The quaternions ℍ

Arun Ram
Department of Mathematics and Statistics
University of Melbourne
Parkville, VIC 3010 Australia
aram@unimelb.edu.au

Last updates: 18 May 2011

The quaternions ℍ

The quaternions is the ℝ-algebra

ℍ = ℝ-span {1,i,j,k} ={ x0+x1i + x2j+x3k | x0,x1, x2,x3 ∈ℝ }
with product determined by
i2= j2= k2= -1, ij=-ji=k, jk=-kj=i, ki=-ik=j.
The topology on ℍ is given by
ℍ≃ℝ4, and ℂ = { x0+x1i | x0,x1 ∈ℝ }
is an ℝ-subalgebra of ℍ. Since ij≠ji, ℍ is not a ℂ-algebra.

Writing ℍ as space-time,

ℍ =ℝ×ℝ3 = {t+v | t∈ℝ, v∈ℝ3 },
the product in ℍ is given by
(t1+v1) (t2+v2) = t1 t2 - v1 ⋅ v2 + ( t1 v2 + t2 v1 + v1 × v2 ).

The norm N:ℍ →ℝ≥0 is given by

N( x0+x1i + x2j+x3k ) = x02 + x12 + x22 + x32 = ‖x‖2 ,
where ‖x‖ :ℝ4→ ℝ≥0 is the usual Euclidean norm on ℝ4. Then
N(xy) = N(x) N(y).
The conjugate P‾ :ℍ→ℍ is given by
x0+x1i +x2j+x3k ‾ = x0-x1i -x2j-x3k and xy‾ = y‾ x‾
so that P‾ :ℍ→ℍ is an antiautomorphism. Then
GL1(ℍ) =ℍ× ={x∈ℍ | x≠0} ∪| U1(ℍ) ={x∈ℍ | xx‾t=1 } = { x0+x1i + x2j+x3k | x02 + x12 + x22 + x32 =1 }
and
ℍ× ⟶∼ (ℝ×) ∘ × U1(ℍ) x ⟼ ‖x‖ ⋅ x‖x‖
Here (ℝ×) ∘ =ℝ>0 is the connected component of the identity in the Lie group GL1(ℝ) =ℝ×. This polar decomposition is an example of the Cartan decomposition G=K⋅(exp𝔭) (see Segal Theorem 4.1 and/or Knapp Prop. 1.2), where K is a maximal compact subgroup of G, and 𝔤=𝔨⊕𝔭 with 𝔤=Lie(G) and 𝔭 orthogonal to 𝔨 =Lie(K) with respect to the Killing form.

Notes and References

The reference [Ch. VIII § 1.4, BouTop] provides a brief, but thorough, introduction to the quaternions.

References

[BouTop] N. Bourbaki, General Topology, Chapter VI, Springer-Verlag, Berlin 1989. MR?????

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