I'm not sure exactly how to categorize Robb's treatment of the spacetime interval. But it seems like a gem of simplicity and insight.
The following illustrations are based on MTW Box 1.3. As drawn, we can think of two unaccelerated observers crossing paths at event $\mathcal{A}.$ One moves along the world line to event $\mathcal{B}$ at which a light pulse originating at $\mathcal{P}$ is reflected back to the worldline $\mathcal{AZ}$ at event $\mathcal{Q}$. With $\mathrm{c}=1$ it is easily seen that the distance $x$ is equal to the proper time from $\mathcal{P}$ to the event labeled $t$ which is equal to the proper time from $t$ to $\mathcal{Q}$. From that we easily find the surprising and simple equation:
$$s_{\mathcal{A}\mathcal{B}}^2=-\tau _{\mathcal{A}\mathcal{B}}^2= -\tau _{\mathcal{A}\mathcal{Q}}\tau _{\mathcal{A}\mathcal{P}}$$
Notice that if we drop my requirement that $\mathcal{A}\mathcal{B}$ be time-like, Robb's equation will still work.
The reason this example is so compelling to me is that I found it illuminating when analyzing Einstein's thunderbolt thought experiment. The first of the following graphics show how events are labeled. The left Minkowski diagram shows the worldline of railbed system vertical. The right diagram shows the onboard origin's worldline vertical. The distance $x$ in the above discussion appears as the magenta line segment originating at event $\mathcal{E}_b.$ It is also the proper time separation between the events terminating the tops of the dashed magenta lines, as well as other significant separations in the diagrams.
See Bergmann's Introduction to the Theory of Relativity, Chapter IV for a discussion of this well-known thought experiment.
Is there any standard terminology established for Robb's treatment of the spacetime interval?