Quaternion group

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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
Cayley graph Q8.svg
Q8
The red arrows represent multiplication on the right by i, and the green arrows represent multiplication on the right by j.
Dih 4 Cayley Graph; generators a, b; prefix.svg
Dih4
Dihedral group
GroupDiagramMiniQ8.svg
Q8
Dih4 cycle graph.svg
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:[1]

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.[2] Every Hamiltonian group contains a copy of Q.[3]

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[4] 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).[5]

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.[6]

Generalized quaternion group

A group is called a generalized quaternion group[7] 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 [4] 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 Q4n and has order 4n.[8] 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 ωn = eiπ/n.[4] It can also be realized as the subgroup of unit quaternions generated by[9] x = eiπ/n and y = j.

The generalized quaternion groups have the property that every abelian subgroup is cyclic.[10] 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.[11] 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.[12] 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 pr 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

Notes

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References

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