Quaternion group

Cycle diagram of Q. Each color specifies a series of powers of any element connected to the identity element (1). For example, the cycle in red reflects the fact that i ² = −1, i ³ = −i  and i ⁴ = 1. The red cycle also reflects the fact that (−i )² = −1, (−i )³ = i  and (−i )⁴ = 1.

In group theory, the quaternion group is a non-abelian group of order eight, isomorphic to a certain eight-element subset of the quaternions under multiplication. It is often denoted by Q or Q₈, and is given by the group presentation

$\mathrm{Q} = \langle -1,i,j,k \mid (-1)^2 = 1, \;i^2 = j^2 = k^2 = ijk = -1 \rangle, \,\!$

where 1 is the identity element and −1 commutes with the other elements of the group.

Compared to dihedral group

The Q₈ group has the same order as the dihedral group D₄, but a different structure, as shown by their Cayley and cycle graphs:

Cayley graph		Cycle graphs
Q8 The red arrows represent multiplication on the right by i, and the green arrows represent multiplication on the right by j.	Dih4 Dihedral group	Q8	Dih4

The dihedral group D₄ arises in the split-quaternions in the same way that Q₈ lies in the quaternions.

Cayley table

The Cayley table (multiplication table) for Q is given by:

Q×Q	1	−1	i	−i	j	−j	k	−k
1	1	−1	i	−i	j	−j	k	−k
−1	−1	1	−i	i	−j	j	−k	k
i	i	−i	−1	1	k	−k	−j	j
−i	−i	i	1	−1	−k	k	j	−j
j	j	−j	−k	k	−1	1	i	−i
−j	−j	j	k	−k	1	−1	−i	i
k	k	−k	j	−j	−i	i	−1	1
−k	−k	k	−j	j	i	−i	1	−1

The multiplication of the six imaginary units {±i, ±j, ±k} works like the cross product of unit vectors in three-dimensional Euclidean space.

$\begin{alignat}{2} ij & = k, & ji & = -k, \\ jk & = i, & kj & = -i, \\ ki & = j, & ik & = -j. \end{alignat}$

Properties

The quaternion group has the unusual property of being Hamiltonian: every subgroup of Q is a normal subgroup, but the group is non-abelian. Every Hamiltonian group contains a copy of Q.

In abstract algebra, one can construct a real four-dimensional vector space with basis {1, i, j, k} and turn it into an associative algebra by using the above multiplication table and distributivity. The result is a skew field called the quaternions. Note that this is not quite the same as the group algebra on Q (which would be eight-dimensional). Conversely, one can start with the quaternions and define the quaternion group as the multiplicative subgroup consisting of the eight elements {1, −1, i, −i, j, −j, k, −k}. The complex four-dimensional vector space on the same basis is called the algebra of biquaternions.

Note that i, j, and k all have order four in Q and any two of them generate the entire group. Another presentation of Q demonstrating this is:

$\langle x,y \mid x^4 = 1, x^2 = y^2, y^{-1}xy = x^{-1}\rangle.\,\!$

One may take, for instance, i = x, j = y and k = x y.

The center and the commutator subgroup of Q is the subgroup {±1}. The factor group Q/{±1} is isomorphic to the Klein four-group V. The inner automorphism group of Q is isomorphic to Q modulo its center, and is therefore also isomorphic to the Klein four-group. The full automorphism group of Q is isomorphic to S₄, the symmetric group on four letters. The outer automorphism group of Q is then S₄/V which is isomorphic to S₃.

Matrix representations

Q. g. as a subgroup of SL(2,C)

The quaternion group can be represented as a subgroup of the general linear group GL₂(C). A representation

$\mathrm{Q} = \{\pm 1, \pm i, \pm j, \pm k\} \to \mathrm{GL}_{2}(\mathbf{C})$

is given by

$1 \mapsto \begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix}$

$i \mapsto \begin{pmatrix} i & 0 \\ 0 & -i \end{pmatrix}$

$j \mapsto \begin{pmatrix} 0 & 1 \\ -1 & 0 \end{pmatrix}$

$k \mapsto \begin{pmatrix} 0 & i \\ i & 0 \end{pmatrix}$

Since all of the above matrices have unit determinant, this is a representation of Q in the special linear group SL₂(C). The standard identities for quaternion multiplication can be verified using the usual laws of matrix multiplication in GL₂(C).

