Does the Cayley-Dickson construction preserve isomorphism of quaternion algebras? I posted this on math.stackexchange to no avail, so I hope it's appropriate to post here despite that it might not be research-level. I expect the answer to this is well-known to people studying non-associative algebras, but I cannot find it in my references and the more thorough literature on the topic is expensive! On a similar note, I would appreciate a recommendation for a reference covering octonion algebras over number fields and the Cayley-Dickson construction, in more generality. I don't mind expensive if it gives a good thorough treatment.
Let $K$
be a number field and let $\mathcal{B}=\Big(\frac{a,b}{K}\Big)$
be a quaternion $K$-algebra.
Then its norm is the Pfister form $\langle\langle a,b\rangle\rangle$
over $K$.
Apply the Cayley Dickson construction to $\mathcal{B}$,
yielding an octonion $K$-algebra $\mathcal{C}$.
What is the Pfister form of the norm of $\mathcal{C}$?
Is it $\langle\langle a,b,ab\rangle\rangle$?
Does the isomorphism class of $\mathcal{B}$
(i.e. different choices for $a,b$ preserving the ramification set of $\mathcal{B}$)
determine the isomorphism class of $\mathcal{C}$?
Equivalently, does the isometry class of the quadratic form $\langle\langle a,b\rangle\rangle$
determine the isometry class of the Pfister form of $\mathcal{C}$ as a quadratic form?
If it does, it makes me wonder about the octonion $K$-algebras with norm the Pfister form of $\langle\langle a,b,c\rangle\rangle$, non-isomorphic to $\mathcal{C}$. It would seem that these also contain $\mathcal{B}$ as a quaternion subalgebra,
and that some variations of the Cayley-Dickson construction would take you from $\mathcal{B}$ to these. How does this work?
 A: Suppose $K$ is a field, and $B$ your quaternion algebra $K$.  The octonion algebra $C$ made from $B$ using the Cayley-Dickson construction depends on an auxiliary choice of an element $c \in K^{\times}$.  Namely, $C$ is the set of pairs $(u,v)$ with $u,v \in B$ with addition 
$(u_1,v_1) + (u_2, v_2) = (u_1 + u_2, v_1 + v_2)$
and multiplication 
$(u_1,v_1)(u_2,v_2) = (u_1u_2 + c\overline{v_2}v_1, v_2u_1 +v_1\overline{u_2}).$
Here $x \mapsto \overline{x}$ is the involution on the quaternion aglebra $B$.  The involution on $C$ is then $(u,v) \mapsto (\overline{u},-v)$.  With this multiplication and involution, one computes that the norm on $C$ is
$(u,v)(\overline{u},-v) = u\overline{u} - cv \overline{v}$.
It follows that if the norm form on $B$ is the Pfister form $<<a,b>>$,  then the norm form on $C$ is the Pfister form $<<a,b,c>>$.
The resulting octonion aglebra $C$ depends not just $B$ but also on $c$.  For example, suppose $B$ is the quaternion division algebra over $\mathbf{R}$ (i.e., Hamilton's quaternions).  If one chooses $c=1$, then the resulting octonion algebra $C$ contains nonzero elements with norm $0$, while if one chooses $c = -1$ then the norm form on $C$ is anisotropic.
