**University**** of Maryland**

**Physics 401----Quantum Physics I----Fall 2005**

**Instructor:** Prof. Thomas Cohen (I prefer to be
addressed as Tom)

**Office: **2104 (

**Phone:** 5-6117 (Office); 301-654-7702 (Home---call before 10:00 p.m.)

**E-mail:** __cohen@umd.edu__

**TA/Grader:** Hao Li

**Office: **4223 (

**E-mail:** __lihao@.umd.edu__

**Office Hours**

Office hours are
immediately following class. I am also generally available in my office and
happy to see students; just drop by--or, better yet, give me a call and then
drop by.

**Course Philosophy**

In my opinion quantum mechanics
is, without a doubt, the most intellectually beautiful part of the
undergraduate physics curriculum and indeed one of the most beautiful in all of
physics. It is a very rich subject in terms of both the phenomena it describes
and in its formal development. The course will start by describing a few
phenomena that simply cannot be understood in terms of the classical physics of

During
the first quarter of the 20th century quantum ideas were developed to describe
such effects and we will explore these ideas including some of the rather
bizarre philosophical implications. Quantum physics at that stage was not part
of a fully systematic and consistent framework. Starting in 1925 such a
framework---quantum mechanics---was rapidly developed by Schrödinger, Heisenberg,
Dirac and others. Indeed, initially it seemed that
there were *two *such frameworks: the wave mechanics of Schrödinger,
and the matrix mechanics of Heisenberg. However, Dirac
soon developed a general treatment using abstract vector spaces and was able to
show that Schrödinger's wave mechanics and Heisenberg's matrix mechanics
were mathematically equivalent and were both special
cases of the general formulation.

The course will begin with
a historical survey of some of the outstanding problems in physics at the end
of the 19^{th} century which lead to the
development of quantum mechanics. Next , quantum
mechanics will be introduced in the framework of Schrödinger's wave
mechanics since the principal mathematical tool of this approach---a wave
equation--- is more familiar to most students. We will use this approach
initially to study one simple problem, the one dimensional infinite square
well. We will concentrate initially on understanding the basic formalism and
its implications (such as the Heisenberg uncertainty relation). .Having
built up some intuition about quantum mechanics from this example,
we will return to the formalism and develop Dirac's
approach in terms of abstract vector spaces. Then we will turn our
attention to a number of simple applications in one dimension. Additional
physically interesting applications of quantum mechanics will be treated in
Physics 402. If time permits we will return to the
formal structure of the theory.

**Books**

The main text for the
course is Griffth's *Introducton**
to Quantum Mechanics *(ISBN
0-13-111892-7)*. *The book is very readable and clear. It has a
couple of drawbacks for the purposes of this course. One principal drawback is
also its principal strength. It develops an abstract formalism for
quantum mechanics relatively early. Thus, there is a lot of mathematical
heavy lifting early in the course. Having mastered this however, the
remainder is straightforward. A second drawback to the book is that its
treatment of Dirac’s general formulation of
quantum mechanics and the elegant notation introduced by Dirac
is not treated particularly well. The lectures will go well beyond the
text in a discussion of these issues. Liboff’s
*Introductory Quantum Mechanics *(ISBN
0-8953-8714-5) does an excellent job on this topic and students who feel
the need for a text book which discusses this issue may find this text a useful
supplement to

**Homework**

Problem sets will be
assigned regularly. Problem sets may require the use of numerical analysis that
can be done in *Mathematica** *or some
other computer program. I strongly encourage students to consult each other on
problem sets. Ideally you should attempt all of the problems by yourselves and
if you get stuck you should then consult your peers.

Homework will count approximately 20% of the final grade.

Not all problems will be graded---a representative sample will be. A set of solutions to the homework problems prepared by the TA will be posted on the course web cite for additional feedback. These solution sets may in part consistent of corrects solutions submitted by students in the course.

**Exams**

There will be a midterm exam and a final exam in this course. The exams will count for approximately 80% of the total course grade.

The exams are currently planned
as take-home. Take-home exams have two virtues: they reduce the time pressure
on students and allow them to perform at their best and they allow for
questions that are less trivial than can be done during a class period. They do
have a potential drawback, however. They are impossible to police efficiently
against cheating. Thus, we must rely on your integrity. I will ask you to
pledge to do the exams alone and to stick to this pledge. I should note that
the whole enterprise of science depends on the integrity of the researchers---
when I read a scientific paper I must assume that the researchers didn't cook
the books or I won't get anywhere.

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****Tentative Course
Outline**

**Introduction to Quantum
Phenomena
**

· Black-body radiation and Planck's conjecture

· Einstein's explanation of the photoelectric effect; photons;

· Wave-particle duality for light---

· The Bohr atom; connection of quantum phenomena to atomic spectroscopy

· De Broglie's hypothesis; wave-particle duality for matter.

· Interference and the Davisson-Germer experimerment.

· Born's probability interpretation of the wave function; Resolution of particle/wave duality.

· Motivating the Schrödinger equation; momentum as a differential operator

**Introduction to the Schrödinger Equation **

· Formal treatment of probability; normalization of the wave function

· Local conservation of probability

· Momentum in the Schrödinger equation; non-commuting operators

· The uncertainty principle

· Time-dependent vs. time-independent Schrödinger equations; stationary states and their superpositions

(Chap 1 )

**Quantum Mechanics in
One Dimension **

· The infinite Square well

· Harmonic oscillator; creation and annihilation operators

· Free particles; propagation

· Delta functions

· Finite Well

· Tunneling Scattering and resonance

(Chap 2)

**The formalism of
Quantum Mechanics**

· Postulates of Quantum Mechanics---operators, measurements and time evolution (

· Hermitian operators and physical observables

· Dirac Notation

· Heisenberg Matrix Mechanics

· Commutators and Uncertainty

· Time evolution and conservation laws

Chap (3)