Q. g. as a subgroup of SL(2,3)

There is also an important action of Q on the eight nonzero elements of the 2-dimensional vector space over the finite field F₃. A representation

$\mathrm{Q} = \{\pm 1, \pm i, \pm j, \pm k\} \to \mathrm{GL}(2,3)$

is given by

$1 \mapsto \begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix}$

$i \mapsto \begin{pmatrix} 1 & 1 \\ 1 & -1 \end{pmatrix}$

$j \mapsto \begin{pmatrix} -1 & 1 \\ 1 & 1 \end{pmatrix}$

$k \mapsto \begin{pmatrix} 0 & -1 \\ 1 & 0 \end{pmatrix}$

where {−1,0,1} are the three elements of F₃. Since all of the above matrices have unit determinant over F₃, this is a representation of Q in the special linear group SL(2, 3). Indeed, the group SL(2, 3) has order 24, and Q is a normal subgroup of SL(2, 3) of index 3.

Galois group

As Richard Dean showed in 1981, the quaternion group can be presented as the Galois group Gal(T/Q) where Q is the field of rational numbers and T is the splitting field, over Q, of the polynomial

$x^8 - 72 x^6 + 180 x^4 - 144 x^2 + 36$.

The development uses the fundamental theorem of Galois theory in specifying four intermediate fields between Q and T and their Galois groups, as well as two theorems on cyclic extension of degree four over a field.

Generalized quaternion group

A group is called a generalized quaternion group when its order is a power of 2 and it is dicyclic group.

$\langle x,y \mid x^{2^m} = y^4 = 1, x^{2^{m-1}} = y^2, y^{-1}xy = x^{-1}\rangle.\,\!$

It is a part of more general class of dicyclic groups.

Some authors define generalized quaternion group to be the same as dicyclic group.

$\langle x,y \mid x^{2n} = y^4 = 1, x^n = y^2, y^{-1}xy = x^{-1}\rangle.\,\!$

for some integer n ≥ 2. This group is denoted Q_4n and has order 4n. Coxeter labels these dicyclic groups <2,2,n>, being a special case of the binary polyhedral group <l,m,n> and related to the polyhedral groups (p,q,r), and dihedral group (2,2,n). The usual quaternion group corresponds to the case n = 2. The generalized quaternion group can be realized as the subgroup of GL₂(C) generated by

$\left(\begin{array}{cc} \omega_n & 0 \\ 0 & \overline{\omega}_n \end{array} \right) \mbox{ and } \left(\begin{array}{cc} 0 & -1 \\ 1 & 0 \end{array} \right)$

where ω_n = e^iπ/n. It can also be realized as the subgroup of unit quaternions generated by x = e^iπ/n and y = j.

The generalized quaternion groups have the property that every abelian subgroup is cyclic. It can be shown that a finite p-group with this property (every abelian subgroup is cyclic) is either cyclic or a generalized quaternion group as defined above. Another characterization is that a finite p-group in which there is a unique subgroup of order p is either cyclic or a 2-group isomorphic to generalized quaternion group. In particular, for a finite field F with odd characteristic, the 2-Sylow subgroup of SL₂(F) is non-abelian and has only one subgroup of order 2, so this 2-Sylow subgroup must be a generalized quaternion group, (Gorenstein 1980, p. 42). Letting p^r be the size of F, where p is prime, the size of the 2-Sylow subgroup of SL₂(F) is 2ⁿ, where n = ord₂(p² − 1) + ord₂(r).

The Brauer–Suzuki theorem shows that groups whose Sylow 2-subgroups are generalized quaternion cannot be simple.

See also

• binary tetrahedral group
• Clifford algebra
• dicyclic group
• Hurwitz integral quaternion
• List of small groups
• 16-cell

References

• Dean, Richard A. (1981) "A rational polynomial whose group is the quaternions", American Mathematical Monthly 88:42–5.
• P.R. Girard (1984) "The quaternion group and modern physics", European Journal of Physics 5:25–32.

External links

• Weisstein, Eric W., "Quaternion group", MathWorld.