Today I noticed that a change of basis of a 3D multivector (i.e. complex quaternion) which obtains idempotent/nilpotent ‘light cone variables’ (elements squaring to themselves or zero) is equivalent to a choice of 2x2 complex matrix representation! (1/6)
The 2x2 matrix is a place to measure spin up and spin down as your two orthogonal basis elements, and your choice of axis determines which direction D lands on the main diagonal as (1+D)/2 and (1-D)/2 whilst the orthogonal components get mixed into the off diagonal elements.
It then becomes intuitive how diagonalizing one choice of representation maximally mixes how much spin up/down you find in a representation with an orthogonal choice. Zeroing those off-diagonals means finding a reference frame where those contributions are equal and opposite!
So if choosing a 2x2 matrix representation forces us to choose a special axis whose eigenvalues are spin up and down, might some more general eigenvalues exist if we *don’t’ convert to a matrix? Can complex quaternions have first class eigenvalues and vectors?
I guess they exist and can be found analogous to pseudo-diagonalizing an asymmetric matrix. Multiplying a multivector by its reverse is exactly like multiplying a matrix by its Hermetian transpose; it squares scaling factors while canceling out any antisymmetric rotation.
The question then becomes how to interpret what our eigenvectors are and what they mean. Should the result be treated as a complex paravector, with complex eigenvalues in x, y, z, and time? Do these relate in any way to a possible real world measurement?
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The complex quaternions are more than a 2D phase rotation and a 3D spatial rotation. They are more than the sum of their parts. Today I want to talk about one such feature that you can’t get from complex numbers or quaternions on their own. I want to talk about projectors. (1/15)
A complex quaternion has real scalar and bivector parts and imaginary scalar and bivector parts. Instead of breaking these up into four complex pieces or two quaternion pieces we can instead mix and match, affixing the imaginary bivector to the real scalar and vice versa.
These mixed ‘paravectors’ aren’t quaternions, and complex paravectors are something new. The scalar acts special… almost ‘time-like’. A rotation between the scalar direction and any vector direction has changed from being elliptic to being hyperbolic.