John Baez wrote:(adsbygoogle = window.adsbygoogle || []).push({});

>So one thing you're saying

>is that a product of rotations in two different rest frames can be

>a boost??

One way to see why the products of some rotations will be boosts is as

follows.

Suppose that for a pair of linearly independent vectors u and v in R^3 we

can find an element of O(2,1) with the following properties:

* it preserves both u and v

* its determinant is -1

* its square is the identity

If we can find such an element, we'll call it ref(u,v).

Now, if we pick three linearly independent vectors u, v and w so that

ref(u,v), ref(u,w) and ref(v,w) all exist, we can construct the following

elements of SO(2,1):

g1 = ref(u,v) ref(v,w) which preserves v

g2 = ref(v,w) ref(u,w) which preserves w

g3 = ref(u,v) ref(u,w) which preserves u

and we have g3 = g1.g2 because ref(v,w)^2 = I.

So if we pick a spacelike u and a timelike v and w, we'll have a boost

that's equal to a product of rotations.

The one question that remains is, when can we find ref(u,v)? This is

trivial in O(3), but O(2,1) is trickier. Generically we can construct a

normal n to the plane spanned by u and v:

n^a = g^{ab} eps_{bcd} u^c v^d

and if it's not a null vector we can construct ref(u,v) as the projector

into the plane minus the projector onto n. But if n is null, I don't

think ref(u,v) exists.

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# Re: This Week's Finds in Mathematical Physics (Week 232)

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