Physics 511-512
Quantum Mechanics I, II
Luming Duan
Fall 2012 - Winter
2013
Welcome to the homepage of the course for
Quantum Theory and Atomic Physics! This is a two-semester graduate-level
course.
Course Description
This course will focus on the explanation of fundamental concepts,
mathematical structure, and calculation methods of quantum mechanics. The
course covers the following topics: fundamental concepts of quantum mechanics
and its mathematical structure, exactly solvable quantum systems, symmetries in
quantum mechanics, approximation methods, atomic and Molecular structure,
scattering theory, quantum many-particle systems, relativistic
wave equations.
Class meetings
Time:
Tuesday, Thursday, 11:30AM -1:00PM
Location: 455 Dennison
Instructors
Luming Duan
4219 Randall Hall
Telephone: (734) 763-3179
Email: lmduan@umich.edu
Web: http://www-personal.umich.edu/~lmduan/
Course website: http://www-personal.umich.edu/~lmduan/QM1-pub.html
Teaching assistant (Grader): Paul Bierdz (Randall 4409) Email:
paopao@umich.edu
Course Requirements
There will be regularly assigned problem sets. Your letter
grade will be based on the two exams (Midterm 20%; Final: 40%), homework (30%),
and class participation (10%).
Prerequisites
The basic mathematical prerequisites are linear algebra and
calculus. It would be useful to have a previous course on introductory quantum
mechanics at the undergraduate level, but that is not an essential requirement.
Some results from group theory will be used for discussion on symmetries, but I
will explain the results before I use them.
Books and References
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Main Reference
Books
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Either of them
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Other
recommended
books
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- J.J. Sakurai, Modern
Quantum Mechanics (1982)
- E. Merzbacher,
Quantum Mechanics (1998)
- P.A.M. Dirac, The
Principles of Quantum Mechanics
- David J. Griffiths Introduction
to Quantum Mechanics.
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Further Readings
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- C. Cohen-Tannoudji, B. Diu, and F. Laloe,
Quantum Mechanics (1997)
- R. P. Feynman and A.
R. Hibbs, Quantum Mechanics and Path Integrals
- L. Landau and E. Lifshitz, Quantum Mechanics: Non-relativistic Theory
- J. Preskill,
Lecture Notes on quantum information and computation (the first four
chapters, which are general quantum mechanics), see
http://www.theory.caltech.edu/people/preskill/ph229/#lecture
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Course Outline
First term (Fall 2012)
- History of quantum mechanics
- Old quantum theory
- Establishment of
quantum mechanics
- Development of
quantum mechanics
- Relation of quantum mechanics to current
physics frontiers
- General structure of this course
- Fundamentals (formalism)
of quantum mechanics
- Overview
- Wave-particle
duality (Albers:p19-23; Sakurai:p2-9)
- What is
wave-particle duality
- The double-slit
experiment
- The Stern-Gelach experiment
- Quantum states and
vectors in the Hilbert space (Albers:p24-34; Sakurai:p10-35)
- Why vectors
- Mathematical review
about vectors
A complex vector space, adjoint
vectors, inner product and norm, basis of a vector space, expansion with a
basis, Hilbert space
- Observables and
operators in the Hilbert space (Albers:p24-34; Sakurai:p10-35)
- How to describe
observables
- Mathematical review
about operators
Linear operators, representation
of operators, functions of operators, Eigenvalue and
eigenvectors, Hermitean and unitary operators, spectral
decomposition, some theorems about operators
- Measurements,
Probability interpretation, and Von Neumann's projectors (Albers:p24-34;
Sakurai:p10-35)
- Formalism for
quantum measurements
- Applications:
distinguishing quantum states and quantum cryptography
- Examples of Hilbert
space: finite-dimensional systems (outside of textbook, further reading:
J. Preskill, Lecture Notes on quantum
information and computation)
- Physical examples of
two-dimensional (qubit) systems
- Description of qubit systems
- Extension to
