meichenl
Regular
I'm wondering if anyone can give me some insight on why the cube group is as large as it is.
I know, for example, that the parity of the permutation of the corners and edges must be the same because each quarter turn is an odd permutation of both (excluding slice turns, double layer turns, and cube rotations). This excludes half of the conceivable permutations of the cubies.
It remains to be shown that the other half of the permutations can be solved. One way to do this is to note that any odd permutation becomes even with a single quarter turn. Also, all even permutations can be factored into 3-cycles. Next, find one 3-cycle, and then conjugate it to produce all conceivable 3-cycles. This shows that the other half of the permutations of the cubies can be solved.
Similarly for orientations, once the orientation of a cubie not at home is defined, it is easy to see the restrictions on cubie orientation. To prove there are no more restrictions we're missing, though, the only way I know is to give commutators that flip two edges or that flip two corners, and by conjugating those show how to solve any remaining orientation of the cubies.
These aren't viscerally satisfying to me, but I haven't found any better way to approach the problem.
I know, for example, that the parity of the permutation of the corners and edges must be the same because each quarter turn is an odd permutation of both (excluding slice turns, double layer turns, and cube rotations). This excludes half of the conceivable permutations of the cubies.
It remains to be shown that the other half of the permutations can be solved. One way to do this is to note that any odd permutation becomes even with a single quarter turn. Also, all even permutations can be factored into 3-cycles. Next, find one 3-cycle, and then conjugate it to produce all conceivable 3-cycles. This shows that the other half of the permutations of the cubies can be solved.
Similarly for orientations, once the orientation of a cubie not at home is defined, it is easy to see the restrictions on cubie orientation. To prove there are no more restrictions we're missing, though, the only way I know is to give commutators that flip two edges or that flip two corners, and by conjugating those show how to solve any remaining orientation of the cubies.
These aren't viscerally satisfying to me, but I haven't found any better way to approach the problem.