quantum Mechanics 12-12:50 PM MWF Olin 103
Physics Lecture 15 Wednesday March 24, 2010 Dr. Andrew Brandt
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 14:
Chap. 17 in Shankar: Magnetic field effects – atoms, charged particles
Last hour: Orbit magnetism
PHY 752 Solid State Physics Plan for Lecture 30: Chap. 13 of GGGPP
7. Quantum-Mechanical View of Atoms
PHY 711 Classical Mechanics and Mathematical Methods
Chapter 9 -- Linear momentum Impulse and momentum in two dimensions
Group theory and intrinsic spin; specifically, s=1/2
Chap. 20 in Shankar: The Dirac equation for a hydrogen atom
Reading: Chapters #5 in Shankar; quantum mechanical systems in 1-dim
PHY 711 Classical Mechanics and Mathematical Methods
“Addition” of angular momenta – Chap. 15
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 103 Plan for Lecture 26:
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 8:
Other examples of one-dimensional motion
Introduction to groups having infinite dimension
Eigenvalues and eigenvectors of a hydrogen atom
“Addition” of angular momenta – Chap. 15
PHY 752 Solid State Physics
Addition of Angular Momentum
Physics 3313 – Review 2 Wednesday May 5, 2010 Dr. Andrew Brandt
Read Chapter # 9 in Shankar Commutator formalism and
PHY 712 Electrodynamics 9-9:50 AM MWF Olin 105 Plan for Lecture 13:
PHY 752 Solid State Physics 11-11:50 AM MWF Olin 103
Chap. 19 in Shankar: Scattering theory
Charged particle in an electrostatic field
The Quantum-Mechanical Hydrogen Atom
LECTURE 12 SPINS Source: D. Griffiths, Introduction to Quantum Mechanics (Prentice Hall, 2004) R. Scherrer, Quantum Mechanics An Accessible Introduction.
LECTURE 11 SPINS.
Presentation transcript:

PHY 741 Quantum Mechanics 12-12:50 AM MWF Olin 103 Plan for Lecture 20: Preparation for studying multi-electron atoms; notions of spin and “addition” of angular momenta – Chap. 14-15 Internal spin Spin interactions 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

10/18/2020 PHY 741 Fall 2017 -- Lecture 20

10/18/2020 PHY 741 Fall 2017 -- Lecture 20

Recall that, we analyzed the general eignstates of angular momentum, especially finding eigenvalues and eigenvectors of J2 and Jz j=integer or half integer 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

Particles can have intrinsic spin angular momentum, related to their magnetic dipole moments 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

Spin ½ systems – 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

Rotation of angular momentum 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

Response of magnetic moment to an applied magnetic field 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

10/18/2020 PHY 741 Fall 2017 -- Lecture 20

10/18/2020 PHY 741 Fall 2017 -- Lecture 20

From this result, we obtain the full solution Some details: 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

In our case -- 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

10/18/2020 PHY 741 Fall 2017 -- Lecture 20

Physical effects of intrinsic spin and orbital angular momentum: Because both are associated with magnetic fields, there is an interaction energy of the form Hyperfine interaction between nuclear spin and electronic spin and angular momentum: 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

Finding the total angular momentum – “addition” of angular momentum. In the absence of external magnetic fields, the internal magnetic dipoles cause spin interactions within each system, however, the total angular momentum of the system should be conserved. Finding the total angular momentum – “addition” of angular momentum. 10/18/2020 PHY 741 Fall 2017 -- Lecture 20

“Addition” of angular momentum 10/18/2020 PHY 741 Fall 2017 -- Lecture 20