I'm going to email him.
https://www.youtube.com/watch?
- The Lorentz transformation from frame tois defined by velocity.
- The inverse transformation from tois defined by velocity.
- Because the structure of Minkowski spacetime is the same for both, neither observer is "preferred" or "special." The relationship is perfectly reciprocal.
- Boosts are symmetric matrices: A "pure" boost (moving in a straight line without rotation) is represented by a symmetric matrix.
- General transformations are not: A general Lorentz transformation includes both boosts and spatial rotations. Because rotations are represented by orthogonal (non-symmetric) matrices, the product of a boost and a rotation generally results in an asymmetric matrix.
- Basis-dependent: Whether a matrix is symmetric is a property of the coordinate basis, not the underlying physical transformation. If you change your basis (for example, by rotating your axes), a transformation that looked symmetric might suddenly look asymmetric.
- Time dilation and length contraction: It is common to focus on one frame "doing the measuring" of the other. While both frames agree that the other clock is running slow, an individual observer sees a specific, one-way result in their own measurements. This isn't an asymmetry in the laws of physics, but a consequence of the relative perspective.