Angular momentum of a single particle I have to answer the following question:

Consider the decay $\rho^0\to\pi^+\pi^-$. The rho meson has angular momentum 1, what must the orbital angular momenta of the pions be, given that they are both spin-zero?

I know this question has been asked before, but I am only marginally interested in the numerical result itself (which I believe to be 1).
I believe angular momentum must be defined with respect to something -- e.g. a reference point, another particle, and so on. Therefore, 1) in "the rho meson has angular momentum 1", am I correct in assuming that it's entirely spin angular momentum? My reasoning is that it would not make sense to talk about the angular momentum of a single particle without a reference point, so I assume it's all spin. Following-up: every time I hear "particle X has angular momentum y", 2) can I assume it is the spin that is being mentioned?
3) is "the orbital angular momenta of the pions" the orbital angular momentum shared by the pions? In this case, with two particles, I believe it makes sense to talk about orbital angular momentum, if we implicitly refer to the angular momentum between them.
UPDATE Actually, in a later question I just read "Both the ground state $D^0$ meson and the excited state $D^{0*}$ have zero orbital angular momentum". I interpret this as saying that the orbital angular momentum is a well-defined quantity -- in this case it is zero, but it needn't be. How can you talk about the orbital angular momentum of a single particle? Without mentioning a reference point? For example, when in atomic physics I used to read about the orbital angular momentum of the electron, I always assumed that implicitly they meant the orbital angular momentum with respect to the nucleus.
 A: What is spin? Spin is the amount of angular momentum necessary so that in the particle interactions we have studied, angular momentum would be conserved, so that angular momentum conservation would still be a strong law. It works, because there has been no falsification of this hypothesis in the study of particle interactions at present. That is how the spin of the particles and resonances has been assigned.
For particles and their  composites, when one is talking of angular momentum, one means angular momentum about the center of mass ( where the nucleus sits is in your example). In the center of mass of the $\rho^0\to\pi^+\pi^-$  system , the two pions have to go in equal and opposite directions,because of momentum conservation. Their spin is zero and  if they are not imagined in an "orbit", they  cannot build up the spin 1 of the rho. The decay would be forbidden by angular momentum conservation. Giving an angular momentum of 1 in the center of mass system, restores conservation of angular momentum and allows the decay.
A: Single composite particles can have orbital angular momentum $L$ as well as spin $S$. In a simplified & intuitive picture, you can think of $L$ as resulting from the motion of the constituent particles and $S$ as resulting from their alignment (e.g. aligned quarks in a meson make $S=1$, anti-aligned make $S=0$).
You may be familiar with this from electrons in an atom or nucleons in a nucleus... it's the same principle for quarks in a hadron.
