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Note. In this chapter ab denotes the quaternion product and not the segment from
a to b as it does in the other parts of the topic.
20.2.1 Proposition. Equations (20.1) in the definition of the quaternion product
on R 4 define a well-defined associative product.
Proof.
Exercise 20.2.1.
Note that the product is not commutative since, for example, ij =- ji . Also, the
identity i 2 = j 2 shows that a 2 = b 2 does not imply that a b . Condition (20.1b) could
have been replaced by the single condition
ijk =-1
and the assumption that we have an associative operation.
Definition. The vector space R 4 together with the quaternion product is called the
quaternion algebra over R and is denoted by H .
For reasons which will become clearer as we go along, it is convenient to identify
the subspace of H generated by 1 with R and the subspace of H generated by i , j , and
k with R 3 . In other words, we shall feel free to use expressions of the form
3
= (
) Œ
r
+
v
,
where r
Œ
R
and
v
v
,
v
,
v
R
,
123
to represent the quaternion
rv v v
1i
++ +
j
3 .
k
1
2
With this identification we have expressed H as a direct sum of R and R 3 . By
identifying
r
with
r 1
and
a
+
b
i
with
a
1
+
b
i
we shall consider both the reals and the complex numbers as being subsets of H , that
is, we have natural inclusions
RCH
ÃÃ.
Definition. Elements of H in the subspace generated by i , j , and k are called pure
quaternions . Let q be a quaternion and express q in the form r + v , where r ΠR and
v ΠR 3 . The number r is called the real part of q and the vector v is called the pure
part of q . To extract these parts, we define functions
re pu
,
: HH
Æ
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