d-dimensions (qudit systems)
- Examples of Hilbert
space: continuous-variable systems
(Albers:p35-38; Sakurai:p41-59)
- Normalization of
continuous-variable states and Dirac's delta-function
- Coordinate-basis
representation
- Fourier transform
theorem
- Momentum-basis
representation
- Transfer between
coordinate and momentum bases
- Cononical
commutation relation
- Uncertainty relation
(Albers:p47-49; Sakurai:p23-35)
Proof of uncertainty relation, minimum uncertainty state (coherent state)
- Quantum dynamics
(Albers:p44-53; Sakurai:p68-108)
- Evolution operator
- Schrodinger equation
- Representations of
Schrodinger equation in different bases
- Schrodinger picture
and Heisenberg picture
- Applications to free
particles and harmonic oscillators, quantum dispersion
- Multiparticle
systems, density matrix, and quantum entanglement (outside of textbook,
further reading: J. Preskill, Lecture Notes on
quantum information and computation)
- Hilbert space of
multi-particles, distinguishable vs. indistinguishable particles
- Density matrix and
its properties
- Quantum
entanglement, characterization, and von Neumann's entropy
- Quantum nonlocality and Bell's
inequalities (Albers:p193-195, Griffiths:p420-427,
further reading: J. Preskill, Lecture Notes on
quantum information and computation)
- Background: EPR
paradox and local hidden variable theories
- The Bell-CHSH
inequality
- Experimental
detection of the CHSH inequality
- Open quantum systems,
decoherence, and interpretation of measurements
(outside of textbook, further reading: J. Preskill,
Lecture Notes on quantum information and computation; Zurek,
arxiv, Physics Today article)
- Evolution of open
quantum systems, Kraus representation
- Master equation and Lindblad form
- Decoherence
- Interpretation of
wave-function collapse for measurements
- Exactly solvable quantum
systems
- Overview
- Evolution of
finite-dimensional systems and applications to atomic clocks and neutrino
oscillation (Albers 63-65; Further reading: see review articles on atomic
clocks from Rev. Mod.Phys. )
- Evolution of
2D (qubit) systems: time-independent
Hamiltonian
- Time-dependent
Hamiltonian and the interaction picture
- Resonant Rabi
oscillation
- Atomic clocks and
Ramsey methods
- Neutrino
interference and oscillation (Albers: p185-190)
- 1D
continuous-variable systems: sectionally-constant
and delta potentials (Albers 66-68)
- General methods and
boundary conditions
- General concepts
from these potentials: quantization, tunneling, and scattering
- The harmonic
oscillators (Albers p68-73, Sakuri:p89-96, Griffiths: p40-58)
- The annilation and creation operators
- Energy spectrum
- Energy eigenstates and their representation in the
coordinate basis
- Generalization of
the harmonic potentials
3-dimensions,
n decoupled and coupled harmonic oscillators,
examples with trapped ions, phonons in solids, and photons from the EM field
- Spherically symmetric
potentials and angular momentum (Albers p74-84; Griffiths:p131-171)
- Angular momentum and
its commutation relations
- Eigenvalues
and co-eigenstates of the angular momentum
operators
- Reduction of 3D spherically
symmetric potentials to 1D potentials
- Hydrogen-like atoms
(Albers p84-90; Griffiths:p145-171)
- Series expansion
method, energy spectrum, general discussion about applications
- Charged particles in
magnetic fields: the Aharonov-Bohm phase and
the Landau levels (part of material in Albers p324-341; Sakurai:p109-142)
- Brief review of
classical EM
- Gauge invariance:
classical and quantum
- The Aharonov-Bohm effect explained from the gauge
transformation
- Charged particles in
a constant magnetic field and the Landau levels
- Brief discussion of
the quantum Hall effects
- Symmetries in quantum
mechanics
- Brief overview about
symmetries and their applications
- Mathematical review:
groups and algebra (Albers:p102-112, Sakurai:p152-173)
- Groups: finite and continuous
(Lie) groups
- Typical Lie groups:
O(n), SO(n), U(n), SU(n)
- Representation of
groups: reducible and irreducible representations
- Representation of
Lie group and Lie algebra in quantum mechanics
- Translation and
rotation groups and algebra, Euler angles
