robphy said:
I think you mean that "rapidity" is the "inverse hyperbolic tangent of the velocity" (that is, tanh(rapidity)=velocity).
Yes, sorry for any confusion. Insert irrelevant excuses here...
These are additive since "rapidity" is the angle between worldlines (or an arc length on a unit hyperbola) in Minkowski geometry.
Of course, hyperbolic-tangents are not additive... their composition law resembles the formula for tanh(A+B).
By the way, the additivity of rapidity corresponds to the multiplicativity of exp(rapidity) ( that is, exp(A+B)=exp(A)exp(B) ).
exp(rapidity) and exp(-rapidity) are special because these are precisely the eigenvalues of a boost, with lightlike eigenvectors.
In the language of Bondi's k-calculus, k=exp(rapidity)=DopplerFactor=sqrt((1+v)/(1-v))...
and the multiplicativity of the k-factors is equivalent to the velocity-composition-formula.
It's interesting (and mentioned by the paper as an example of the main theorem) that there is a transformation that transforms the group structure of multiplication over a suitable interval into the addition of real numbers. The needed mapping is of course logarithmic, adding logarithims gives the logarithm of the product. So it's not surprising and indeed expected that the additive quantity is the log of the multiplicative quantity.
If I understood the OP correctly he wasn't so interested in k-calculus, as he didn't want to have to introduce coordinates, just consider what we could learn from the velocity composition law. My conclusion is that there are (unsurprisingly) an infinite number of velocity composition laws that obey the group axioms, only one of which is the relativistic velocity composition law.
It's not clear if the OP has more structure to add to the velocity composition laws than the group axioms, but it's unclear how one might go from saying that "there is some function of velocities that adds" to "rapidities add" without considerably more structure than the OP was proposing.
Once one introduces coordinates, and demands that there be some linear transformation between between coordinates that represent a change-in-frames, i.e. a Lorentz boost or an addition of velocity, it becomes obvious (once explained, at least) the requirement that a point on a light cone through the coordinate origin be mapped to another point on a light cone through the coordinate origin implies that the coordinates of the points on the lightcone are eigenvectors of said linear transformation.
[add]
If we let the velocity of light be c, and consider a 2-d space (t,x), then points on the light cone are all a scalar multiple of (0,c).
And the definition of an eigenvector of a linear transformation is that it maps vectors to scalar multiples of a vector. Since the points on the lightcone are all scalar multiples of the same vector, that vector, representing the velocity of light, must be an eigenvector of the linear transformation, as must any vector on the light cone.
The rest follows as you explained, the k-values are the eigenvalues corresponding to the eigenvectors.
But this requires the introduction of coordinates, something the OP was resisting (at least from what I read).