For a group action of on a set and , the orbit-stabilizer theorem statesIf is finite, this becomes . The underlying bijection sends the left coset to . Equality of two image points is equivalent to , so this map is both well-defined and injective, and it is surjective by the definition of the group orbit.
Place the cube's vertices at . Every symmetry fixes its centre, and permutes the three perpendicular pairs of face normals, so it is a signed permutation matrix. Conversely every such matrix preserves the cube. The symmetry group of a cube acts transitively on its eight vertices: independent coordinate sign changes take to any vertex.
A symmetry fixing must permute its three incident edges. This gives an injective map from its stabilizer subgroup into , since those three edge directions determine the linear transformation. All six permutations are realized by coordinate permutation matrices, which fix . Thus the vertex stabilizer has order six. The orbit-stabilizer theorem now yieldsThe use of all symmetries includes reflections as well as the twenty-four elements of the rotational symmetry group of a cube.
There are nontrivial proper normal subgroups. The determinant defines a surjective group homomorphism . Its kernel is the rotational symmetry group of a cube, a normal subgroup of order twenty-four. Also is a central subgroup of order two: central inversion preserves the cube and commutes with every matrix. Both provide affirmative examples.
For the body diagonal through , write a general cube symmetry as , with a permutation matrix and , each . Since , preserving the unoriented diagonal requires to be either or . ThusThe map from to is a group homomorphism, because central inversion commutes with every coordinate permutation. It is surjective by the displayed description and injective because a permutation matrix cannot equal the negative of another permutation matrix. Consequently the body-diagonal stabilizer in the cube symmetry group isThis also agrees with the orbit-stabilizer theorem for the transitive action on the four body diagonals. The line is preserved as a set, so exchanging its opposite endpoints is allowed.
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