- Wigner's d-functions
and Schwinger's representation of angular momentum operators (Alber: p113-119; Sakurai:p168-173, p217-222)
- Representation of
angular momentum operators and rotation groups, Wigner's d-functions
- Schwinger's
representation of angular momentum operators
- Calculation of
Wigner's d-functions from Schwinger's representation
- Addition of angular momenta and Clebsch-Gordan
coefficients (Albers:p120-130; Sakurai: p203-216)
- Why addition of
angular momenta
- Addition of angular momenta: procedure
Note its relation with irreducible
decomposition of tensor product representation of rotation groups (algebra)
- Clebsch-Gordan
(CG) coefficients and their properties
- Calculation of C-G
coefficients: intuitive picture and the recursion relations
- Addition of
more-than-two angular momenta
- Rotation
transformations and selection rules for scalar and vector observables
(Alber:p138-143; Sakurai:p232-242)
- Symmetry
transformations on operators: Heisenberg versus Schrodinger picture
- Scalar and vector
observables under rotation, spherical components
- Selection rules for
vector observables
- Rotation
transformations and selection rules for tensor observables, Wigner-Eckart theorem (Alber:p144-150; Sakurai:p232-242)
- Tensor observables
- Decomposition of tensor
observables into spherical components
Note its relation with addition of
angular momenta, both corresponding to irreducible
decomposition of tensor product representation of rotation groups (algebra)
- Wigner-Eckart theorem and its proof
- Selection rules for
tensor observables
- Discrete symmetries
(Alber:p151-163; Sakurai:p251-281)
- Examples of discrete
symmetries: space and time reversion, translation and rotation in
lattices
- Space reversion and
parity
- Time reversion,
anti-unitary operators, and Kramers degeneracy
Second term (Winter 2013)
- Brief introduction and
review
Review of the course structure and the first-semester contents
- Approximation methods in
quantum mechanics
- Overview of
approximation methods in QM
- Time-independent
perturbation methods (Albers:p202-205; Sakurai:p285-303; Griffiths: p249-265)
- The general method
and classification of perturbation theory
- Bound-state
non-degenerate perturbation
Basic recursion relations for
arbitrary order perturbation, explicit formula for 1st and 2nd order
perturbation
- The degenerate
perturbation method
- Convergence,
asymptotic series, and limit of perturbation theory
- Example applications
of the time-independent perturbation (Albers:p206-211;
Sakurai:p285-303;)
- d.c. Stark
shift (from a static electric field) of the ground state of the
hydrogen-like atoms (non-degenerate perturbation)
- d.c. Stark
shift of excited states of the hydrogen-like atoms (degenerate
perturbation)
- Atom's polarizability and atom's trap
- a.c.
Stark shift (from a laser) of the ground state of the hydrogen-like
atoms
- Design of optical
lattice from a.c. Stark shift
- Time-dependent
perturbation, transition, and Fermi's golden rule (Albers:p288-291;
Sakurai:p316-340; Griffiths:
p340-367)
- Time-dependent
perturbation (formalism)
- Time-energy
uncertainty relation
- Fermi's golden rule
for transition (discrete spectrum to continuous spectrum)
- Atomic transition
through broadband incoherent (thermal) light
Stimulated emission and
absorption, explain of spontaneous emission
- Quantum Zeno effect
(coherent vs incoherent transitions)
(Albers:p313-314; Griffiths:
p431-434)
- The variational method (Albers:p223-228;
Sakurai:p313-316; Griffiths:
p293-314)
- The general idea
- The variational principle for the stationary Schrodinger
equation
- The variational principle for the dynamical Schrodinger
equation
- A simple
illustrative example: Harmonic potential
- Example applications
of the variational method
- The ground state of
the Helium-like atoms (Albers:p225-227; Griffiths: p299)
- The band-gap
structure for atoms in the optical lattice (outside of textbook)
- Quantum phase
transitions in quantum magnetism: mean-field theory for the anisotropic
Heisenberg model (outside of textbook, further reading: any book on ¡°Quantum Magnetism¡±)
- The semi-classical
(WKB) method (Albers:p237-243; Griffiths:
p315-339)
