A pure quaternion in a BB over a field FF of characteristic different from two is an element with zero. Their space is

B0=ker⁡(trd⁡:B→F)={x∈B:xˉ=−x}.B_0=\ker(\operatorname{trd}:B\to F) =\{x\in B:\bar x=-x\}.

It has dimension three. In B=(a,b)FB=(a,b)_F, it is Fi⊕Fj⊕FijFi\oplus Fj\oplus Fij, and B=F1⊕B0B=F1\oplus B_0.

Squares and the norm

For x∈B0x\in B_0, the reduced characteristic identity gives x2=−nrd⁡(x)x^2=-\operatorname{nrd}(x). In the ,

(bi+cj+dk)2=−(b2+c2+d2).(bi+cj+dk)^2=-(b^2+c^2+d^2).

This is why quadratic-field embeddings there connect to sums of three squares.

Linear space and Lie algebra

Pure quaternions are not generally closed under multiplication: i2=ai^2=a is scalar. They are closed under the commutator [x,y]=xy−yx[x,y]=xy-yx, because reduced trace is cyclic. The multiplication and the commutator are different algebraic structures.

References
  1. John Voight, Quaternion Algebras, author's text, §§2.4 and 5.1, the trace-zero subspace.
  2. The coordinate formulas and reduced characteristic identity directly verify the displayed properties.