The quotient group consists of the cosets , with multiplicationFor well-definedness, replacing representatives by and changes their product to . Since is a normal subgroup, the final two factors lie in , so the product coset does not change.
Associativity follows from that in ; the identity element is the coset , and . Hence these cosets form a group. By Lagrange's theorem, every subgroup has order dividing , and its subgroup index is . In particularNormality is needed for the quotient multiplication, whereas Lagrange’s counting formula holds for every subgroup.
The four displayed matrices fail closure: for example is not one of them. Thus they do not form a group by themselves.
Let and . The enlarged set is the single-qubit Pauli groupThere are 16 distinct matrices: are linearly independent, so two different ones cannot be scalar multiples, and the four phases are distinct for each nonzero matrix.
The Pauli matrices satisfyHere is the Kronecker delta and the Levi-Civita symbol. Thus any product of two Pauli matrices is another Pauli matrix or the identity times a phase in . Multiplying by the two original phases preserves membership in , proving closure of all 16 matrices.
Associativity is inherited from matrix multiplication, the identity is , andThis proves every group axiom. The resulting group is non-Abelian, since reversing changes its sign.
For every positive integer , the group laws give . ConsequentlyThe sets of positive exponents returning the two elements to the identity element are identical. If this set is nonempty, its least member is the order of a group element in both cases. If it is empty, neither element has finite order. Therefore, including the infinite-order case,For a direct divisibility argument in the finite case, if has order , then , so its inverse’s order divides . Reversing the roles shows divides that order, forcing equality. This is the general fact that an element and its inverse have the same order; it also reflects as cyclic subgroups.
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