Structure
Quaternion algebra here means something more general than the algebra of Hamilton quaternions. When the coefficient field F does not have characteristic 2, every quaternion algebra over F can be described as a 4-dimensional F-vector space with basis, with the following multiplication rules:
- i2 = a
- j2 = b
- ij = k
- ji = −k
where a and b are any given nonzero elements of F. A short calculation shows k2 = −ab. (The Hamilton quaternions are the case where and a = b = −1.) The algebra defined in this way is denoted (a,b)F or simply (a,b). When F has characteristic 2, a different explicit description in terms of a basis of 4 elements is also possible, but in any event the definition of a quaternion algebra over F as a 4-dimensional central simple algebra over F applies uniformly in all characteristics.
A quaternion algebra (a,b)F is either a division algebra or isomorphic to the matrix algebra of 2×2 matrices over F: the latter case is termed split. The norm form
defines a structure of division algebra if and only if the norm is an anisotropic quadratic form, that is, zero only on the zero element. The conic C(a,b) defined by
has a point (x,y,z) with coordinates in F in the split case.
Read more about this topic: Quaternion Algebra
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