Symplectic geometry arose from the study of optics and the study of mechanics. (In MAS 441 we won't consider mechanics.) In the past 20 years or so it has become a major part of modern mathematics.

When a ray of light passes through a lens (such as the lens in
a pair of spectacles, or in a telescope) its direction is changed
-- or *refracted* -- and the change in direction corresponds
to a *symplectic matrix*. The definition of a symplectic matrix
looks similar to that of an orthogonal matrix and just as an orthogonal
matrix preserves the dot product, and hence distances and angles,
symplectic matrices preserve a `symplectic structure', which we'll
define early on in the course. Although symplectic matrices are
defined in a similar way to orthogonal matrices, their properties
are very different.

Symplectic geometry enters modern mathematics in several different ways. For example, the set of all straight lines in the plane, or in any Rn, has a symplectic structure. Symplectic structures arise in the study of Lie algebras, and in complex geometry. (We will touch on the first two of these examples.)

Symplectic geometry is actually part of differential geometry, but MAS 441 is quite different to MAS 336, which focuses on curves and surfaces in three dimensions.

MAS 441 does not assume any knowledge of the physical properties of light. What is required is actually quite small, and will be covered as we need it.

If you look on the web or in books for information about symplectic geometry you will probably be told that the subject developed from theoretical mechanics. In fact Hamilton (1805-1865), who developed what is called the Hamiltonian formalism in mechanics, first developed his theory for optics, and only afterwards realized that the same mathematical ideas apply to mechanics. This is not at all obvious and is a striking example of how a mathematical theory can have applications which are unrelated to each other. The underlying phenomenon is that the solutions of a variational problem have a symplectic structure.

The prerequisite course is MAS 211 Advanced Calculus and Linear Algebra (or, if you took second year in 2013-14, MAS 201, Linear Algebra for Applications, and MAS 202, Advanced Calculus.

If you haven't taken MAS 211,
it * may *
still be possible to take MAS 441. In this case, you should get in touch with me to
discuss your background.

Other relevant course:

- MAS 336 Differential Geometry.

If MAS 441 interests you, then MAS 336 probably will too, and conversely. MAS 441 uses the concept of parametrized surface and implicit surface, just as in MAS 336, but you will have met these in MAS 202 or elsewhere, and revision of them is included. MAS 441 does not make any use of curvature or other main concepts from MAS 336.

To summarize: Provided you have taken MAS 211, you are welcome to enrol in MAS 441. It is helpful, but not necessary, to have taken MAS 336.

Over the years I have presented this course in two different ways. In one version I work entirely in Euclidean spaces; that is, in coordinates. In the other I use abstract vector spaces and make use of dual vector spaces. Each version has advantages and complications. As the start of the course approaches I will decide which version to give this year. If you are taking the course and have a firm preference, please let me know.

October 26, 2016