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Division Algebras, Lie Algebras, Lie Groups and Spinors
One of the most
beautiful equations in all of mathematics is the exponential
of a pure imaginary complex number:
A really big point
to make here is the following: the only property of the complex
unit i used by this equation is i2 = -1. If u is an element of an
algebra that has an
identity (1), and u2 = -1, then exp(uθ)
= cos(θ) + u sin(θ). We
shall use this fact
repeatedly in what follows.
The norm squared
(length squared) of the complex number z = x + iy is:
zz* = (x + iy)(x - iy) = x2 + y2, where z* = (x - iy)
is the complex conjugate of z.
The complex conjugate of exp(iθ) is exp(-iθ)
= cos (θ) - i sin(θ),
so the norm
squared of exp(iθ) is
That is, the set
of all exp(iθ) is just the unit sphere (circle) in
the 2-dimensional
complex plane. This set plays many roles. In particular, it is the 1-sphere,
one of
three nontrivial parallelizable spheres (more anon); and it is the Lie group
U(1).
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