Multivectors, spinors and index theorems

Lecturer: Andreas Rosén, andreas.rosen@chalmers.se

Course description

Link to course plan

Notices:

20/11:
The course is finished. Please note that if you have feedback of any kind on the book, I VERY much appreciate if you share it with me! This will improve the next version.

17/11:
Last set of home work problems posted below. Deadline for that: 28/11.

11/11:
Three lectures left. We plan to finish the course next week. Information about the oral exam is posted below.

6/11:
Home work problems 6 posted below.

27/10:
Home work 5 posted below, with deadline next week.

2/10:
Home work 1 corrected. I hand them back on Monday. See below for information about grading, and hints for the home works problem.

23/9:
Three lectures this week, all in MVH11 (see below). No lectures next week.
Home work problems, set 2 and 3, are posted below.

15/9:
No lecture today, due to information meeting for PhD students.

5/9:
You find the first set of home work problems below.

1/9:
Course literature "Geometric multivector analysis" is now available at DC= DistributionsCentralen. (Somewhere a little south from Hörsalarna, and west from Gibraltargatan.)

21/8:
Welcome to the web page for this PhD course. First thing is to decide when to schedule the lectures: This is to be decided on our first meeting 1/9 at 13.15 in room Pascal: Please bring your calendar.

Lectures:

The following plan for the lectures will be continuously updated during the course.

Dates
Contents of lectures
Sections in
the book
Deadlines
and other to-do:s
Lecture 0: 1/9
room Pascal
Info about the course and examination
An informal overview of the course:
What are multivectors, spinors and Dirac operators?
What are the index theorems that we aim to prove?
1.1-1.3
Get a copy of the
course book:
Available from DC
(=Distributions-
Centralen)
at course start.
Lecture 1: 4/9
10.00-11.45
MVH11
Construction of multivectors, universal property
Grassmann cone, oriented measure
2.1-2.4
1.5

Lecture 2: 8/9
13.15-15.00
MVH11
Duality, inner product spaces
Multicovectors and alternating forms
Interior products and Hodge stars
2.5-2.8

Lecture 3: 11/9
10.00-11.45
MVH11
The Clifford product
Three dimensional rotations, quaternions and spin

3.1-3.2

Lecture 4: 18/9
10.00-11.45
MVH11
The Clifford cone
Euclidean rotations and spin groups
Infinitesimal rotations and bivectors
4.1-4.3
Home work 1:
exterior algebra
Lecture 5: 22/9
13.15-15.00
MVH11
Abstract Clifford algebras
Representation of real Clifford algebras
3.3-3.4

Lecture 6: 23/9
10.00-11.45
MVH11
Complex spinors in inner product spaces
The standard representation
Ideals in matrix algebras
5.1-5.2
1.4, 1.6

Lecture 7: 24/9
10.00-11.45
MVH11
Uniqueness up to almost unique isomorphism
Mappings of spinors
5.2-5.3

Lecture 8: 6/10
13.15-15.00
MVH11
Exterior derivative and pullback
Interior derivative and pushforwards
7.1-7.2
Home work 2:
Clifford algebra
Lecture 9: 9/10
10.00-11.45
MVH11
Integration of k-covector fields and general k-forms
Embedded oriented k-surfaces
Stokes theorem
7.4-7.5
6.1
Home work 3:
spinors
Lecture 10:13/10
13.15-15.00
MVH11
Elliptic Dirac operators and hypercomplex analysis
Maxwell's equations
9.1-9.2


Lecture 11: 16/10
10.00-11.45
MVH11
The tangent bundle
Levi-Civita covariant derivative
Frames
Covariant derivative 1-forms
The exterior bundle, its covariant derivative
6.2-6.4
7.3
11.1

Lecture 12: 20/10
13.15-15.00
MVH11
Hyperbolic Dirac operators
Maxwell's equations, Dirac's equation
10.1-10.2
Lecture 13: 24/10
13.15-15.00
NOTE: Friday!
MVH11
Exterior and interior derivatives on manifolds
Curvature 2-forms
Commutator formulas for
covariant derivative and curvature
11.1-11.3
Home work 4:
affine multivector
calculus
Lecture 14: 27/10
13.15-15.00
MVH11
Hodge decompositions
Gaffney inequality
Weitzenböck, Laplace-Beltrami operator
11.4-11.5
8.2

Lecture 15: 30/10
10.00-11.45
MVH11
Cech Cohomology
Algebraic calculation of Betti numbers
Poincaré's theorem
11.6
8.8-8.9
8.1

Lecture 16: 3/11
13.15-15.00
MVL14
Chern-Gauss-Bonnet 1
The heat equation method
Normal coordinates
12.1-12.2
Home work 5:
multivectors and
manifolds
Lecture 17: 10/11
13.15-15.00
MVL14
Chern-Gauss-Bonnet 2
Trace calculations
Pfaffian
12.2

Lecture 18: 13/11
10.00-11.45
MVL14
Spinor bundle
Covariant derivative and curvature
Stiefel-Whitney classes
12.3
Home work 6:
Chern-Gauss-Bonnet
Lecture 19: 17/11
13.15-15.00
MVL14
Atiyah-Singer 1
spin-Dirac operator
Weitzenböck formula
12.3-12.4

Lecture 20: 20/11
10.00-11.45
MVL14
Atiyah-Singer 2
Mehler's formula
The A-roof functional
12.4
Home work 7:
Atiyah-Singer


Examination:

For PhD students taking the course, the examination consists of
Home work problems. This file is updated during the course. Last update: 4/12.

About one week before each deadline, the version will be final for that set of home works.
Home work 1: above version is final.
Hints:
1: Exc. 2.30, 2.46, 2.47, 7.54
2: Cor. 2.69, Exc. 2.73
3: Prop. 1.40
Home work 2: above version is final.
Hints:
1: Prop. 3.17: The key problem: what multiple of pi is b unique modulo?
2: Lem. 4.22, Ex 4.24 and 4.25
4: Exc. 3.31, Lem. 3.45 + recall from lecture 5 the representation of the euclidean line.
Home work 3: above version is final.
Hints:
1: Thm. 5.5, Props. 5.16-18
2: Prop. 5.24, comment after Prop. 5.15
Home work 4: above version is final.
Hints:
1: Why is the formula valid for general MULTVECTOR fields?
3: Prop. 7.8(i)
Home work 5: above version is final.
Hints:
1. The dual basis may be useful.
2: Which of the two dualities requires orientablility for its global formulation?
3. For a bounded and bijective linear operator T:X->Y between Banach spaces: What does functional analysis say about its inverse?
Apply this result for suitable T, X and Y. Be careful to say which norms you use! When is Hodge used?
Home work 6: above version is final.
1: Prop. 1.43 can be used for a short proof.
2. Bianchi symmetries? Prop. 3.12? ???
3: Note: any metric on the given manifold will give the same CGB integral, right?
Home work 7: above version is final.
1: Note: it is meaningless to say that an n-vector field on a manifold is constant. But you want to show that such a field has zero covariant derivatives.
3: If the y-integral of k(x,y) is 1 with almost all the mass in a small neighbourhood of x, then int k(x,y)f(y)dy is roughly...