Physics 717
Graduate Quantum Mechanics I
Fall 2004
Instructor:
Lev Kaplan
Lectures:
MWF 10:00 - 10:50, in room ***
Textbooks:
Dirac, Principles of Quantum Mechanics, 4th edition
Messiah, Quantum Mechanics
Possibly
useful reference books: Sakurai, Modern Quantum Mechanics (especially
early chapters)
Cohen-Tannoudji et al., Quantum Mechanics (complete treatment)
Landau et al., Quantum Mechanics
Merzbacher, Quantum Mechanics
(traditional "standard" text)
Shankar, Principles of Quantum Mechanics
(introductory level)
Ballentine, Quantum Mechanics: A Modern Development (conceptual)
Office:
5046 Percival Stern Hall
Office
hours: to be arranged after first class meeting, or by appointment
Email:
lkaplan@tulane.edu [A great way to ask a question or arrange an appointment]
Telephone:
504-862-3176 (x3176) [Please leave a message if I’m not there or try email]
Welcome to Graduate Quantum
Mechanics I at Tulane University!
General
Course Objectives and Requirements:
This course, part one of a two-semester
sequence, is intended to help you master the basic principles and mathematical
formalism of quantum mechanics at the introductory graduate level. The emphasis
will be on fundamentals and general structure of the theory rather than on
detailed applications, with specific examples used primarily to illustrate the
general development. Although the course is self-contained, a solid background
in quantum mechanics at the undergraduate level is strongly recommended. The
required mathematical tools (e.g., linear algebra) will be introduced as
needed. While some formal aspects of quantum mechanics will be emphasized, the
focus will be on the physics rather than on mathematical rigor. Topics covered
will include states and operators, measurement theory, n-level and 2-level
systems, representations, unitary transformations, Schrodinger and Heisenberg
pictures, quantum statistical mechanics, angular momentum, time-independent and
time-dependent perturbation theory, and many-particle systems. The classical
limit of quantum mechanics will be discussed where appropriate.
Grading:
Homework: 30%
Midterm
exam: 30%
Comprehensive
final exam: 40%
Homework:
Homework will be assigned every one or two
weeks. The assignments may include derivations and examples that extend the
class discussion.
Examinations:
One midterm and a comprehensive final exam will
compose 70% of your final grade. The date of the midterm is subject to very
minor adjustment, but the date of the comprehensive final exam is set by the
university. Each exam may contain a combination of definition/conceptual
questions (short-answer), derivations, and calculations. Exam problems and
questions will be drawn from material covered in class as well as from homework
problems. More information will be provided prior to the date of each exam.
Tentative
Course Schedule:
This
schedule is subject to likely adjustments, which will be announced in class.
Brief
introduction/history (Messiah I, II)
Failures of classical mechanics, old
quantum theory
Wave mechanics and matrix mechanics
Quantum
"kinematics" (Messiah VII)
States and vectors, complex vector space
structure, superposition principle
Kets and bras, scalar product,
norms, overlaps, probabilities
Linearly dependent and independent
states, complete orthonormal sets
N-state systems, connection with
matrix mechanics
Example: 2-state systems
("qubits")
Tensor products
Operators
and observables (Messiah V, VII, VIII)
Linear operators, adjoint, self-adjoint,
matrices, projection operators
Eigenvalues and eigenstates,
definition of observable, completeness relation
Discrete and continuous spectra,
normalization, delta function, normalizability
Functions of observables
Example: particle in one or
dimensions
Expectation value and fluctuations
Example: 2-state systems (spin 1/2),
Pauli matrices
Representations
and unitary transformations (Messiah VII, VIII, V)
Example: position representation
Change of representation, unitary
operators, effect on states and observables, norm conservation
Spin 1/2 systems
Momentum representation and wave
functions, commutation relations, Fourier transforms
Uncertainty
principle and displacement operators (Messiah IV, V, VII, VIII)
Commutation relations and uncertainty,
position and momentum
Infinitesimal transformations,
translations, generators, finite displacement operators
Complete sets of commuting
observables
Time
evolution ("dynamics") (Messiah VIII, VI)
Hamiltonian operator as generator,
Schrodinger equation
Stationary states, stationary state
basis
Finite time evolution and time
ordering
Schrodinger, Heisenberg,
intermediate pictures
Ehrenfest theorem and classical
limit
Quantum commutators and classical
Poisson brackets
Analogy with classical Hamilton's
equations, canonical quantization
Constants of motion and symmetries
Example:
particle in one or more dimensions
Gaussian wave packets
Energy-time uncertainty relation
Mixed
states and statistical mechanics (Messiah VIII)
Pure and mixed states, density operator,
traces, expectation values, entropy
Example: matrix mechanics
Time evolution of density operator
Thermal equilibrium and partition
function
Example:
Harmonic oscillator (Messiah XII)
Creation and annihilation operators,
number operator, spectrum, expectation values
Thermal equilibrium
Position representation: wave
functions
Wave packets and semiclassical
description
Multi-dimensional or coupled
harmonic oscillators
Example:
angular momentum (Messiah XIII)
Rotations, commutation relations
Eigenstates of angular momentum
Special case: spin 1/2
Perturbation
theory: time independent (Messiah XVI)
Degenerate perturbation theory
Perturbation
theory: time dependent (Messiah XVII)
About
me:
I am a first-year Assistant Professor at Tulane, and prior to coming here I did research at the University of Washington in Seattle. I was born in Latvia (former USSR), went to school in New Jersey, did my undergraduate studies at the University of Pennsylvania, and my graduate “work” at Harvard University (on the theory of high-energy particles). My present research interests include something called “quantum chaos.” If you want to know what that means, just ask. I strongly encourage you to stop by my office to talk about physics, Tulane, questions, concerns, suggestions, or anything else that may be on your mind.