Physics 404 - Quantum Physics III -
Spring 2002
Welcome to the Physics 404 WWW pages!
The motivation for this course is to teach some fundamental aspects of quantum
mechanics and, in particular, to illustrate their relevance and applications to
major areas of physics including condensed matter, optical, molecular, nuclear, and
particle physics.
- Instructors:
D.S. Armstrong,
W.E. Cooke ,
G.L. Hoatson,
K.A. Griffioen,
- Organization: G.L. Hoatson Small 213, x13517,
gina@physics.wm.edu
- Mon., Wed., Fri., 11:00
- 11:50 am (or by negotiation) , Small Hall 152
- Prerequistes: Phys 313 &
Phys 314
A syllabus is given
below:
Photon Physics (Cooke)
[Jan. 16- Feb. 6]
Although the concept of a photon – a quantized unit of electromagnetic
energy – was crucial for the creation of quantum mechanics, we have often
relegated it to a minor role simply explaining the photo-electric effect. This section of PHYS 404 will begin by laying a formal
foundation for second quantization, which quantizes electromagnetic fields to
produce photons. From there, we
will show how the photon itself simplifies a wide variety of calculations that drive
current optical research.
- Second Quantization:
Quantizing the electromagnetic vector potential introduces creation and
annihilation operators.
- Relativistic Photons:
The particle nature of a photon makes it easy to transform electromagnetic
fields.
- Lasers:
Stimulated emission is a fundamental quantum effect that leads to optical
gain.
- Photon Interactions:
The concept of a photon cross-section is surprisingly general and
extremely useful.
- Cooling and Trapping with
photons:
One of the most active areas of atomic physics uses laser to cool and trap
atoms. We will discuss some
of the clever mechanisms, such as Doppler cooling and Sisyphus cooling,
and some of the best current traps (e.g. the MOT).
- Nonlinear Optics:
Conservation rules for photon energy and momenta easily explain most nonlinear
optical phenomena.
Spectroscopy and NMR (Hoatson)
[Feb. 8 - Mar. 1]
Spectroscopy refers to the interaction of electromagnetic
radiation with matter, and provides many beautiful examples of quantum
mechanical principles. Quantized (bound) states are obtained by solving the
time-independent Schrödinger equation in absence of radiation, and the
probability of radiation-induced transitions among these states is obtained by
solving the time dependent Schroödinger equation. Statistical mechanics
is needed to extend this formalism to the interaction of radiation with
condensed matter, and to account for effects of phase coherent radiation. This
series of lectures will develop these principles and illustrate them with
specific examples taken from Nuclear Magnetic Resonance (NMR). NMR provides
particularly clear examples of the general quantum mechanical formalism, and
the results indicate how useful information about condensed matter systems can
be obtained. Topics to be covered include:
- General Spectroscopy:
Regions of the electromagnetic spectrum and the physical phenomena
responsible for spectroscopy. Classification of bound states, stimulated
and spontaneous emission.
- Quantum Mechanics of
Angular Momentum:
Matrix representation of angular momentum operators, commutation
relations, exponential operators and rotations in Hilbert space.
- Time Independent
Schrödinger Equation:
Hamiltonian operator, eigenvalues (energies) and eigenfunctions (state
vectors) for nuclear spins interacting with each other and with a static
magnetic field. Exact solution of the appropriate Schrödinger
equation will be obtained and compared with results of perturbation
theory.
- Density Matrix Theory:
Wavefunction expansion coefficients and how they relate to observables.
Ensemble averages, eigenstate populations, and coherent superpositions of
eigenstates. Illustrative examples include ensembles of spin 1/2 and spin
1 particles.
- Time Evolution:
Phase coherence, the free induction decay signal and the NMR spectrum.
Spin echoes and analogies with optical quantum beats and photon echoes.
- Multiple Quantum
Coherence:
How to measure "forbidden" multiple quantum phase coherence, and
why this is useful. Effective Hamiltonian operators, indirect detection
and two dimensional Fourier transformation.
Nuclear Physics (Griffioen)
[Mar. 11 - Apr. 3]
- The Deuteron:
- Nuclear Shell Model:
- Nuclear alpha-decay:
phenomenology, barrier tunneling, WKB approximation.
Particle Physics (Armstrong)
[Apr. 5 - Apr. 26]
Particle physics is the
study of the fundamental particles in nature and their interactions.
Elementary particles are
intrinisically quantum-mechanical objects, and so they exhibit many properties
that can only be understood via quantum
mechanics. We will study a selected number of these phenomena that highlight
various features of quantum mechanics, including interference and superposition,
field quantization, and new symmetries, and we will
introduce some areas of current research.
- Introduction to Particle
Physics:
Fundamental Forces, the classification of particles (fermions, bosons,
leptons, hadrons, baryons, mesons, etc.)
- Fundamental Symmetries and
new Quantum Numbers:
Noether's theorem, parity, isospin, flavor, color, time-reversal, etc.
- Survey of Elementary
Particle Dynamics
- Scattering and Partial
Wave Analysis:
- Hadron Spectroscopy and the
Quark Model:
angular momentum coupling, selection rules, 'exotic' particles,
charmonium, etc.
- The neutral Kaon system:
interferences, basis states, CP violation, CPT.
College of William and Mary,
Dept. of Physics
armd@physics.wm.edu
last updated: Jan. 7 2002