Irish Quaternions

Robin Puffin The real quaternion algebra H is a non-commutative normed 4-dimensional division algebra over the real field R discovered by Hamilton in 1843. Its traditional basis is r = {1, i, j, k}, where multiplication is determined by the rules i2 = j2 = k2 = -1 and [in a cyclical arrangement] i*j = -j*i = k, j*k = -k*j = i, k*i = -i*k = j, like depicted on the stamp below. So an arbitrary element q of H can be written [in a unique way] as a real linear combination q = a*1 + b*i + c*j + d*k. This may be rearranged into q = (a+b*i)*1 + (c+d*i)*j showing that H is a 2-dimensional algebra over the field C of complex numbers with basis s = {1, j}. So next to the real representation [q]r = [a,b,c,d], with respect to r, we have the complex representstion [q]s = [a+b*i, c+d*i]. The algebra H posesses an involution, an anti-automorphism of order 2, viz. q --> q_ = a*1 - b*i - c*j - d*k which extends complex conjugation and is called likewise. In number theory q*q_ = a2 + b2 + c2 + d2 is called the Norm N(q) of q. It follows that q-1 exists ( q-1 = q_/N(q) ) for any nonzero q. The algebra H is a division algebra, indeed. In analysis, the norm |q| of q is given by the square root of N(q), that is, |q| = (a2 + b2 + c2 + d2)1/2, the euclidean norm of [q]r in four-space. One calls a*1=a the scalar part of q and q - a its vectorial part. If qn = bn*i + cn*j + dn*k for n=1,2 (no scalar parts), then q1*q2 has minus the inner product of [q1]r and [q2]r as scalar part and its vectorial part corresponds to the outer [or cross] product of [q1]r and [q2]r. A famous theorem of Frobenius from 1886 states that R and C and H are, up to isomorphism, the only [associative] real division algebras.

Just like the complex field C can be represented as the division algebra of all real matrices of the form
c-matrix,
the quaternion skew field H can be represented as the division algebra of all complex matrices of the form
h-matrix.

In fact the first representation is just the matrix-representation with respect to the basis {1, i} of the R-linear mapping of C into itself given by z --> (a + bi)*z, while the second is the matrix representation with respect to the basis (1, j} of the C-linear mapping of H into itself given by q --> ((a + bi)+(c+di)*j)*q. It is essential here to view H as a right-linear vector space over C, since otherwise the multiplication mapping above is not C-linear, by lack of commutativity. In particular, to recognize the first column, write (a + bi) + (c + di)*j as (a + bi) + j*(c - di).

illustration


Up to isomorphism there are just two non-commutative groups of order 8 [surprisingly both have the same character table], namely, the dihedral group D4 and the quaternion group {1, -1, i, -i, j, -j, k, -k}. If we add the 16 elements of the form (e1*1 + e2*i + e3*j + e4*k)/2, where ei is equal to -1 or +1, for i = 1,2,3 and 4, we obtain the group of all units in the ring of integer quaternions, after Hurwitz.

Let F be any field of characteristic not 2 and let a, b in F be nonzero. Then the general quaternion algebra (x,y | F) is defined as the F-algebra with basis {1, s, t, s*t} and multiplication rules s2 = x, t2 = y and t*s = -s*t, so that H = (-1,-1 | R).

Og an Abha Mhór opposite Cloghane (Dingle peninsula) [23-06-2001] A polynomial of degree n over a field F has at most n roots in F. For instance, X2 + 1 has no roots over R and two, the maximum, over C. The situation is dramatically different over the skew field H. If V is the real 3-d subspace of H with basis {i, j, k},that is, if V is the subspace of all quaternions without scalar part, then the set of all q in H with q2 + 1 = 0 is infinite and actually equal to the unit sphere S = {b*i + c*j + d*k | b2 + c2 + d2 = 1} in V. Moreover, the multiplicative group of H acts on S as the full rotation group. In fact, let s(q) denote the scalar part of q and fq the internal algebra-automorphism of H defined by fq(x) = q*x*q-1. Then s(fq(v)*fq(w)) = s(fq(v*w) = s(fq(s(v*w)) = s(v*w), for v,w in V. This settles the orthogonality of fq viewed as a linear transformation from V into itself. The real line through q-s(q) is its rotation axis.
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A. A. Jagers
Make Burton quilts [links to a Western Oregon University applet and program] displaying D4, quaternion and many other symmetries.
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