So I thought a little about those question and here are the partial answerThe only part I have been abledon't know how to find,answer is the non-emptyness of the spectrum... I'm still thinking about it so, and it might be related to those possible additional condition I'm mentioning just above. I will edit if I found more answerfind something.
LetSo, let $A$ be a quaternionic $C^*$-algebra, and $a \in A$ I guess you want to define the spectrum as $\{ h \in \mathbb{H} | a - h \}$ is non-invertible.
As I said, 'non-empty' is trickier because the spectrum in a real $C^*$-algebra don't have to be inhabited and we don't have holomorphic calculus at disposition for complexquaternionic $C^*$-algebra (althoug it might be an idea to develop it a little, the resolvant is still locally a formal series so maybe one can use a kind of quaternionic Liouville's theorem).
But it seems difficult to produce a counter example: For example, as soon as you have an element which commute to some purely imagnary unit $u$, then $x,x^*,u$ generates a complexe $C^*$-algebra (with $u$ as $i$) hence $x$ has a non-empty spectrum inside of it (and we can hope that, and it implies that $x$ has a non-empty sepctrum (as in real $C^*$-algebra it also true that $x$ is invertible is a subalgebra if and only if it is invertible in the initiallarger algebra, although this: it is not obvious eitherproved by taking the complex form of the algebras).
OneBut one can do bettergive a more explicit condition: A quaternionic $C^*$-algebra is of the form $H(X)$ if and only if "selfits self adjoint element (x^*=x) are central"central.