- The WKB
approximation
- Turning points and
the connection formula
- Example applications
of the WKB method (Albers:p243-247; Griffiths:
p315-339)
- Quantization
condition for a single-minimum potential
- Quantization
condition and the eigen-energies of the
double-well potential
- Tunneling through
any potential barrier
- The adiabatic
approximation and the Berry's phase
(Albers:p341-349; Griffiths:
p368-393)
- The fast and slow evolution:
sudden versus adiabatic approximation
- The adiabatic
theorem and the Berry's
phase
Proof the adiabatic theorem,
dynamical and Berry's
(geometric) phase, Estimation of the transition probability
- The adiabatic
passage with counter-intuitive pulses (out of textbook, see arxiv research articles on STIRAP)
- The adiabatic
quantum algorithm (out of textbook, see arxiv
research articles on adiabatic quantum computing)
- The Berry's phase for
a two-level system
- Structure of atoms and
molecules
- Overview
- Overview of the
atomic and molecular structure
- About the units
- Fine structure of the
hydrogen-like atoms (Albers:p212-216; Sakurai: p304-312, Griffiths: p266-276)
- Spin-orbital
coupling
- Splitting of the
energy levels due to the spin-orbital coupling
- The relativistic
correction to eigen-energies and the whole
fine structure
- The hyperfine
structure of the hydorgen-like atoms
(Albers:p218-220; Griffiths:p283-292)
- The basic picture
- The hyperfine
coupling Hamiltonian
N, L coupling, N,S
coupling (contact vs. dipole terms)
- The hyperfine
splitting of the ground state
Level splitting, applications in
radio astronomy
- Influence of magnetic
fields on atomic structure: Zeeman effects (Albers:p217-218; Sakurai:
p304-312, Griffiths:
p277-282)
- Atomic magnetic
moment
- Zeeman effects
within Fine structure
- Zeeman effects
within hyperfine structure
- The molecular
structure (Albers:p229-236; Griffiths:
p304-314)
- The Born-Oppenheimer
approximation
- The electronic
structure of the molecular hydrogen ion
- Vibrational
and rotational levels
- Scattering theory
- Overview
- motivation and
general picture of scattering
- Formulation of
scattering and the Lippmann-Schwinger equation (Albers:p264-269,291-307;
Sakurai: p379-385,424-428; part in Griffiths:
p394-408)
- The general problem
and the Green's operator (propagator)
- Derivation of the
Lippmann-Schwinger equation
- The
Lippmann-Schwinger (LP) equation in the coordinate basis
- The cross section
from the LP equation
- The Born
approximation and its applications (Albers:p264-270; Sakurai: p386-389, Griffiths:
p408-419)
- The Born series
- Some applications
with spherically symmetric potentials
- The transition matrix
and the optical theorem (Albers:p291-307; Sakurai: p390-391)
- The dressed
propagator and the transition matrix (T-matrix)
- The cross section
with the T-matrix
- The optical theorem
- Method of
partial-wave expansion (Albers:p270-272; Sakurai: p399-409, Griffiths:
p399-407)
- Partial-wave
expansion
- Unitarity
requirement and the collision phase shift
- Solve the collision
phase shift
- The low-energy scattering
and the the resonance scattering (Sakurai:
p410-420)
- The low-energy
scattering
- The resonance
scattering
- Feshbach
resonance and its applications in ultracold
atomic physics (outside of textbook)
- Quantum many particle
systems
(Outside of the textbooks. Some further readings for
this chapter: A. Fetter and J. Walecka, ¡°Quantum Theory of Many-Particle Systems¡±,
Ch. 1, p3-50; Abrikosov, Gorkov,
Dzyaloshinski, ¡°Methods of
Quantum Field Theory in Statistical Physics¡±, Ch. 1,p1-40; Dirac, ¡°Principles of
Quantum Mechanics¡±, p207-252.)
- Overview
- First-quantization
representation of identical particles
- Identical particles
and different quantum statistics
- The
first-quantization representation of states for bosons and fermions
- Second-quantization
representation of identical particles
- Non-interacting bosonic and fermionic
systems
- Bose condensation
- Fermi surface
- Interacting bosonic systems
- Mean-field theory
and the Gross-Pitaevskii equation
- Interacting fermionic systems
- Mean-field theory
and the Hartree-Fock equation
Homework
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